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Download "ОПТИКА, КВАНТОВАЯ И ЯДЕРНАЯ ФИЗИКА ЗА 6 ЧАСОВ! | ЕГЭ по Физике | Саня Эбонит"

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Физика
ЕГЭ
Эбонит
Александр Касио
Саня Эбонит
На марс
Демидова
Золотухин
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00:00:11
Hello my dears, hello my dears
00:00:14
cool viewers so now a little sound
00:00:17
I'll chop it off
00:00:18
So
00:00:21
bee bee bee bee bee bee bee bee
00:00:25
so it’s me and what’s not, I opened it like this
00:00:30
hello friends, we're here today
00:00:32
this is a very important day with you this long ago
00:00:35
waited, many of you didn’t pass at all
00:00:38
quantum physics or optics or I dirk
00:00:40
or all of this combined
00:00:42
many of you left for later and such
00:00:45
[ __ ] it maybe someday
00:00:47
I’ll learn and now there’s almost no time
00:00:49
the last thing left is hours
00:00:53
last moment when you can
00:00:56
go through this topic
00:00:57
yes, that is, those who did not study at
00:01:01
in my courses this is the only chance
00:01:04
obtain adequate information on optics
00:01:07
in a quantum duel for free and finish off
00:01:10
everything you need to know
00:01:13
So today we will go through optics
00:01:19
geometric and wave
00:01:22
today we will go through quantum
00:01:24
physics and nuclear physics
00:01:27
means quantum nuclear my bend
00:01:30
my forecast my forecast
00:01:33
a good one will be on number twenty-six
00:01:35
more likely
00:01:36
geometric wave optics rather
00:01:39
everything will be in the twenty-ninth, but somehow
00:01:40
no one says they can't exist
00:01:42
there let's say twenty-fourth and there
00:01:46
maybe at 29 there will be magnetism in general
00:01:48
something else but most likely still
00:01:51
it will be the same as on early cooking
00:01:54
need this option therefore this option
00:01:56
Today's analysis is very important, it will give
00:01:59
you have a lot of secondary points, that is, there are 5 here
00:02:02
points for five points we are at least with
00:02:03
you bonuses so
00:02:06
yes such things
00:02:09
means guys pdf here they ask pdf tele
00:02:13
pdf where to get pdf oh let me be creative
00:02:18
I'll draw f
00:02:22
pdf can be taken from
00:02:27
my cart means now I'll give it to you
00:02:31
link
00:02:33
it means here in my cart you see
00:02:37
let me bring it closer
00:02:39
you saw better
00:02:43
in general, in my cart and go to qr
00:02:46
code you can download the gravy
00:02:49
today's lesson
00:02:50
tasks that will be done today
00:02:52
lesson this webinar
00:02:56
compiled according to a similar task
00:02:59
which I had in
00:03:02
Last year
00:03:03
but with the only exception that here
00:03:07
other numbers other numbers so you
00:03:11
you can watch today's webinar and
00:03:14
work through the tasks from last year’s webinar
00:03:18
in optics there are also 55 tasks like
00:03:22
today we will sort it out so
00:03:25
everything will be cool
00:03:33
I'm becoming so predictable
00:03:36
lately so guys a few words who
00:03:39
who doesn't know me damn it's a little awkward
00:03:43
that the person we are changing doesn’t know to think
00:03:47
that I'm so vulgar and
00:03:50
[music]
00:03:52
all the time in the forest list I will put
00:03:56
I put censorship so that they don’t think
00:03:59
bad
00:04:01
All
00:04:03
Now
00:04:05
censorship more acceptable
00:04:09
So my name is Sanya Zolotukhin I passed
00:04:12
my maximum exam score in mathematics
00:04:15
and physics 100 points twenty-first year
00:04:17
I dragged it onto a hundred and released it into
00:04:20
17 swimsuits for the twenty-first year
00:04:22
graduated from the Faculty of Mechanics and Mathematics at Moscow State University
00:04:24
2009 that is, I am not my angel
00:04:28
competitors, one might say, taught them physics
00:04:31
and mathematicians in due time since 2006
00:04:34
I work as a teacher
00:04:37
I also have all sorts of my creative
00:04:40
activity
00:04:42
I wrote it down with your fit technique here
00:04:46
the track is regional but of course this is a hint
00:04:48
for the 30th task of the north community this is
00:04:51
I didn’t buy it at all
00:04:54
teeth transposh etrex for
00:04:59
glasses wholesale drugs why not
00:05:03
why clan themes are classic theme in
00:05:06
rap of the undisclosed song here you can
00:05:08
check out listen also means
00:05:11
I got a 50k track released the other day
00:05:13
which I
00:05:15
I tell you what a difficult path it was for me
00:05:18
in order to reach the top in
00:05:21
teaching physics well become popular
00:05:24
teacher here
00:05:26
in which I wish good luck to all my
00:05:29
colleagues who also work on this
00:05:32
field I also have my serious
00:05:35
group 500 tickets which I am not
00:05:38
there's a park that doesn't hurt everyone
00:05:40
[ __ ] up and all that, but really the songs
00:05:43
which is like the soul of the whole heart
00:05:45
you can listen to the non-profit project
00:05:47
on itunes here it’s everywhere in general
00:05:51
I express myself
00:05:54
metal band to laugh
00:05:56
we have several constant bars there
00:05:58
songs there are three songs you do
00:06:01
ok it's all clear night let me
00:06:04
I'll show you today's lesson plan
00:06:07
Sanya who said this to all the fish
00:06:10
community when this track got hyped
00:06:12
here on rap.ru it’s scattered everywhere and
00:06:16
anyway, what is this, what is this [ __ ]
00:06:19
not like the old container is yours
00:06:22
the technique was previously a group full
00:06:24
container
00:06:26
all these extra drug addict threads, what's where
00:06:30
where is your favorite text about drugs?
00:06:35
in general look look at this plan
00:06:38
it's approximate it's based on last year's
00:06:41
six-hour webinar, well, as you can see
00:06:44
he wasn't 6 o'clock
00:06:47
630 hour so look what
00:06:51
the topic is relevant to you although in reality
00:06:53
guys even if you think that I am god
00:06:56
optics I am the master of these topics then
00:07:00
look anyway, even here is the theory I
00:07:02
I’ll explain it to you now at the very beginning or
00:07:05
there will probably be some for lenses
00:07:07
something you didn't know, let's say
00:07:09
tricky question, you know how
00:07:14
the beam will behave
00:07:17
if it's in the focal plane
00:07:19
there is a passage and here is the exact source
00:07:24
is how he will behave
00:07:26
after passing the lens if you don’t know
00:07:30
then I watched to the end as they say and
00:07:33
completely rain in any topic I will find you
00:07:36
problem areas
00:07:38
So here's geometric optics first
00:07:42
refraction of light then all sorts of lenses
00:07:45
optical instruments at 14:40 with us
00:07:49
wave optics will begin
00:07:51
Then
00:07:54
quantum physics in 1545 then we will discuss
00:07:58
light pressure is a topic that
00:08:01
for some reason they are missing out, they haven’t forgotten about the light and
00:08:05
about and and pressure
00:08:07
therefore, we will continue to discuss nuclear
00:08:10
physics in general throughout the body topic
00:08:13
we'll go over everything you need to know and discuss it
00:08:16
So
00:08:18
that means today's stream too
00:08:21
naturally we have it for a reason
00:08:23
sponsor sponsor these are my courses that I
00:08:26
unfortunately I have other sponsors
00:08:29
no, despite the fact that I advertise
00:08:32
constantly at the cash register and all sorts of crap, that's me
00:08:34
I read my humble destiny
00:08:37
our intensive starts on May 25th at which
00:08:42
we will go through this for eight days
00:08:45
the first day is dedicated to each section
00:08:48
mechanics the second day also mechanics
00:08:50
third day im k-t 4 electric 5
00:08:54
magnetism very all all all
00:08:56
Let's go through all the sections in detail if
00:08:58
want to show yourself as the best crucian
00:09:00
be sure to sign up for the exam
00:09:03
for intensive and if you
00:09:07
tenth grader if you are in 10th grade then
00:09:11
you have a unique opportunity to groove and
00:09:13
again at the link in the description
00:09:15
sign up for the next list bonita 2023 for
00:09:19
no this is my main annual course which
00:09:22
shows the highest results on
00:09:24
in which students simply know everything
00:09:27
It’s only possible to know at the end of the year
00:09:30
Most physicists are starting to fumble
00:09:33
cases cooler than their teachers
00:09:35
school teacher limited
00:09:38
time limited by topics limited
00:09:40
stupidity
00:09:42
and general ignorance of what surrounds him
00:09:45
but the students who come to him are not there
00:09:48
they are not limited by anything they get
00:09:49
sea ​​of ​​information and
00:09:52
at the end of the year the Sharif is really cooler than the school ones
00:09:54
teachers because of which they are brought to tears
00:09:57
but what can you do what can you do if you
00:10:00
handsome you know better than anyone
00:10:03
you will also get into intensive summer training in
00:10:07
summer school
00:10:09
you will receive records of the annual course and a bath
00:10:11
2022 summer free in general
00:10:14
take care of your preparation now
00:10:16
so that you can enjoy what you are doing later
00:10:19
lowest price
00:10:21
that means the price is now about intensive
00:10:24
if you return the cost of the intensive course here
00:10:26
such 1190 test 1990 complex and that's it
00:10:31
It's better to take everything together because
00:10:33
even if you really think you're handsome
00:10:36
test part you'll be wrong there
00:10:39
three mistakes in the dough you are reading this one
00:10:42
didn't make it complicated, [ __ ] it, it's better to live
00:10:44
work through the test properly and
00:10:46
complex also underwater
00:10:50
follow the first link in the description
00:10:51
write metal words
00:10:54
so and also with my partners, here with Eric
00:10:59
already why are you calling me Yarik already
00:11:01
went down intensive
00:11:04
already all these first day to 1 day
00:11:07
intense already the most powerful intense filled
00:11:10
for now I missed it a little later
00:11:13
Artyoma computer science will be shorter for everyone
00:11:15
Oksana will speak extremely Russian
00:11:17
I recommend it’s going well with us in general
00:11:20
which subject you take and go
00:11:24
my dear and so
00:11:27
as usual
00:11:29
as usual
00:11:32
that means we need
00:11:36
the sky is in the cart
00:11:41
sky no
00:11:43
cart
00:11:44
pdf can be found on yabla no but
00:11:50
It's already Yarik's second day, excuse me for something
00:11:53
mixed up
00:11:56
[music]
00:12:00
to yabla no
00:12:07
What end is sticking out to you?
00:12:11
I don't understand it, it's gone, you say
00:12:14
so guys we need to come up with something
00:12:17
will come up with something
00:12:19
what to do
00:12:22
what to do if we dial some
00:12:25
number of likes
00:12:27
So
00:12:30
to do
00:12:32
let's think
00:12:37
I don't really want to
00:12:41
it turned into some kind of trash
00:12:44
stream
00:12:47
but I have an electric machine
00:12:57
which accumulates a static charge
00:12:59
[music]
00:13:11
what kind of lightning I'm starting to pass through
00:13:21
it's a pity Oleg is not here now
00:13:29
okay let's really
00:13:34
if this stream
00:13:39
if this stream gets enough
00:13:43
give me a thousand likes I don't even though I really
00:13:45
I want to beat myself
00:13:47
but 1000 likes me
00:13:52
I'll charge myself with vigor
00:14:00
I charge myself and how it feels like Duracell
00:14:04
like the hare from the duracell commercial so everything
00:14:09
remembered and
00:14:11
Then
00:14:13
begin
00:14:19
hit
00:14:27
after 1000 every three likes recharge
00:14:35
when the price for the annual price rate is known
00:14:38
for the annual course we announce at the beginning
00:14:40
July
00:14:42
yes guys so if you are not a sadist then don’t
00:14:46
please like if you are kind
00:14:49
Human
00:14:50
Yes, I'm kidding, give it to me for fun
00:14:54
I've already unclenched me once
00:14:58
live
00:15:02
That's when I was shaken quite a bit
00:15:05
sword this time I'll feel sorry for myself
00:15:07
I'm sorry
00:15:21
the coil will date like or the capacitor
00:15:25
ok guys let's get started
00:15:28
It's been a bit too long already
00:15:30
I'm behind schedule
00:15:31
Let's
00:15:33
let's discuss the very basics in general there is there
00:15:37
point light source what happens in
00:15:40
geometric optics geometric
00:15:43
optics, rays propagate in a straight line and
00:15:46
where the rays hit we have light
00:15:50
there's a better place than this
00:15:54
here are the illuminated places
00:15:56
there's a better place where we don't get shadows
00:16:00
with this I think you all know with this you
00:16:03
everyone is familiar but if we have a big one
00:16:06
the source here it shines in all directions and
00:16:10
this is some kind of obstacle we have with you at night
00:16:14
so let's make it smaller, that is, there is space in
00:16:17
of which not a single piece falls
00:16:19
there are places where not all rays
00:16:21
they end up here, that is, these ones
00:16:23
get hit get hit get hit
00:16:28
this is where everyone ends up and this is where
00:16:31
not everyone ends up here and these are the ones here
00:16:34
places it will be partial shade, that is, right here
00:16:37
penumbra and
00:16:39
here receiving and here at this point at this
00:16:43
all the splinters are already starting to hit the point and
00:16:46
it's just a bright, illuminated place
00:16:50
and this is the shadow when you have extended
00:16:53
sources this happens too
00:16:57
So
00:17:01
further
00:17:03
then guys, let's get on with it
00:17:05
solve and also
00:17:07
straight mirror mirror image
00:17:10
is at the same distance
00:17:13
from which an object is removed from it
00:17:15
mirrors okay now we'll discuss
00:17:17
oh almost
00:17:21
erased the pier
00:17:24
So
00:17:26
what else does that mean
00:17:28
that the angle of incidence is also equal to the angle
00:17:32
reflections here the beam falls
00:17:35
the angle of incidence is measured with the normal to
00:17:37
surface, here the beam is reflected along the same
00:17:40
the very corner is the law of reflection
00:17:45
so where in and d is the angle between the incidence and
00:17:50
The angle of reflection is not called
00:17:53
the angle between the vectors and the angle between
00:17:56
with these rays
00:17:59
which contradicts mathematics a little but
00:18:03
what can you do if it's like this
00:18:05
formulation by ours and
00:18:08
ok let's solve the problem in general
00:18:11
little by little
00:18:15
opaque circle illuminated by a dot
00:18:17
light source and casts a round
00:18:19
shadow on the screen determine the diameter of the circle
00:18:22
if the diameter of the shadow is 0 3 meters here we have
00:18:26
let's have a flat drawing, here's the shadow we have 0
00:18:31
3 meters
00:18:33
distance from the light source to the circle in
00:18:38
three times less than the distance from
00:18:40
source to the screen that is
00:18:44
this is this this is this distance b
00:18:49
from now
00:18:52
distance from light source to circle
00:18:56
h&b and distance from source to screen
00:19:02
3b night it turns out that these are 2
00:19:06
triangles, let me show you like this
00:19:08
this triangle and this one
00:19:10
triangle they are similar and
00:19:13
their base x applies to 033 the same way
00:19:17
how are their heights also like trip sorry b
00:19:21
refers to 3b in similar triangles
00:19:24
this is how it turns out x is equal to 0 3 divided by
00:19:29
3 that is 0 1 meter
00:19:32
answer give meters in general
00:19:36
circle diameter
00:19:38
we will find with you
00:19:48
go ahead
00:19:53
focus on the board before
00:19:59
right now
00:20:04
ok now I want to be seen
00:20:07
And
00:20:13
when this approximation appears yes
00:20:20
All
00:20:22
now the norm
00:20:33
my friend paint
00:20:37
caught my eye
00:20:46
some water
00:21:05
damn you could see every pimple on it
00:21:08
The figure on the left shows two flat
00:21:10
mirrors z1 g2 and beam horizontally
00:21:13
falling on the mirror mirror 2
00:21:15
rotated relative to horizontal
00:21:17
axis passing through point o at an angle of 15
00:21:20
degrees what is the angle between the rays?
00:21:22
reflected from mirror 1 and from mirror 2
00:21:32
let's think about what the angle is
00:21:41
reflect here the beam falls
00:21:44
here we have
00:21:48
in general it just falls further here
00:21:52
And
00:21:54
we have
00:21:59
we turn it 15 degrees
00:22:06
15 degrees means
00:22:10
the normal also turned 15 degrees, wait
00:22:13
here too it turns out to be 15
00:22:18
[music]
00:22:20
Well, it's easy to prove because
00:22:23
this 90 this then 75 and then I have to
00:22:27
be 15 so that there is a straight angle and
00:22:31
here at an angle the law is also 15 degrees
00:22:35
reflections it is then reflected, that is
00:22:37
our beam goes like this now that we
00:22:40
turned with you and we are asked to find
00:22:44
angle between
00:22:48
rays reflected from mirror 1 that is
00:22:52
with this ray and
00:22:56
from mirror 2
00:23:01
mirror 2 reflected well that's it
00:23:04
yes it turns out in response we write with you
00:23:06
this angle is 30 degrees
00:23:08
I hope everyone got it
00:23:12
Sanya how often for a task from afar
00:23:15
East coincides with Moscow 0 times
00:23:18
this has never happened and will never happen in this
00:23:21
year so don’t look at the Far East
00:23:24
in physics 0 1 from there how many exams I have
00:23:31
no matter how much I prepare the book 2009
00:23:34
not a single task matched once
00:23:43
to the center of the top edge of the transparent cube
00:23:47
A ray of light falls at an angle of 60 degrees
00:23:52
the refracted ray hits the top of the cube
00:23:55
and define show refraction
00:23:57
the material from which I prepare the cube means
00:24:00
look here
00:24:02
let me make a 3D drawing here
00:24:05
us cube and
00:24:12
it means a beam is falling, let's have a beam
00:24:16
draw blue like mine here
00:24:19
it falls at some angle alpha and
00:24:22
then it hits and is already refracted under
00:24:26
at some angle beta and
00:24:29
gets to this vertex and
00:24:33
then we know that alpha is 60
00:24:36
degrees a
00:24:38
what can we tell you about beta?
00:24:41
strictly speaking, but look, it means
00:24:44
it turns out that here
00:24:47
this is this this is this side this is a
00:24:52
this is the side, well, that is, if I
00:24:56
found the diagonal of the cube then it would
00:24:59
was equal to a root of 2 to but it turns out
00:25:02
then this is what the roots of 2 are in half then
00:25:06
there are two times less and it turns out that
00:25:08
this is the hypotenuse
00:25:11
y is the root of a square plus a roots
00:25:16
of two halves squared the root and
00:25:20
square plus a
00:25:23
divide and divide the square by 2, well here if
00:25:27
simplify and it turns out that is
00:25:31
there you need to multiply 3-star by 2
00:25:35
root of 3 second a
00:25:37
this is what our hypotenuse will be
00:25:41
son of the desert great Robert to each other
00:25:44
so that means sine beta then and
00:25:47
This
00:25:49
means a
00:25:51
roots of 2 by 2 and all this but
00:25:55
the opposite leg somewhere roots from
00:25:58
two by two also divided by the hypotenuse y
00:26:02
to the root of 3 by 2 a
00:26:06
that is, it turns out to be the root of two
00:26:09
thirdly, if you cut down all the unnecessary things, well
00:26:13
now to find the indicator
00:26:15
refraction
00:26:16
calculate sine alpha divided by sine
00:26:19
tetta
00:26:22
It turns out the sine of 60 degrees divided by
00:26:26
root of two thirds let's calculate
00:26:31
how much can we get
00:26:37
sine 60
00:26:42
root
00:26:44
Thirdly
00:26:48
this is not yet -
00:26:51
106 refractive index
00:26:54
[music]
00:26:56
so here, unfortunately, it doesn’t say why
00:26:59
need to
00:27:00
two under the root 2 under the root and wait
00:27:05
up pretty thank you it's good that you tell me
00:27:09
they said I almost counted it
00:27:11
wrong so 2 under the root and
00:27:15
really then
00:27:18
when than then it will be different
00:27:22
root
00:27:26
out of 2
00:27:28
to the root of 4
00:27:31
but root of 3 is root of 2
00:27:35
that is, it is 1 to the root of 3 to
00:27:41
22
00:27:44
to that is, one to the root of 3 here y
00:27:48
there is only one of us
00:27:51
yeah guys I have no answers to
00:27:54
today's task because they
00:27:56
are unique and we haven’t solved them yet, that’s why
00:27:59
thank you very much for checking me on
00:28:02
errors
00:28:05
very grateful to you
00:28:16
in mathematics they are just lazy people
00:28:21
everything about the table it’s normal for me to worry
00:28:24
without knowing, of course, I fired everyone a long time ago
00:28:27
those who give the Far East similar
00:28:30
tasks for central Russia because
00:28:33
it's not fair, just what the [ __ ]
00:28:36
if you live in the Far East then
00:28:38
you have no game information if you
00:28:41
if you live in the central part then you have it
00:28:44
it's unfair I think
00:28:50
So
00:28:53
great great 7
00:28:57
before theory will be on the course theory too
00:29:00
there will be a nose for us, of course, practice theory
00:29:02
so just refresh your memory so y
00:29:05
like us there and for now I'm in
00:29:08
safe zone
00:29:10
not many likes
00:29:13
perhaps even
00:29:16
electric shock but there are no tracks for me, in short, it’s not so
00:29:21
a lot in general I'm safe thank you
00:29:24
thank you for your concern, let's move on
00:29:29
the exact light source is in
00:29:32
containers with liquid and lowered
00:29:34
vertically down from the surface and so
00:29:36
here I need to talk a little about refraction
00:29:38
speak
00:29:40
next next topic
00:29:42
then look, if you have two
00:29:47
environment
00:29:48
here is one medium with refractive index
00:29:52
n 1 and 2 medium with refractive index
00:29:56
with absolute refractive index n 2
00:30:01
What is an absolute indicator anyway?
00:30:04
refraction is the speed of light in a vacuum
00:30:07
at the speed of light in a medium that's what it is
00:30:11
such and
00:30:13
it turns out that there is such a law
00:30:16
called Snell's law
00:30:22
which shows how the indicator is related
00:30:25
refraction and angle of incidence and angle
00:30:29
refraction in general, it is most convenient to write it in
00:30:33
this type of refractive index
00:30:35
environment by the sine of the angle in the environment is equal to
00:30:38
half the other environment
00:30:40
sine of an angle in the environment, well, it’s even easier
00:30:45
formulation when the sine of alpha is sine
00:30:47
theta equals there
00:30:50
n2 to n1 but then back
00:30:54
proportional dependence is more complex and
00:30:56
if you have
00:30:58
a large number of these records are in
00:31:02
this form is much simpler by this law
00:31:04
In general I recommend using it like this
00:31:06
remember
00:31:09
so what else did I want to say
00:31:12
it turns out if we are n there I don’t know n2
00:31:17
divide by n1 then it will divide everything by
00:31:20
in 2 divided by price 1, that is, it is in 1
00:31:25
divide by v2 and
00:31:27
it turns out if we express everything from here
00:31:30
this will be equal to the ratio of sine alpha to
00:31:33
sine theta
00:31:34
Well, you see that is
00:31:37
sine of angle
00:31:39
proportional to speed
00:31:41
it turns out but back to tonal
00:31:43
refractive index here's another one
00:31:45
the form in which with which you
00:31:47
you can write Snell's law in this case
00:31:50
if you have a body from a denser environment
00:31:54
it comes out less densely, let's say the water is here
00:31:58
air
00:31:59
then your beam
00:32:03
refractions can reach 90 degrees and
00:32:06
in fact, in this case the entire beam will be
00:32:09
let's reflect into the angle of incidence alpha
00:32:14
here beta 0 let's call the exit angle 90 well there
00:32:19
if we take n of air approximately equal
00:32:21
unit and by the water I don’t know there 133 then we
00:32:26
we can calculate the angle of total internal
00:32:27
remember the reflection is called an angle
00:32:30
total internal reflection, that is, it
00:32:32
it turns out sine theta zero on
00:32:35
The refractive index of water is
00:32:38
unit is air per
00:32:44
sine 90 which is also equal to one then
00:32:50
there it turns out to be the sine of the total
00:32:53
internal reflection
00:32:54
one for the refractive index of water here
00:32:57
so you can find the whole thing
00:33:12
No need to enter the name of the law no
00:33:15
it is enough to write the formula of the law
00:33:18
I know what it is
00:33:21
some teachers who yell from
00:33:25
all the cracks that you have not written the name
00:33:28
the law will not give you the maximum
00:33:31
point no this is a fallacy I don’t know how
00:33:35
how many years do I still have to fight this?
00:33:37
I already posted my varik in which
00:33:40
your work for which they gave 100
00:33:42
points I didn't write a single title
00:33:44
laws just wrote the formula for this
00:33:47
enough but this teacher
00:33:49
still this is not enough they continue
00:33:51
continue to talk and carry all kinds of heresy in
00:33:55
in general, don’t listen to teachers who
00:33:57
They say that a name is also required
00:34:00
law and formula can be one or the other
00:34:03
only the formula or only the name
00:34:08
what can I say to this teacher
00:34:10
who continue this anyway
00:34:12
I can say I wish them something to eat
00:34:16
I won't I won't I won't I won't
00:34:20
talk bad about people
00:34:27
go ahead
00:34:34
so this is ours
00:34:37
task
00:34:39
point light source is in
00:34:41
containers with liquid and lowered
00:34:43
vertically down from the surface of the liquid
00:34:46
while on the surface of the liquid
00:34:48
a spot appears within which the rays
00:34:50
light from the source comes out of liquids
00:34:53
air source immersion depth
00:34:55
distance from the surface of the liquid to
00:34:57
light source measured measured
00:34:59
at regular intervals and
00:35:01
corresponding bright spot radius
00:35:03
presented in the table
00:35:07
so what is the refractive index
00:35:10
liquid answer to within
00:35:12
hundredths
00:35:16
So
00:35:18
means that you and I see
00:35:21
we see that he has
00:35:25
we are a bright spot let's discuss how
00:35:29
it is formed
00:35:31
it's not that bright spot when you're in
00:35:34
you float up in the pool you feel warm
00:35:36
this is a little different, imagine this
00:35:38
you have a light bulb like this on
00:35:42
Basik day, well, not for a day, just here
00:35:44
somewhere there is a light bulb and these rays
00:35:46
these rays come out from the surface
00:35:50
Ivan, well, it seems that the place is illuminated here
00:35:54
yes, and at some point the beam came out
00:35:58
refracted here and at an angle of 90 degrees
00:36:01
that is, this just applies to the angle
00:36:03
total internal reflection
00:36:09
so that means we can do it
00:36:14
spot radius
00:36:17
let's take the very first option 10
00:36:21
10 cm, that is, I’ll erase this radius
00:36:26
10 centimeters and immersion depth in
00:36:30
this moment h is equal to
00:36:33
8 centimeters turns out we can find
00:36:38
this is the corner bed and that is, if here
00:36:40
draw here like this, then here too
00:36:43
will be 8 cm
00:36:44
and here it will also be 10 centimeters then
00:36:50
[music]
00:36:51
it turns out that this is the hypotenuse
00:36:57
Let's
00:36:59
let's use the Pythagorean theorem, here we go
00:37:02
this hypotenuse is 8 squared plus 10
00:37:05
squared guy from 164
00:37:10
oh what a stupid number to assign to him
00:37:12
sung
00:37:14
10 to the root of 164 is obtained
00:37:18
refractive index knives question on
00:37:21
these one for sine this thing for 10 for
00:37:27
root of one hundred and sixty-four notes n
00:37:29
this is one on sine theta and then this
00:37:34
here's the thing we've got, let's do it
00:37:36
let's calculate how much it comes out and here I am
00:37:38
write guys suggest this 128 if
00:37:43
round to the nearest hundredth
00:37:44
thank you I will believe you because I
00:37:47
lazy
00:37:49
just lazy I was too lazy to finish
00:37:52
phrase
00:37:53
lazy who
00:37:58
[music]
00:38:02
while I'm alive studios I want her to show up
00:38:05
sense
00:38:20
so I erase all this
00:38:35
the stream will last up to 6 hours even
00:38:38
It’s more unfortunate that I’m slowing down
00:38:43
Everything is safe enough with our likes
00:38:46
by likes
00:38:49
573
00:38:55
This doesn’t make me happy by the way where are the likes
00:38:59
I try and you like if the light comes from
00:39:05
substances with refractive index n in
00:39:08
vacuum here it is by the way if in more
00:39:13
tight then the angle actually
00:39:15
increases
00:39:18
limit angle of total internal
00:39:20
reflections
00:39:22
equals 45 what is equal to a
00:39:26
ok then, well, in short, here he is at 90
00:39:32
comes out
00:39:33
it turns out sine 90 sine alpha there 790
00:39:41
by 1 is equal to n times sine alpha and that means
00:39:46
exponent one per sine
00:39:50
alpha 1 per sine
00:39:53
45
00:39:56
is the root of 2 the root of two
00:39:59
this is 143 if up to 24 hours it’s rubles I don’t have
00:40:03
I thought I read this in the chat
00:40:06
Thanks guys
00:40:10
Thank you yourself for the hall Taurus a little
00:40:13
Friday Primus broadcast carts was
00:40:15
It's nice to listen to him and thank you for that
00:40:17
watched too
00:40:24
141
00:40:27
someone let me down another 1 1 but
00:40:43
maybe we won't get it anyway
00:40:46
1000 likes for this ferrari
00:40:48
I don’t remember the stream you dialed me
00:40:51
still like a
00:40:53
140 cops
00:40:56
141
00:40:57
141 because
00:41:00
1414 if after the units there are 4 then we round
00:41:03
downward
00:41:07
units because the vacuum is up to the indicator
00:41:10
refraction in vacuum alone and in air
00:41:14
almost 1 actually
00:41:16
compared to water up to then can be considered
00:41:24
light comes from matter where is the speed of light
00:41:29
265
00:41:34
265
00:41:36
one meters per second
00:41:40
conducted matter where the speed of light is 285
00:41:45
meters per second what is sine equal to
00:41:49
limit angle of total interior
00:41:51
reflections, express your answer accurate to
00:41:53
decimal means let's repeat it again
00:42:00
reports to think
00:42:03
ok, let me describe us in more detail
00:42:06
it turns out
00:42:08
n1 per sine alpha is equal to n 2 per sine
00:42:13
tetta
00:42:15
means in a less dense environment
00:42:19
where the speed of light is greater we should
00:42:23
be 90 degrees means who should I
00:42:26
charge for 90
00:42:28
degrees alpha or beta which is equal to 90
00:42:33
degrees
00:42:38
first option alpha second option beta
00:42:57
Hello Alexander, how are your joints?
00:43:01
although they just started asking for reports
00:43:03
It seems like my joints are always fine
00:43:05
was
00:43:07
hips b option beta that is, we have
00:43:11
it turns out n1 this price one per sine
00:43:17
alpha is equal to price 2 times sine 90 then
00:43:23
sine alpha
00:43:25
1 in 2 and it works
00:43:29
265 to 285 but even if you were wrong
00:43:34
it's okay because you would
00:43:36
got a sine greater than one that
00:43:38
says that you would have confused
00:43:41
to correct
00:43:42
so 2.65 is a divisor by 2.8
00:43:46
50 929 taking into account so to within
00:43:51
thousandths
00:43:53
round by 1000
00:43:56
093 extra 09
00:44:01
298 if rounded to thousandths then this is in
00:44:05
large side to dishes 0
00:44:07
It’s clear that we’ll round up to thousandths, but
00:44:11
the answer came with photos
00:44:31
do not write down exactly 093
00:44:37
the bottom will be salty
00:44:40
looks depends on whether
00:44:42
tear my bottom
00:44:43
inclusive
00:44:45
I try not to take a break because
00:44:48
that it’s hard to fit the entire webinar into 6 hours
00:44:51
so much information
00:44:53
the most concentrated information
00:44:56
six o'clock at
00:44:57
what a handsome guy who came in
00:45:00
so a beam of light falls from air into
00:45:04
glass what happens to
00:45:06
frequency of electromagnetic oscillations
00:45:08
light wave speed
00:45:10
propagation wavelength for each
00:45:12
values ​​determine the appropriate
00:45:13
nature of changes
00:45:16
without 0 the error will not be so already rounded
00:45:20
to thousandths but the number turned out to be from
00:45:25
rounded to thousandths like this
00:45:26
cleanliness guys everything never changes
00:45:32
remember as our father
00:45:35
What was the frequency? What remains?
00:45:39
speed in a denser environment in water
00:45:42
ours is written there from air into glass
00:45:48
glass
00:45:49
glass but will move slower
00:45:52
so well, it seems to me purely if you
00:45:55
fumble a little and understand how it leads
00:45:57
All
00:45:59
light do you understand that
00:46:02
it would be brut brud it was clear what we were talking about
00:46:06
wavelength
00:46:08
wavelength let's think about it
00:46:11
wavelength is speed
00:46:16
multiplied by
00:46:18
divided by purity
00:46:20
speed doesn't change
00:46:23
oh frequency does not change speed
00:46:26
decreased means the wavelength too
00:46:29
will decrease
00:46:30
get up here is how the wave behaved
00:46:33
so I have the same one
00:46:37
frequency moves back and forth but due to
00:46:39
that it’s not the speed that has decreased
00:46:40
slowly became smaller
00:46:50
take a break for half an hour
00:46:53
[music]
00:46:59
so now let's
00:47:02
let's check
00:47:03
how much do you fumble the same question
00:47:08
but the sound
00:47:10
that's if the sound
00:47:13
you said the score there
00:47:16
someone
00:47:27
imagine that
00:47:33
you you someone this you your friend
00:47:37
[ __ ] on the back and dived into the pool and you
00:47:40
You yell something at him and there’s a sound
00:47:44
extends to and
00:47:47
here it is now spreading in the water
00:47:51
please tell me how it will behave
00:47:55
purity
00:47:59
propagation speed and length
00:48:02
sound wave now write again
00:48:20
oh handsome guys oh well done look sound
00:48:24
the wave behaves a little differently than the sound wave
00:48:27
wave, the denser the medium, the better because
00:48:30
what's going on this is what's going on
00:48:32
mechanical transmission that is, here you are
00:48:35
imagine you are in a crowded subway
00:48:37
someone was pushed
00:48:39
the next person starts to fall and
00:48:42
pushes the next one the closer these people are
00:48:44
are here this one pushed this one
00:48:46
this one pushed this one pushed this one and
00:48:48
Here the wave turns out to be transmitted quickly
00:48:51
if the medium is dense therefore the speed is in
00:48:54
water
00:48:55
the water will increase here if that speed
00:48:58
distribution will increase and again by
00:49:00
same formula 1 speed
00:49:03
spread has increased in frequency
00:49:04
remained the same, then the wavelength also
00:49:07
will increase so don't confuse the sound
00:49:10
electromagnetic waves
00:49:12
they behave differently in the environment
00:49:17
there is in the water if you scream then
00:49:19
the speed of sound will be much greater
00:49:25
why are there 666 likes oh
00:49:34
well done
00:49:37
well done brothers on the theory it was before
00:49:42
go ahead
00:49:47
A
00:49:48
so we moved on to the difficult part then there
00:49:52
waited with a spoon it started
00:49:55
guys listen to the refraction of light
00:49:57
maximum
00:49:58
details about
00:50:15
cool thanks bro find the corner
00:50:19
falling light beam into glass
00:50:21
the plates are plane parallel at
00:50:23
offset 168 millimeters
00:50:31
if at offset
00:50:34
one millimeter angle of incidence is
00:50:38
30 degrees
00:50:40
one millimeter angle of incidence
00:50:45
sinus
00:50:48
oh oh frame 30 play
00:50:52
So
00:50:58
refractive index
00:51:00
155
00:51:02
15
00:51:04
labor
00:51:08
I'll start eating here we have a plane parallel
00:51:11
plate how light behaves
00:51:16
when falling
00:51:18
here that goal alpha angle of incidence
00:51:21
getting smaller
00:51:24
environment
00:51:27
same here
00:51:30
then it turns out it turns out, but it’s
00:51:35
alpha there too
00:51:37
we call one and
00:51:39
it turns out that it’s in the air here, but we’ll be there
00:51:43
count approximately one
00:51:45
here with us
00:51:47
155 and here in the air again approximately
00:51:52
units are obtained n air
00:51:55
air on
00:51:57
sine alpha equals n times sine theta
00:52:02
again the same thing here n times sine
00:52:05
theta equals n times sine alpha 1 n air
00:52:12
that is, if you look at this here
00:52:15
then it turns out he comes out under the same
00:52:18
the angle that came in is why we say
00:52:20
about
00:52:21
parallel displacement of the beam, that is, here
00:52:24
he moved
00:52:26
by some amount by a value d
00:52:29
let's now think about how this value
00:52:31
d can be found find it can be found enough
00:52:35
we just see that this leg d is like
00:52:39
since you take this angle well, let's
00:52:43
I'm so heroin to him red
00:52:45
I’ll indicate this angle that’s interesting to us
00:52:49
how to find this angle red let's
00:52:52
and a warrior on this
00:52:55
this is the letter indicated
00:53:01
gamma from home
00:53:04
by the way, what is the gamma equal to chat?
00:53:07
write
00:53:10
write dear
00:53:22
alpha minus b handsome guys that is
00:53:25
we get like vertical angles
00:53:28
these here we have alpha equals beta plus
00:53:31
hama hama this is alpha minus b to b then
00:53:35
can be found from the law of refraction then
00:53:38
is in this form here if
00:53:40
take advantage of sine beta
00:53:42
sine alpha by
00:53:47
n n air approximately 1 and
00:53:52
it turns out
00:53:56
What
00:54:00
hence beta is arc
00:54:04
sine sine alpha on n that is beta y
00:54:09
we exist now what we do with you we
00:54:13
we know that the width of the plate is up to
00:54:19
then the cosine of theta is equal to divided by y
00:54:26
on the other side
00:54:29
sine gamma equals b divided by the same
00:54:33
the y is already from this triangle
00:54:36
then from these two things you and I
00:54:39
we get that sine gamma divided by sine
00:54:43
on execute and on cosine beta
00:54:47
equals h
00:54:50
take
00:54:52
d divide by y very d divide our there
00:54:57
all that remains is
00:54:58
Here
00:55:16
so ask me to show the hour angle
00:55:19
incidence of light beam
00:55:24
alpha 1 is alpha 2 that is
00:55:30
you and I know
00:55:34
What
00:55:36
sine gamma one
00:55:43
per cosine beta 1
00:55:47
equals d 1 divided by h and sine gamma 2 by
00:55:54
cosine beta 2 equals d 2 divided by a
00:55:59
what exactly follows from this?
00:56:05
sine gamma one by sine gamma 2
00:56:12
by cosine beta 2 by cosine beta 1
00:56:19
equals b 1 divided by d2
00:56:23
so now if I
00:56:27
I'll set you up
00:56:29
what I know
00:56:36
it turns out sine gamma
00:56:39
This
00:56:41
alpha 1 minus
00:56:45
arcsine sine ive 1 divided by n
00:56:57
sinus
00:57:00
to sine
00:57:02
alpha 2 minus arcsine
00:57:06
sine alpha 2 divided by r
00:57:10
then I get d 1 divided by d2
00:57:21
yo-ma-yo a
00:57:26
so I have it I can find it
00:57:30
this is what I can find
00:57:34
it's like how do I solve this
00:57:38
damn it
00:57:45
These curators made my task more difficult
00:57:49
she turned into some kind of dregs
00:57:58
why else do I know about
00:58:00
sinus
00:58:08
in general I think this is possible
00:58:11
decision to finish two numbers because
00:58:16
well this is kind of [ __ ] up
00:58:20
in fact, everything is usually much better there
00:58:23
easier
00:58:24
brought to 2 beta, we also need to reach the goal
00:58:27
well damn it's a sine
00:58:32
sine alpha 2 by n
00:58:35
sinus
00:58:38
Naturally this can’t happen guys
00:58:41
it is very important for you to understand
00:58:46
Yes, what is important for you guys to understand
00:58:49
it's important to understand that you can do this
00:58:52
you can write it down like this and
00:58:56
What
00:58:59
angle at which it falls on a plane
00:59:01
parallel is equal to the angle at which
00:59:03
exits parallel search and
00:59:09
let me, there are two things to consider here
00:59:11
triangle but my curators were just
00:59:16
let's go too far, let's go too far
00:59:20
let's know what we'll do
00:59:24
let's change this a little bit
00:59:27
let us give alpha 1 the task
00:59:35
alpha 1
00:59:37
so what happens if the angle of incidence
00:59:47
let's remove d2 a bit instead, let it
00:59:51
conditions will be alpha where I am like this
00:59:53
changed the conditions of the problem but so that it
00:59:55
was solvable
00:59:58
let alpha 1 be 45 degrees to cairns
01:00:03
what is it equal to and
01:00:04
they ask what the displacement is equal to then
01:00:07
this problem becomes solvable
01:00:10
So
01:00:13
Well, let's now express express
01:00:16
what is d 2 in this case?
01:00:30
d2
01:00:33
This
01:00:36
d1
01:00:41
let's express first
01:00:43
on
01:00:45
these are not a shuttlecock right away, let's express d1 by
01:00:49
sine alpha 2 minus arc sine sine
01:00:53
alpha 2 on n
01:00:57
by cosine
01:00:59
sine alpha 1 by n
01:01:03
divide by sine alpha 1 minus
01:01:08
arcsine of sine alpha-1 by n by cosine
01:01:13
sine alpha 2 on n
01:01:17
that is, you are setting the guys up, and I
01:01:21
I will write what you tell me even with
01:01:25
the game was wrong
01:01:28
so do the math on the calculator
01:01:32
please sine before me
01:01:35
alpha 2 is 30 minus
01:01:39
arcsine of sine
01:01:42
30 per
01:01:44
155
01:01:46
by cosine of sine
01:01:51
45 by 155 and below the sine
01:01:58
alpha 1 is 45 minus arc sine of sine
01:02:06
45 by 155 by cosine of sine
01:02:17
what the hell did I write down
01:02:21
arcsine
01:02:26
arcsine of sine and
01:02:34
cosine
01:02:36
from arcsine sine
01:02:41
alpha 2 on n
01:02:45
arcsine sine alpha 1
01:02:48
and this is equal
01:02:51
d1 to d2
01:02:56
here
01:02:58
arc cosine
01:03:01
And
01:03:03
here
01:03:04
cosine of arc sine
01:03:17
cosine like this
01:03:19
sine and
01:03:22
cosine of arc sine sine 45 by
01:03:30
155 I'm sick of it
01:03:37
thanks to the curator damn it, okay who?
01:03:41
I didn’t count or no one counted
01:03:49
I'll count
01:03:54
O
01:04:02
counted up
01:04:13
I'll check how I set people up
01:04:17
everything is correct
01:04:32
van that little was considered
01:04:36
I'll have to count here
01:04:51
here 30
01:04:59
sine 3
01:05:25
because
01:05:33
here means sine 45
01:05:37
minus
01:05:39
arcsine
01:05:46
/ sine 45
01:05:51
deep sea 5
01:05:56
like this
01:05:59
like this
01:06:02
so equal
01:06:10
so we respect
01:06:14
divided by the cosine of the arcsine
01:06:20
fraction sine 45
01:06:24
But
01:06:27
all five
01:06:32
cosine divider
01:06:38
arcsine
01:06:41
dad sine 30
01:06:46
155
01:06:49
two brackets close
01:06:56
so in general it worked out for me
01:07:01
099 8 7 millimeters a
01:07:10
By the way
01:07:12
well, like about 1 millimeter essentially I
01:07:16
I hit the sky with my finger, I guessed which one
01:07:20
the angle should have been in the thirtieth
01:07:23
that is, I guessed it and then
01:07:24
it actually turns out to be a shift by one
01:07:27
a millimeter but it's just a miracle gentlemen
01:07:31
ok, in general, we coped with the task
01:07:34
although very somehow for a sage for a sophisticated one
01:07:38
variation ok thanks anyway
01:07:40
to my curator for such interesting things
01:07:44
steamed of course conditions
01:07:49
that is, the answer in the original number would be
01:07:52
30 degrees turns out
01:07:59
yeah, put it down and that's when mine
01:08:02
curators come up with wording they
01:08:05
Apparently they are lazy about solving problems themselves
01:08:09
So you swapped the numbers and
01:08:12
changed there what is being asked but you
01:08:15
I am sure that this can really be resolved within the framework
01:08:17
school curriculum anyway
01:08:19
in this case the person did not check
01:08:21
I haven’t tried to solve it myself, obviously, but
01:08:24
ok I'm twenty what
01:08:26
you can do it
01:08:34
the actual depth of the lake is
01:08:37
3, 4 meters a
01:08:41
ice thickness 65 centimeters
01:08:46
What is the depth of the lake to a fisherman?
01:08:48
show someone standing on transparent ice
01:08:50
melting ice 131
01:08:54
water 133
01:08:58
so look here with us
01:09:02
let's say for us because it seems to the fisherman
01:09:06
look, this is ice, this is good for a fisherman
01:09:09
it seems like this
01:09:11
the bottom is here so let's do it
01:09:14
he's looking at the coin and looking at it
01:09:17
looks at the coin from the coin
01:09:20
the light is reflected, it seems to him that this
01:09:22
the light is reflected like this, that is, like ours
01:09:24
the eye is made our eye sees
01:09:29
a diverging beam of rays that
01:09:31
gets into it and completes the construction
01:09:33
direct eye image stupid he is not
01:09:36
understands that something is bent there but
01:09:38
in fact this beam hits the eye
01:09:41
differently, let's see how he's doing
01:09:44
actually gets it, that is, he
01:09:46
goes like this, which is at a right angle
01:09:48
he doesn't change at all, but this one is coming
01:09:51
like this, that is, first it goes at an angle
01:09:53
alpha let's use different colors
01:09:55
draw so where is green green then
01:09:59
He
01:10:00
decreased
01:10:02
is already going at an angle or even
01:10:08
at the interface of this medium he
01:10:11
changed again and
01:10:14
goes at an angle gamma
01:10:18
like this
01:10:21
gamma and
01:10:23
in fact this is a coin
01:10:27
is located here, that is, this
01:10:31
Seems
01:10:33
this is reality the real situation
01:10:36
coins, that is, this coin right here
01:10:40
the archer sends
01:10:41
and here sending a ray that
01:10:43
refracted refracted and general
01:10:45
gets into the eye and when our eye sees
01:10:48
a diverging beam of rays then it’s his
01:10:50
so finish it this way well I do
01:10:53
drew that they are far away but on
01:10:55
this is actually a small distance
01:10:57
we will assume these angles are small
01:11:01
consider
01:11:04
small
01:11:05
angles
01:11:08
then sine alpha is approximately equal to alpha and
01:11:13
approximately equal to tan alt for small
01:11:15
corners
01:11:17
it turns out
01:11:19
if I express
01:11:23
let's say
01:11:26
here let's x1
01:11:31
here it is and here it is
01:11:36
It turns out that sine is gamma
01:11:41
equals x 1 divide our if I will
01:11:45
express sine beta
01:11:48
this little tash this is x2
01:11:51
it turns out that sine theta is equal to x 2 divide
01:11:56
on oh sorry not the force Sarah tangent well
01:12:01
tangent is equal to sine
01:12:04
sinus
01:12:06
approximately equal
01:12:08
approximately
01:12:10
sine beta
01:12:13
so then from here I can conclude
01:12:18
What
01:12:22
hx1
01:12:25
equals
01:12:30
as much as sine gamma
01:12:34
x2
01:12:37
equals h sine battan and
01:12:44
now let's look at just the angle
01:12:47
alpha, that is, this is how it seems to us they will be
01:12:50
there will also be alpha and this is the distance you
01:12:53
x1 plus x 2 and
01:12:59
what is the depth of the lake
01:13:08
so so so
01:13:13
lake depth fish
01:13:17
here's football
01:13:27
Apparently I'm just thinking what's being asked
01:13:30
but I'm glad I understand that what's being asked here is not
01:13:34
the depth is exactly the lake
01:13:40
depth
01:13:42
just from the surface to the bottom
01:13:46
to the ice surface to the bottom
01:13:50
let's find it means b&b questions and
01:13:54
then for the tangent alpha which
01:13:59
approximately equal to our sine alpha
01:14:03
it turns out this ratio will be x 1 plus
01:14:07
x 2 divided by b
01:14:12
therefore x1 plus x 2 equals b sine
01:14:17
alpha
01:14:18
so everyone understands what we did
01:14:21
Hope
01:14:31
actually it's possible
01:14:33
you can find this problem here
01:14:39
it will seem to him
01:14:41
the ice ends where it seems to him
01:14:45
ends in begins ends
01:14:47
water but it will take too long I need it
01:14:50
it will still be
01:14:52
consider the case when he looks at
01:14:54
ice where he thinks the ice is and damn
01:14:59
I don't think it's worth it anyway
01:15:04
let's just find the depth at which
01:15:06
there is a bottom from the surface of the ice here and
01:15:08
everything turns out that sine is alpha
01:15:15
1 is equal to the refractive index of ice
01:15:19
on
01:15:20
sine beta
01:15:23
where can we find
01:15:27
sine beta
01:15:30
it is equal to sine alpha divisor by nld
01:15:34
also we can find the sine
01:15:38
gamma over n water is equal to sine theta
01:15:44
on n ice and
01:15:47
it is equal to the sine alpha of this
01:15:51
it turns out therefore sine gamma
01:15:54
equal to sine alpha times n water and
01:16:00
in general this way
01:16:05
we can work with you
01:16:07
find this distance b
01:16:10
this is the distance then
01:16:13
will
01:16:16
if x1 is substituted it’s already
01:16:21
on
01:16:25
sine alpha by n water + x 2 substitute
01:16:31
this is as much as
01:16:33
sine iPhone and ice
01:16:41
equals
01:16:44
Now
01:16:50
b to sine alpha, that is, this is what we have
01:16:54
will happen in this case
01:16:56
that is, we have ice depth
01:17:02
the depth at which the water is located and
01:17:04
ice depth
01:17:07
will decrease by a factor of refractive index
01:17:10
that is, by the way, it’s cool to look at
01:17:13
this is what actually seems to be
01:17:16
depths this is it
01:17:20
apparent waters a
01:17:24
this is the apparent depth of the ice and
01:17:30
we can now count it
01:17:33
b
01:17:36
means your big 3, 4 divided by water
01:17:42
133
01:17:44
plus
01:17:46
065 on
01:17:49
131
01:17:53
So
01:17:56
count the fraction 3 4 divided by 133
01:18:01
+ 0 all 5 divided by 131
01:18:07
it turns out 3
01:18:10
as much as 0 5 meters in total
01:18:16
in fact, by the way, she’s not that much
01:18:20
different please note that is there
01:18:25
3.4 although it is indecent there are four meters but
01:18:28
approximately 4 meters actual depth
01:18:31
it looks like it's three meters there
01:18:35
approximately four-thirds times
01:18:37
is different So let’s write it down anyway
01:18:43
apparent ice and apparent in, well, that is
01:18:47
here is the apparent
01:18:49
water
01:18:51
here is the apparent ice and
01:18:57
you can also paint them, that is, if I
01:19:00
Here
01:19:01
I am writing an apparent
01:19:04
3-4 water will be here
01:19:08
256
01:19:10
meters, well, approximately, but the apparent ice is
01:19:15
there will be 065 divisor by
01:19:19
131
01:19:21
it will be located at 0 496
01:19:26
meters
01:19:28
well, this is how it will be distorted
01:19:56
this is the height from the surface to the ice
01:20:00
more likely
01:20:02
from the surface to the ice on there
01:20:05
really deep lake
01:20:07
[music]
01:20:15
ok guys we won't
01:20:18
easy to redo
01:20:22
so you know the wording is like this
01:20:25
it turned out that but it’s not completely clear
01:20:28
what did they mean
01:20:31
the depth of the lake is from what to what but
01:20:34
if yes if the depth of the lake
01:20:36
meant from the ice surface to
01:20:39
bottom of the water then we would take it there
01:20:43
this width is such a big minus
01:20:46
h a little well, it’s understandable and that’s why
01:20:48
the meaning doesn't change, the main thing is that you
01:20:50
generally understood what was happening at the game
01:20:53
everything will be formulated clearly, how
01:20:56
rule there are no such uncertainties but
01:20:58
was again forgiven by his curator for
01:21:01
such a formulation, in general, the main thing is that
01:21:04
you understood the meaning
01:21:06
so let's move on
01:21:09
in general, in short, what is the moral of this
01:21:13
fables and
01:21:15
we can prove it
01:21:17
in some environment
01:21:20
apparent depth
01:21:23
refractive index times less than
01:21:27
in real
01:21:29
that is, imagine this means
01:21:33
you want to slap someone's ass
01:21:43
that's his ass
01:21:45
here she is at some depth
01:21:48
And
01:21:49
You
01:21:51
when will you
01:21:53
to swing you need to aim a little
01:21:57
below a
01:21:58
specifically four thirds if you are in
01:22:01
hit the water, that is, if you are under water there
01:22:05
you see an ass at a distance of 30
01:22:08
centimeters then you need to move 10
01:22:11
centimeters down, that is, spanking and so on
01:22:13
as if you were on
01:22:15
hit at a depth of 40 centimeters and
01:22:20
then everything will be clear you will get there
01:22:28
Sanya why even divide by nb this
01:22:31
apparent
01:22:32
the distance is easy to deduce if
01:22:34
we just had the same environment, here it is
01:22:37
logical reasoning
01:22:44
let's all move on
01:23:45
a parallel beam of light falls from
01:23:47
air on a stack of four flat
01:23:49
parallel glass plates and
01:23:51
comes out of it at an angle of 45 degrees like this
01:23:54
beta 45 degrees at what angle is the beam
01:23:59
entered this pile if the indicator
01:24:01
refractive index of the plate is equal to 1 of
01:24:06
71 of 71
01:24:10
from 6 and
01:24:15
15 and 14
01:24:20
So
01:24:23
this is how I entered if I left at 45 and here
01:24:30
will help us
01:24:32
Snell's formula and not written in
01:24:37
in the form of sine alpha divided by sine beta a
01:24:40
in the form n multiplied by sine equals
01:24:43
sine is equal to them by sine that is what I mean
01:24:46
I say you have an alpha angle
01:24:49
then he is a beta there and here and here
01:24:55
Then
01:24:58
gamma
01:25:03
here he is, highlighting the task
01:25:07
etc.
01:25:12
and then there is sigma
01:25:16
sigma they take it yes here is sigma
01:25:20
here too sigma and here even
01:25:28
lunch and upstairs balyan so here for something else
01:25:32
come up with
01:25:34
that the single
01:25:37
gamma
01:25:38
[music]
01:25:40
I forgot what it's called
01:25:44
look, well, if you use this one
01:25:47
this is the formula I showed you
01:25:50
then everything becomes quite simple
01:25:55
no matter what happened between them
01:25:58
provisions, the main thing is that he was in
01:26:01
air
01:26:02
n air multiplied by sine alpha then
01:26:07
he's there n1 sine psy
01:26:10
n 2 sine gamma
01:26:15
n3 sine theta
01:26:19
n4 sine sigma and then still n
01:26:25
air sine beta what happens here
01:26:29
this thing is equal to this thing and just
01:26:31
alpha anyway I could do it right away
01:26:34
write I wanted you to remember
01:26:37
so as not to torture yourself
01:26:39
with these complex calculations
01:26:44
task file in cart
01:26:50
pdf in
01:26:53
cart
01:26:56
in the cart
01:27:01
f.b.
01:27:03
No
01:27:16
so, okay, let's move on in general
01:27:19
generally entered at the same angle at
01:27:22
which came out
01:27:55
so I completely missed the schedule
01:27:58
I wonder how much I love him
01:28:00
I'm falling behind
01:28:01
so 13 3 6 and according to the plan I should have
01:28:09
when a
01:28:13
well, I’m behind but not much by 16 minutes
01:28:16
normal
01:28:18
human yes guys
01:28:21
let's talk about it, a couple of things
01:28:25
Let's take a little break, which means
01:28:28
what does it mean to be first on the news?
01:28:31
news if we get 1000 likes
01:28:37
become a man and close to this I am
01:28:42
I'll cut the electro for the new car
01:28:46
by itself, here we have 3 pieces in Rome today
01:28:50
but I understand that nothing will happen to me
01:28:54
I'll just cheer myself up properly so
01:28:58
put likes, I’m even interested in it
01:29:01
how energized I'll be after
01:29:05
of this action
01:29:06
oh, of course it’s scary and a little bit, but I’m already
01:29:09
fought so nothing fatal
01:29:11
scary
01:29:14
someone free dislikes beats me here
01:29:18
for 1000 likes
01:29:20
so what else
01:29:24
if you are in eleventh grade and
01:29:27
create and gene most likely this is so
01:29:29
because I have such people there now
01:29:31
look then you can sign up for my
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which starts on May 25th on which you
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We'll get through everything, write in our group at
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01:29:45
sign up with a discount so
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subscribe sign up for intensive
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start 25
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you need to buy dough, it can be difficult, it can be
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this is this together that is there you will lead
01:29:58
have all your knowledge in order and come to
01:30:01
exam fully armed, show yourself with
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the best side of a
01:30:05
if you are a tenth grader, then follow the link below
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video again you can sign up before
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You will also attend summer school
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get a summer intensive get records
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ebonite 2022 in general is absolutely colossal
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some amount of water, that is, a record
01:30:28
the hospital of 2022 will be available to you
01:30:31
In any case, we open the duvan earlier
01:30:33
will be available earlier than others immediately
01:30:35
After the exam, in general, go to
01:30:37
link in description to order
01:30:39
pre-register our group in contact again
01:30:41
the same but also from our heroic teachers
01:30:45
which also work great already too
01:30:48
someone started intensively to whom
01:30:50
then soon we won’t miss everything
01:30:53
advertising is over
01:31:09
so guys let's talk about now
01:31:16
thin line formula
01:31:20
the path is normal
01:31:23
enough of this childish humor
01:31:30
V
01:31:34
2 draws
01:31:38
like children so
01:31:41
Means
01:31:43
what what else let's get started
01:31:48
lenses what we know about
01:31:51
converging lens
01:31:57
it turns out if it falls on it
01:32:01
parallel beam
01:32:05
this is called the main optical axis
01:32:08
all these rays are refracted
01:32:11
into focus
01:32:13
I won't drink.
01:32:15
so they will all go through the trick
01:32:20
it’s clear guys the beam that passes through
01:32:24
center of the main optical axis
01:32:25
it won't refract at all
01:32:27
went on and on
01:32:30
now if we
01:32:33
direct the beam
01:32:35
let me show you separately now, that is
01:32:38
now if the rays go through the center of the main
01:32:40
it doesn’t change the optical axis in any way
01:32:45
its trajectory as it went and goes
01:32:49
this one would also go better in the general center
01:32:52
The main optical axis is very convenient.
01:32:55
to direct the beam because it's better not
01:32:58
change their direction
01:33:02
so what happens if
01:33:05
the rays fall at an angle, let's say here
01:33:09
our beam goes like this
01:33:12
where will he go next
01:33:14
for this you need to draw the focal
01:33:17
plane focal plane is but
01:33:20
passes through a point
01:33:22
focus on the main optical axis and voila
01:33:26
through . you draw a plane then you
01:33:28
build an auxiliary angle
01:33:31
parallel and
01:33:34
all the rays that are fed in parallel are here
01:33:37
this passing through the center of the passing
01:33:39
must not be refracted through the center
01:33:41
intersect at one point at the focal
01:33:43
planes, that is, they will all intersect
01:33:45
here, and in particular this beam
01:33:49
will go further here like this
01:33:51
build a beam incident at an angle
01:33:55
at an angle
01:33:56
but also if we use the property
01:34:00
reversibility
01:34:03
diameter in geometric optics then we have
01:34:07
it turns out if
01:34:09
in focus
01:34:11
the source is located
01:34:13
then this source hits the lens
01:34:17
how to go further
01:34:20
parallel
01:34:22
this is how the rays will go
01:34:25
that's why if you want accurate
01:34:28
turn the source into parallel
01:34:32
source
01:34:33
homogeneous field, then you can put it into the lens
01:34:37
place it at 0 and point it at the lens
01:34:40
By the way, I did it in a program in one
01:34:42
to show the dispersion effect
01:34:46
So
01:34:48
And
01:34:50
the latter again I use reversibility
01:34:53
rays if you have a focal plane
01:34:56
the source is located
01:35:00
then when it hits the lens
01:35:05
this one doesn't refract until
01:35:09
the rest are underway so they all go
01:35:13
parallel to this one which is not
01:35:15
refracted
01:35:17
also run in parallel
01:35:20
this is what concerns the collecting lens and
01:35:25
I'm washing
01:35:59
focal plane passes through focus
01:36:02
perpendicular to the main optical axis
01:36:05
to define a plane it is enough to specify
01:36:08
point and
01:36:10
that's the straight line it will be
01:36:13
perpendicular
01:36:15
So
01:36:17
Now
01:36:19
what does a diverging lens do?
01:36:22
We’ll also discuss it quickly
01:36:26
she makes it a parallel beam
01:36:30
the rays seem to come from the back
01:36:32
focal plane
01:36:34
that's what she does
01:36:41
that is, they behave better as if
01:36:45
they shone from this point, that is, if
01:36:48
I'll point it at the diverging lens
01:36:51
parallel beam of rays then you too
01:36:53
look at this light then you will
01:36:56
seem like he's in focus
01:36:58
it will seem to you that the image is there
01:37:01
located actually just checked
01:37:03
beam of rays falling
01:37:05
So
01:37:08
that's all well
01:37:11
let's probably
01:37:13
Let's move on to solving the problem: fine formula
01:37:16
I'll show you the lenses in practice
01:37:26
probably here
01:37:30
I'll do that in the picture there
01:37:36
one cell two centimeters what is it
01:37:40
focal length let's do this
01:37:43
let's continue this line
01:37:51
this straight line will continue like this
01:37:55
I'll continue this straight
01:38:01
bright understanding somewhere a or higher should
01:38:04
were to cross paths
01:38:08
bolin oleg steel beveled shorter actually
01:38:13
in fact they should
01:38:15
intersect at this point, that is, we
01:38:18
Let's assume that it's all one. OK
01:38:22
it turns out our lens is located
01:38:25
here
01:38:27
this is where our lens is located
01:38:32
Now
01:38:41
were it turns out that with such cream
01:38:45
we won't be able to clearly find the picture
01:39:05
let me just fix the drawing
01:39:09
in general
01:39:12
Oleg just squinted but that should have been it
01:39:16
go like this
01:39:18
Here
01:39:20
a year since the beam was supposed to go in reality
01:39:23
guys, but excuse me, our braids are crooked
01:39:26
there he went a little to the side and everything was already
01:39:29
it turns out wrong and it turns out ours
01:39:32
the lens should be clearly located here
01:39:36
our collecting lenses will be located and
01:39:46
it turns out that
01:39:48
we can build an auxiliary beam
01:39:51
let's give him a little black one
01:39:54
parallel to our incident ray and
01:39:59
we know that it will intersect with
01:40:02
by this focal plane ray, that is
01:40:04
here is the focal plane, here it is
01:40:07
purple
01:40:10
just about the focal plane, that is, here
01:40:12
here is the focus
01:40:19
here is the focal point, that is, we have one
01:40:22
a cell is two centimeters
01:40:24
that means focus is 2 cm, let’s write it like that
01:40:30
f-no two
01:40:33
centimeter
01:40:41
the arrow skewed a little but not
01:40:43
pay attention she will be on the exam
01:40:46
normal
01:40:48
just Oleg's imperfection
01:40:52
but I'm raising Oleg, I'm constantly raising him
01:40:57
subjecting modifications so to speak
01:41:07
let's all move on
01:41:26
well, by the way, I didn’t fully say that
01:41:29
it will be if at an angle so guys if on
01:41:34
diverging lens beam falls at an angle
01:41:37
that's how then how will he behave
01:41:41
lead look again we are building the side
01:41:44
auxiliary beam parallel to this and
01:41:47
he will behave like this, let’s say
01:41:50
this is where the focus is yes
01:41:53
as if it's coming
01:41:56
from the same point as
01:42:00
this ray, that is, would not be refracted
01:42:03
and it will seem to be coming from a point in
01:42:05
focal plane and will go further
01:42:07
like this
01:42:08
this ray will go like this
01:42:13
this one is better there, I don’t know which one
01:42:15
something goes as if it comes from this
01:42:18
points this beam serving will go like
01:42:22
as if it comes from this, you know
01:42:28
Yes
01:42:30
this is not refracted
01:42:33
it’s clear guys how everything works and also
01:42:36
you can use the reversibility property
01:42:37
if you are pointed in this direction
01:42:40
better who are trying to get them together
01:42:41
focus they will go further in parallel
01:42:43
the same thing if there are rays here
01:42:46
converge on the main optical axis
01:42:49
focus then they will go there parallel all the way
01:42:52
reverse side also works all this
01:42:55
erase
01:43:19
further
01:43:21
The figure shows the progress of a generally point-by-point
01:43:24
light source and through a thin lens
01:43:27
what is the optical power of the lens taste in
01:43:29
diopters rounded to whole numbers
01:43:32
Give 2 in diopters
01:43:40
but we see that our exact source
01:43:44
the ray that goes like this then should
01:43:48
refract focus results in focal
01:43:52
the distance is one two three 4 5 6 6
01:43:59
which corresponds to 6 centimeters
01:44:02
the fact that one cell is 1 cm
01:44:08
she will ask the optical power of the lens
01:44:12
The optical power of a lens is measured in
01:44:14
dioptres and is equal to 1 divided by this is one divided
01:44:17
if transferred to the system
01:44:19
7006
01:44:21
that is, that is the sixth
01:44:25
16, yes if you round to whole numbers then
01:44:29
approximately 17 and
01:44:31
diopter optical power dimension
01:44:55
the pencil is perpendicular
01:44:57
main optical axis thin collecting
01:45:00
lenses at a distance of 50 centimeters from
01:45:03
lenses look here is the distance from
01:45:06
object to the lens with the letter d
01:45:09
indicates the optical power of the lens
01:45:12
deep three
01:45:14
therefore focus 1 by 1 by 5 that is
01:45:21
0 2 meters or 20 centimeters
01:45:26
So
01:45:28
the height of the pencil image is 0 0 6
01:45:33
meters height of the image like this
01:45:36
denoted by 0 0 6 meters what is equal to
01:45:39
the height of the pencil itself, see the question
01:45:44
first let me show you how
01:45:46
build item we have there focus 20
01:45:50
centimeters
01:45:52
here's a double trick and you get an object
01:45:56
is even further than double focus
01:45:59
now we are building two beams one beam
01:46:02
passes through the center of the main optical
01:46:04
the axis is not refracted, that is, let's
01:46:07
I'll draw it green, that is
01:46:11
here he goes like this
01:46:13
the second beam is parallel to the main one
01:46:16
optical axis and it is directed to focus
01:46:20
that is, here he goes like this and here is ours
01:46:24
the image will look like this
01:46:28
that is, it's already
01:46:33
image size is very small
01:46:36
subject
01:46:37
this is the distance from the object to the lens
01:46:41
why do we need the letter d
01:46:43
distance from lens to image
01:46:45
small letter f and for them
01:46:49
thin lens formula 1 is fulfilled
01:46:52
divide by d plus 1 divide by iv also
01:46:55
also similar to this one
01:46:57
triangle and this similar one between
01:47:00
we can conclude that as much
01:47:03
big our little these here
01:47:04
quality are treated the same as
01:47:07
horizontal legs and because angle
01:47:09
here the vertical ones are the same too
01:47:11
how to divide ef by d so what do we have here
01:47:18
d it would be nice to have flown a little
01:47:22
it is equal to 1 divided by f minus 1 divided
01:47:25
on d well and with substitution
01:47:29
1 divided by 20 minus 1 divided by 50
01:47:34
let's count how much we get
01:47:40
guys drawing if this is problem 26 not
01:47:46
look if it doesn't say do it
01:47:48
drawing then drawing is not necessary
01:47:50
that's all
01:47:59
so 100 thirds
01:48:05
it turns out h is equal
01:48:08
hd divided by f
01:48:12
006
01:48:14
50 to 100 and 3 goes up
01:48:23
6 but I promise inside
01:48:27
[music]
01:48:30
009
01:48:33
here is the actual size of the item
01:48:48
yes, this formula is calcification and
01:48:51
no need to withdraw
01:48:56
you just multiplied centimeters by meter
01:49:01
I'll explain
01:49:03
that means I have 103 centimeters here
01:49:07
here is a centimeter and ultimately centimeters
01:49:10
decreased oh there were meters and meters and
01:49:13
stayed so I ran up that I didn't tell you
01:49:17
explained but it doesn’t matter here
01:49:37
So
01:49:38
well everything is clear
01:49:48
our physics teacher told us that
01:49:52
next year justification will have to be
01:49:54
write in each problem in the second part
01:49:56
This is true
01:50:02
can I keep silent
01:50:07
who should I
01:50:11
an attack of rabies sometimes occurs when
01:50:13
I hear the stories of school teachers
01:50:20
this nonsense they talk about
01:50:28
it's good that she says something else
01:50:32
crazier
01:50:35
we will glue you leniently
01:50:42
I can I would where she will soon be able to write
01:50:45
book of myths and legends
01:50:46
physics teachers
01:50:49
school teachers physics teachers
01:50:57
fairy tales and fables
01:51:11
45 years it will be like this and Tamara 8
01:51:15
I said you didn't listen to me, okay cue
01:51:23
so let's move on, thin rod
01:51:26
located perpendicular to the main
01:51:28
optical axis of a thin collecting lens
01:51:31
apparently one end of the rod is on
01:51:34
main optical axis
01:51:38
image of the rod obtained on the screen
01:51:42
with this two and a half lens
01:51:43
times larger than the rod itself
01:51:46
image two and a half times
01:51:48
larger than the focal rod itself
01:51:52
distance 1 centimeter
01:51:56
at what distance is the rod located?
01:51:59
from the lens
01:52:03
everything and
01:52:05
the thin rod is located
01:52:07
perpendicular to the main optical axis
01:52:09
that is, here we have a lens and here is a rod
01:52:12
is perpendicular, that is, that’s it
01:52:14
these points will be located at some
01:52:16
same distance
01:52:18
let's do something else
01:52:28
so we know that as much as h is equal to f by d and
01:52:33
it also turns out to be equal to 2 and 5, that is
01:52:37
f equals 2 and a half d
01:52:39
1 over f equals 1 over d plus 1 divided by f
01:52:44
that is, d 1 divided by f equals 1 divided
01:52:48
by d plus 1 divided by two and a half d
01:52:51
expose it to 2 it to 5 so that with
01:52:55
fractions do not deal one to f is equal to
01:52:58
[music]
01:53:00
7 5 7 years at 5 d
01:53:05
so therefore d
01:53:10
equals 7 fifths f
01:53:16
d equals 14 centimeters
01:53:21
Of course, you need to substitute 705 there first
01:53:25
by one centimeter, but we already get the answer
01:53:33
micrometer why micrometer makar
01:53:42
Hello Marina Yuryevna Demidov
01:53:44
dear, glad to see you
01:53:48
please tell me that there will be 29 problems
01:53:51
optics in 26 quantum
01:53:57
brotherly
01:53:59
purely for those who came in and watched my
01:54:02
six hour stream
01:54:03
we won't tell anyone
01:54:22
collector examine with
01:54:24
magnifying glass element stamp and blows its imaginary
01:54:27
image enlarged by two s
01:54:29
half times
01:54:31
two and a half times from apple
01:54:34
the element in question is located on
01:54:36
at a distance of 4 millimeters from the lamp
01:54:40
4 millimeters at what distance from
01:54:44
the lens contains his image
01:54:49
rf question but with this module
01:54:52
because cook guys when we
01:54:56
we get a virtual image
01:54:59
we place the object closer than the focus
01:55:03
that is, look, let’s say you
01:55:07
look like this but you want something
01:55:10
to make it seem bigger
01:55:16
what to do for this
01:55:20
you need
01:55:22
arrange an object
01:55:25
closer than focal length a
01:55:30
here's to my relatives
01:55:34
the closer you get to the focus I will be
01:55:36
get closer
01:55:39
there will be more subject
01:55:46
after all, I am a man, but I have become, I have increased my
01:55:50
nose
01:55:51
that is, this is an imaginary image
01:55:53
it will be on the same side and
01:55:56
won't be upside down
01:56:04
Here
01:56:09
And
01:56:15
let's show how the object behaves
01:56:17
what about these rays?
01:56:20
they are coming
01:56:23
here at this focus to which it is parallel
01:56:26
and these rays
01:56:29
they are not refracted but it turns out that
01:56:32
these rays intersect, you are this and this
01:56:36
somewhere behind
01:56:37
if the object itself is like that then
01:56:41
the image of the object will appear
01:56:43
enlarged here and the b-stroke will be
01:56:46
so in this case we believe that
01:56:49
if we use a thin lens formula
01:56:52
that f is negative if in general
01:56:56
the image of the object is in the same
01:56:59
half plane where the object itself is then we
01:57:01
we assume that f is less than 0
01:57:12
take the magnifying glass, I called because we'll be here for a long time
01:57:15
Then
01:57:16
I can't stop playing with her
01:57:20
in general, what is the point of this whole fable
01:57:24
as much as dividing ours is equal to f modulo divide
01:57:29
on d equals 2 and a half means f 2 s
01:57:36
half of 4 10 millimeters that's all
01:57:41
what do you need to know here
01:57:56
in millimeters but we had to [ __ ] and
01:57:59
our
01:58:19
so it all erases
01:58:36
so responsible for likes what's there
01:58:39
us happening, by the way, what if the lens
01:58:42
scattering then my RF is less than zero we take
01:58:48
991 likes and I was already afraid of what would happen now
01:58:53
1000 likes and
01:58:55
will have to discharge to charge
01:59:00
no lime yet fortunately
01:59:03
yes yes there just if I get thousands
01:59:06
likes then
01:59:08
I'll have to charge my phone
01:59:11
cars, but fortunately there are still some
01:59:13
There is not
01:59:18
fate saved
01:59:21
maybe we won't get it
01:59:33
Oh damn
01:59:36
why did I say
01:59:44
OK
01:59:47
words must be kept
02:00:10
So
02:00:13
are you ready my young sadists, look here
02:00:17
that's why you see
02:00:20
a spark jumps and you know what I did
02:00:23
I'll turn off the lights
02:00:27
the world is still populated
02:00:35
such as
02:00:44
now I'll try
02:00:46
[music]
02:00:51
for this spark to pass through my fingers
02:01:00
these like this through my finger and this one
02:01:02
piece
02:01:06
creepy
02:01:11
sled through the right hand without anything through
02:01:15
the heart didn't go up to
02:01:19
were he
02:01:22
dressed will fall
02:01:34
phew
02:01:38
Fine
02:01:39
you would have seen the spark, I just didn't expect it
02:01:44
if those I didn't know what to expect
02:01:53
went even better
02:02:01
I've already discharged everything
02:02:08
bet he's dressed
02:02:12
also ask me exactly like this
02:02:15
cut themselves
02:02:20
there were movies it was pain no
02:02:25
there's no point in doing this
02:02:28
charging
02:02:31
ohhhhhhhhhhhhhhhhhhh
02:02:34
that's all I I I asked I cheered up thank you
02:02:38
thank you for the likes guys thank you for that
02:02:41
How about cheering me up?
02:02:57
interesting I don't have through me there on
02:03:01
there's really nothing wrong with it because
02:03:02
that the electricity passed through purely
02:03:05
my finger actually could
02:03:09
when Oleg will be held a little
02:03:11
another experiment I
02:03:15
I'll take Oleg and spread out these balls and
02:03:19
electricity throughout Oleg
02:03:21
passed that is, so that here is one ball
02:03:23
Oleg holds and on the other hand so that he
02:03:26
I held my hand exactly like this
02:03:28
others passed the current and
02:03:30
let's see what happens but for
02:03:32
I need an assistant for this
02:03:36
ok anyway
02:03:38
little by little
02:03:40
the format of webinars and bonita goes into
02:03:43
I don’t remember such a path of trash streams
02:03:47
displacement of streams is prohibited, well, in general
02:03:49
let's see what
02:03:52
will you bring the final subscriber or
02:03:55
goblin has a weaving session there and here he is
02:03:58
in general, it’s super from behind, I can’t
02:04:02
so ok
02:04:05
let's move on
02:04:09
a small item is on the main
02:04:13
optical axis of a thin collecting lens
02:04:15
at double focal length from it
02:04:17
how it changes when an object approaches
02:04:21
to the focal length of the lens are the following
02:04:23
three sizes
02:04:24
image size of its distance from
02:04:27
lenses optical power
02:04:30
it is in dual focus
02:04:32
distance
02:04:36
look here's what's interesting and especially
02:04:40
double focal length
02:04:45
so that's what's interesting double crooked
02:04:49
on and yours
02:04:52
so in general I erase everything
02:04:58
little sadists
02:05:02
what's interesting about dual focal length
02:05:04
look at the distance, you have focus
02:05:06
here we have
02:05:09
double focus
02:05:12
when the subject is in double focus
02:05:15
look here the beam is coming
02:05:19
Then
02:05:21
So
02:05:23
So
02:05:26
the ray is refracted by focus and
02:05:31
here the second ray goes like this and
02:05:37
it turns out that they intersect
02:05:40
tyutelka tyutelka right here that is
02:05:43
the item we will have is the same
02:05:45
size in double foxy h is equal to ours if
02:05:50
d is equal to 2 and well, according to the thin lens formula
02:05:56
if you and I sign
02:06:00
one divisor by f in minus 1 palace y
02:06:04
we get the image
02:06:07
be also in double focus
02:06:11
So
02:06:13
Well, it turns out that the object is enlarged
02:06:18
it won't happen what will happen
02:06:21
if we start
02:06:24
bring an object closer to the focal point
02:06:27
distances by persons
02:06:30
look
02:06:33
what's happening
02:06:36
let me draw it red when
02:06:40
I brought it closer, what will change is this one
02:06:44
this is how the line went, this is how it goes, that is, it
02:06:47
will not change, but this ray
02:06:52
it will fall at a large angle and
02:06:56
the item will be deleted
02:06:59
you see, that is, we will have
02:07:01
increase in size
02:07:04
us according to the formula only lenses if you
02:07:08
paint
02:07:10
as d decreases, f increases since
02:07:14
on the left there should also be something the same
02:07:15
that is, for reducing the EFR then
02:07:18
grows and if f grows then it is equal to
02:07:23
y divided by d when decreasing yes it is
02:07:26
growing means the image will also be
02:07:28
it's better to grow up like this
02:07:32
remember and work on this
02:07:34
similar tasks means size
02:07:36
the images will become larger and larger
02:07:39
distance from image to lens
02:07:42
will increase
02:07:44
optical power of the lens but naturally it
02:07:46
will not change
02:07:48
because it only depends on focus
02:07:52
then the answer is 113
02:07:55
that's it friends
02:07:59
[applause]
02:08:21
stream starts at 12 if that's the case
02:08:28
so guys, and here the door open your soul
02:08:30
such a hut
02:08:34
a little bit of air on the shoulder and today
02:08:38
there's still no one at all
02:09:07
spiral light bulb located located
02:09:10
near the main optical axis of the thin
02:09:12
diverging lens with focal
02:09:14
distance equal in modules to
02:09:16
perpendicular to this axis the distance from
02:09:18
lenses to spiral less than 2 f but more than f
02:09:22
let's draw
02:09:24
so less 2f more
02:09:30
Well, here are the spirals of a light bulb on with a light bulb
02:09:33
here comes the spiral
02:09:41
scattering let's build
02:09:43
give me the image and put it in a little bit
02:09:46
let there be a light bulb like this
02:09:49
it turns out that the object itself is a.b.
02:09:53
one ray comes here and is not refracted
02:09:57
the other one comes here and
02:09:59
as if it comes from this focus then
02:10:03
it will seem to us that this is it
02:10:05
the light bulb is here
02:10:08
this is where image 1 will be located
02:10:12
b1 is her image
02:10:15
that's how it turns out
02:10:18
we need it when the lens is diverging in
02:10:22
point b it turns out this
02:10:24
image but what kind of direct image will it be?
02:10:27
there you see where it's pointing there
02:10:29
looks and it's straight
02:10:31
me my
02:10:33
virtual image
02:10:35
it is when
02:10:38
in the same picture
02:10:42
in the same
02:10:45
semi plane
02:10:49
same thing
02:10:52
when in another half-plane it means
02:10:56
indeed we depict him
02:10:58
we can project it somewhere when I need to
02:11:00
mothers simply deliberately complete how
02:11:02
like it's there
02:11:05
wow this means an imaginary image
02:11:08
direct imaginary and reduced what is the size of
02:11:12
there will be less of it and it will be better
02:11:15
diverging lens it always gives
02:11:17
direct in it reduced how would you be there
02:11:20
what they didn’t twist will always be wrong
02:11:23
always inverted image
02:11:25
reduced and always that's all in short
02:11:27
such
02:11:30
direct
02:11:33
reduced third answer option yes but
02:11:37
if we replace this thing with a collecting one
02:11:40
lens
02:11:45
we will replace
02:11:48
let's just see what it will be like for us
02:11:52
image
02:11:55
Means
02:11:58
it goes like this
02:12:01
it goes like this
02:12:04
the image will become
02:12:06
enlarged
02:12:08
inverted and
02:12:12
really and
02:12:22
really inverted magnified
02:12:25
one
02:12:28
By the way, let's pay attention
02:12:31
what if we
02:12:34
in 2 auto the image is the same, what if
02:12:38
further than 2f
02:12:42
us image will be reduced
02:12:51
such a tan and reduced size
02:12:56
inverted
02:12:58
really, let's do it this way
02:13:01
booze let's show what the image will be like
02:13:05
converging lens if
02:13:08
the object is closer than the focus, well here it is
02:13:11
I've already built this but I want to do it again
02:13:13
show so everything is in one place
02:13:15
look this one goes like this
02:13:21
then focus and
02:13:24
this one is not refracted in the end they
02:13:27
intersect here, it seems to us that
02:13:30
item
02:13:33
increased
02:13:34
straight
02:13:36
imaginary
02:13:39
so this is Abe
02:13:41
this stroke stroke
02:13:46
that is, a collecting lens can give
02:13:49
three types image enlarged
02:13:51
inverted indeed and when about
02:13:53
between focus and double focus
02:13:57
enlarged inverted indeed and
02:14:00
when more than double foresails are reduced
02:14:02
inverted 10 when more than double
02:14:05
foxy and
02:14:06
magnified direct imaginary when an object
02:14:10
are closer to focus
02:14:13
draw f
02:14:16
here they are
02:14:24
this problem has been navi for two years by the way
02:14:27
back
02:14:33
let's move on
02:14:37
to complex geometric optics
02:14:41
there will be a break because he is me
02:14:44
I feel like I still need him
02:14:46
coming soon
02:14:47
now let's finish the optics and
02:14:50
I'll take a break for a second
02:14:56
5 minutes
02:15:20
6 o'clock according to errors it seems to me
02:15:23
there it is necessary to arrange a 30-hour
02:15:26
at least because the error is six
02:15:28
you won't pass the clock
02:15:33
if the subject is in focus no longer
02:15:36
images before so there is there it turns out
02:15:40
what are you looking at
02:15:43
1 divide by i
02:15:46
plus 1 divided by f if you stream d
02:15:51
to focus left
02:15:55
you can do it
02:16:00
that one on f minus May 19 with a minus
02:16:06
this is a very small difference
02:16:10
and it is positive
02:16:13
they she is negative it turns out f minus
02:16:17
minus f long
02:16:22
that is, f minus is slightly less than
02:16:25
focus that is, it follows that f
02:16:27
tend to minus infinity
02:16:34
this is what will happen to you
02:16:36
if you have fk plus a little more than
02:16:39
focus yes then your f tends to plus
02:16:43
infinity
02:16:48
well, in fact, you focus the subject
02:16:52
you won't be able to focus on the screen
02:16:53
because the image is on the screen
02:16:56
deliver very far
02:17:01
so okay let's
02:17:25
stronger physics in the profile to sleep too
02:17:32
that would be cool
02:17:34
but not this year his life
02:17:37
the ball is suspended on a thread and makes
02:17:41
oscillations at the extreme points a and b lie on
02:17:43
optical axis of the collecting lens projection
02:17:46
the ball's equilibrium point is at
02:17:48
distance root of 5 from the first focus
02:17:51
lens distance from it to the extreme points
02:17:54
equals 1 centimeter between images
02:17:57
explain the extreme points of the converging lens
02:18:00
distance between the extreme images
02:18:02
points equals 2 centimeters find
02:18:05
lens optical power
02:18:23
so I have a suspicion that
02:18:28
so let's
02:18:42
here we have
02:18:46
icon like this
02:18:50
this is f
02:18:53
this turns out to be f + root of 5 but
02:18:58
I mean this is the distance at
02:19:01
this and the taste of the root of 5 is obtained here
02:19:04
this is the distance f + root of 5
02:19:13
so this minus 1 centimeter
02:19:23
this is the distance
02:19:26
f + root of 5 + 1
02:19:31
Well, it turns out that let’s give this point
02:19:35
let's call them already named b.a.
02:19:40
then it turns out 1 divided by the top exactly
02:19:44
one divide plus 1 divide by and that is f
02:19:49
b equals 1 divisive f minus one
02:19:52
divisor by db
02:19:55
such of I was given a
02:19:58
turnouts and recently
02:20:00
but I won't look
02:20:07
ok
02:20:14
distance between images
02:20:17
let's think if we have
02:20:20
the object is further away then it
02:20:22
the image is closer, that is
02:20:25
the b-stroke image will be here
02:20:28
image stroke will be here
02:20:30
therefore fb stroke is less than f a stroke
02:20:36
fb for less than something
02:20:40
but there it will naturally be upside down
02:20:45
it turns out
02:20:50
we are given that the distance between
02:20:53
images two centimeters that is f a
02:20:55
minus fb 2 centimeters they still need
02:21:01
here it turns out f is 11 9 plus 1
02:21:05
divide by d that is 1 divided by 10 c
02:21:10
minus 1 divided by f
02:21:14
+ root of 5 minus 1 minus
02:21:19
11 visible iv minus
02:21:23
plus root of 5 plus 1 equals 2
02:21:29
but actually it’s just linear
02:21:31
the equation is essentially
02:21:34
[ __ ] me of course
02:21:51
so and
02:22:00
plus root of 5
02:22:03
boss
02:22:09
this led to a common denominator
02:22:12
denominator
02:22:15
minus
02:22:17
f by i plus root of causes plus one
02:22:23
root of 5
02:22:25
minus f
02:22:31
equals 2
02:22:42
so this is the root of 5 minus 1 so that
02:22:46
get rid of well lead to the general
02:22:47
denominator
02:22:48
bottom 5 plus 1 sorry
02:22:54
graduate they fit on top of each other
02:22:57
So
02:23:00
what comes out
02:23:04
squared
02:23:08
plus f to the root of 5 minus 1
02:23:13
to the root of 5
02:23:16
plus 1
02:23:18
minus f squared plus f to the root of 5 +
02:23:25
1
02:23:27
5 min root from India
02:23:37
So
02:23:41
root is pretty plus 1 by and squared
02:23:46
plus
02:23:48
f
02:23:51
5 minus 1 4 by 4 minus f squared by
02:23:57
root of 5 minus 1 minus
02:24:01
4 divide
02:24:03
by 4
02:24:07
12
02:24:09
so it's shrinking
02:24:15
[music]
02:24:19
it turns out
02:24:21
root of 5 root of 5 is reduced
02:24:26
f + is two and squared is equal to
02:24:32
8f squared by 4 f equals 2 centimeters
02:24:54
[music]
02:25:01
1 2 equals
02:25:04
why are 1 2 not one side all
02:25:08
right
02:25:19
what vitamins would I recommend taking haze
02:25:25
I didn't turn over the fractions
02:25:32
can't digest anything here with me
02:25:35
so I just set it up and here I led to
02:25:40
in general, yes, I’ll tell you in more detail one
02:25:43
here f + root of 5 minus 1 minus f
02:25:49
divide by RF by turnout with root of 5 minus
02:25:53
1
02:25:56
if 1 is divided by this fraction then it’s simple
02:26:00
turns over that's all so that's all
02:26:02
right it's not 1 2 equals
02:26:04
why are a1 and b1 located the way they are?
02:26:08
on the contrary because
02:26:10
according to the formula thin lenses with removal
02:26:14
subject
02:26:16
the image is zooming in so that's all
02:26:19
equaled a constant value, this is 29
02:26:22
number in game
02:26:25
through magnification
02:26:30
probably possible, but I don’t even know why
02:26:39
why do you need this increase
02:26:46
by the way, find those optical powers
02:26:49
let's tempted
02:26:52
1 divided by f
02:26:55
1 divided by zero zero
02:26:59
250 diol 3
02:27:13
tags
02:27:28
go ahead
02:27:33
and you need it when you have its formula on a piece of paper
02:27:35
write substitute or you can immediately in
02:27:37
braid the answer look at the rules
02:27:40
registration
02:27:42
when do you substitute
02:27:44
I should definitely put it here
02:27:48
just instead of a letter, I imagined it in
02:27:50
the end already
02:27:52
[music]
02:27:54
yeah, well, when you set it up, it’s already possible
02:27:58
enter the calculation into the calculator
02:28:05
I erase all this
02:29:21
I
02:29:23
I want to see how many people I need and
02:29:26
Why are there so few new subscribers?
02:29:31
in the cart
02:29:34
get at least 5 thousand
02:29:56
where is the electric shock and I've already had the electric shock
02:30:01
the peace has already dissipated
02:30:03
grandpa drink he can't see well up close because of
02:30:06
farsightedness for reading books on
02:30:08
best vision distance 25
02:30:11
centimeters and
02:30:15
I have to use my glasses by force
02:30:18
2 and a half diopters
02:30:25
if the object is located closer than 25
02:30:28
centimeters for example at a distance of 15
02:30:30
centimeters
02:30:36
what glasses with what optical power
02:30:39
grandfathers will have to wear
02:30:43
look at grandpa's eye
02:30:49
Grandfather's eyes have some kind of optical
02:30:52
the power of the lens is what the eye essentially is
02:30:54
also a lens that focuses
02:30:56
image on the retina and to
02:31:00
he wouldn't have to feel comfortable
02:31:02
strain like this like this like this
02:31:05
to strain his eyes he uses glasses
02:31:08
let's draw one such point
02:31:12
it turns out because the optical power
02:31:14
positively this is a point-collector and
02:31:17
it turns out d1
02:31:20
plus d2 for
02:31:24
equal to
02:31:26
1 divided by
02:31:28
d1 plus 1 divided by f and the retina
02:31:33
is always on the same
02:31:35
distance you can't move
02:31:37
the retina of the eye is so ok fat if
02:31:40
struck great and flattened my eye no
02:31:43
that doesn't happen in general distance
02:31:45
always between the pupil and retina
02:31:47
is the same, so his f does not change
02:31:50
and now he put on another [ __ ] and
02:31:55
moved closer
02:31:58
the object to find d2 must be subtracted from
02:32:02
lower 2 and then immediately both dg and retina
02:32:05
will go away that is b 2 minus 1 is
02:32:10
1 by 2 minus 1, etc.
02:32:15
it turns out d2 equals d1 plus 12 minus 1
02:32:22
Where
02:32:23
let's substitute 2 and a half diopters
02:32:26
1 means d2 is necessary
02:32:30
damn let's change the variable
02:32:35
d1 d2
02:32:38
then I'll get confused
02:32:41
that's how it turns out
02:32:46
one on one
02:32:48
d20 15 so that everything is exactly on
02:32:52
-1 divided by 0 25 here
02:33:04
2 and 5
02:33:06
plus 1 divided by 0 15
02:33:12
minus 1 divided by zero 25
02:33:18
this is the optical power
02:33:22
didn't work out 5,
02:33:25
[music]
02:33:26
6 and 7 167 diopters
02:33:35
[applause]
02:33:46
so everyone understands guys
02:33:50
back to the cart nuka nuka let's see
02:33:57
again thousands of subscribers
02:34:00
e-e-e
02:34:06
Thank you
02:34:20
Sanya, you have a boost, what do you think about this?
02:34:22
topics
02:34:24
I'm specially holding 2 this year
02:34:27
six o'clock so that you have
02:34:29
6 hours to inspect the tasks and
02:34:32
6 hours to do yes homework
02:34:35
the task is why I have 2 6 hour strips
02:34:54
if the diverging lens were
02:34:58
the optical power would be less than zero with
02:35:06
using the lens on the screen we got a clear
02:35:09
image of a candle flame having
02:35:11
height
02:35:14
15 centimeters
02:35:16
moved the candle away from the lens
02:35:20
one and a half centimeters
02:35:23
one and a half centimeters and
02:35:28
moving the screen got a clear
02:35:30
image of candle flames still having
02:35:32
height 10 cm
02:35:37
find the height of the candles if focal
02:35:40
lens distance 18 meters
02:35:45
candle height
02:35:53
That
02:35:58
it was necessary here
02:36:05
so well
02:36:07
what
02:36:13
here we had some kind of image
02:36:15
such
02:36:17
as much as this
02:36:22
d is f
02:36:26
it turns out
02:36:40
h but these are so Pasha that is a cage
02:36:45
small just like the Russian Federation refers to d
02:36:53
in this case we have
02:36:57
h1 is related to the same as f1
02:37:02
gd
02:37:05
h2 is to small the same as f2
02:37:09
g.b.
02:37:11
we moved away
02:37:16
pushed back to
02:37:25
nights tf decreased
02:37:43
so I have a fight
02:38:08
I can find it twice
02:38:11
why do I need h1 then
02:38:14
I may be misunderstanding the condition
02:38:21
moving the candle away from the lens
02:38:24
distance
02:38:34
this damn wording is oblique and incomprehensible
02:38:38
distance from candle to lens
02:38:43
or moved at a distance
02:38:47
another one and a half centimeters
02:38:50
that this probably changes the conditions
02:38:55
it was implied if as I understand it
02:38:58
initially we don’t need h1 but
02:39:01
if so
02:39:03
moved another centimeter and a half
02:39:06
then you need then here d plus b
02:39:17
then it will be useful ok
02:39:26
so therefore d.m.
02:39:39
For what
02:39:40
ff1 won't be useful
02:39:43
where will I need it
02:39:55
what nonsense to do then
02:40:09
aif is 11 liters plus 1 divided by 2
02:40:33
do a little
02:40:43
let's improve fate, let's express it
02:40:55
And
02:40:56
let's substitute here
02:41:00
but this
02:41:03
ff by f minus and
02:41:08
that is, h1 by h is equal to
02:41:13
ff1 to f1 minus f
02:41:20
oh and there after
02:41:23
f1
02:41:26
ff1
02:41:31
f1 minus f
02:41:34
here
02:41:42
f2
02:41:50
but its minus f
02:41:53
but ff2
02:41:58
So
02:42:03
it is not known h1 h2 it is known to impose and
02:42:10
right here d + f so let's do it then
02:42:16
So
02:42:29
I'm stupid
02:42:37
this is bjj b
02:42:42
no cheat
02:43:04
so I do this
02:43:06
confused
02:43:09
damn I'm confused
02:43:14
variables
02:43:31
what do I have I don't have even a small one
02:43:35
this is bad
02:44:05
it's 6 now
02:44:09
for autumn
02:44:10
Well, in general, in such cases you can simply
02:44:15
create a system of equations if not
02:44:19
it turns out in general terms to solve immediately
02:44:21
you can just write down all the equations
02:44:24
which you have and substitute the numbers and
02:44:27
then think about how there is something through them
02:44:29
let's express it this way in this case
02:44:31
let's do that, that is, we know that there is h1
02:44:35
on h is equal to f1 on d and it is also known that
02:44:41
one by f equals
02:44:43
10 plus 1 on d
02:44:46
on f1 we also know that there are as many as two on
02:44:52
ashik equals f2 on
02:44:55
di1 9 phrases but one of 2 plus 1 divided by
02:45:00
b plus b and
02:45:03
that's when in general terms sometimes
02:45:06
somehow you understand somehow
02:45:09
you don't get it sometimes how to set it up
02:45:13
how to express it so purely if
02:45:15
see how many unknowns we have
02:45:17
here we have as many unknowns here
02:45:20
small
02:45:22
f1 f2 and d we have four unknowns and 4
02:45:28
equations, that is, it is absolutely possible
02:45:31
mindlessly express from one equation and
02:45:34
substitute in the rest, well, actually
02:45:37
why not do that
02:45:39
Here
02:45:41
so here d + business
02:45:47
maybe, let's say
02:45:50
slowly get rid of excess
02:45:52
variables as much as, for example, equal to h1 d divide
02:45:57
on f1 and we will have three equations below
02:46:01
already with three unknowns one on f
02:46:04
1 and f 1 plus 1 when
02:46:08
h, by the way, this variable is us like
02:46:12
times asked to find
02:46:16
maybe I can express something else here?
02:46:25
So
02:46:29
we are asked about the task your question is how
02:46:33
once find the height of the candle
02:46:37
maybe the numbers just suck and that’s it
02:46:41
give us numbers and a bath and so on for a long time
02:46:45
I'll sit
02:46:46
15 divide our equals f 1 divide by d here
02:46:53
a bunch of generally unknown people in one
02:46:54
equation 3 unknown
02:47:01
ok here
02:47:04
118 equals one myth 1 plus 1 divided by d
02:47:08
here 10 to h is equal to v2
02:47:15
on d plus one and a half
02:47:18
1 divided by 18 is equal to 1 divided by and in 2
02:47:22
plus 1 divided by d plus one and a half
02:47:28
So
02:47:33
f1
02:47:34
[music]
02:47:41
so look, f1 definitely pisses us off
02:47:44
participates like this, I wrote it down and I felt
02:47:46
it's easier to think that is, let's get rid of
02:47:48
from f1 and f2
02:47:51
f1 is 15d divided by h and
02:47:58
substitute in the second we will have two
02:48:00
already equation 1 divided by 15 d h plus 1
02:48:07
divide by yes
02:48:09
here we express f2
02:48:12
that's 10d + one and a half
02:48:16
divide by
02:48:18
h1 18
02:48:21
1 divide by 10d + 15 by h plus 1 divide
02:48:28
on d plus one and a half
02:48:31
well great, there are two left
02:48:33
equations this is this and this is now
02:48:36
Well, ideally express from here let's
02:48:39
from this we can express d
02:48:42
well, if you take it out of brackets 1 1 18
02:48:47
equals 1 divided by d
02:48:50
h 15 plus 1
02:48:54
that is one
02:48:56
18 equals h plus 15 divided by 15 d means
02:49:03
m
02:49:07
18 h plus 15
02:49:10
divide everything by 15 and substitute it into this
02:49:14
the equation we will have is one unknown
02:49:17
so 1 18
02:49:21
h divide by
02:49:27
180 h plus 15
02:49:30
divide by 15 plus 15
02:49:35
plus 1 divided by
02:49:38
18 h
02:49:48
plus 15
02:49:52
9 by 15 plus one and a half, that's all
02:49:57
in fact, we now have one
02:49:58
variable
02:50:02
long ago now one variable
02:50:09
That
02:50:23
what can we do here
02:50:30
[music]
02:50:42
let's convert
02:50:57
1 18
02:51:00
h divide by
02:51:10
By the way, this is ten times different
02:51:12
Let's
02:51:20
for real 10 times, that is, here 10 here
02:51:25
that is, I can just multiply by 10
02:51:28
I will have a numerator and denominator
02:51:30
the denominator is the same
02:51:32
10 turns out to be 108 experience + 15 + 15
02:51:37
great it turns out h plus 10 here in
02:51:42
denominator and
02:51:43
here and there 180 h + 15 +
02:51:50
15 squared and this is 15 below
02:51:55
go up
02:51:57
Here you go
02:52:03
it turns out
02:52:04
180
02:52:12
the participant can, in principle, be reduced
02:52:15
by 3
02:52:24
I don’t want to do it like that, ok then
02:52:28
180 h plus 180 by 15 plus 15 square then
02:52:38
cross equal
02:52:40
1518 by h plus 10
02:52:47
it turns out
02:52:50
[music]
02:52:55
h15 by 18 minus
02:52:59
180 equals 180 times 15 plus 15 squared
02:53:05
minus 15 18 by 10 well that's it
02:53:11
calculator case
02:53:22
So
02:53:25
table 8
02:53:28
15
02:53:29
plus 15 square
02:53:33
Cute
02:53:35
minus 15
02:53:38
until 18 10
02:53:46
15
02:53:49
minus 180
02:53:52
and a half
02:54:00
centimeter by can be added
02:54:10
Well, maybe it could be easier somehow
02:54:13
maybe I should have found it first
02:54:15
some other variable then it would be
02:54:17
it was easier to do I don't know the guys in
02:54:20
in general
02:54:22
I did this and it seems like some of you
02:54:26
there was also such an answer
02:54:36
even Arthur
02:54:40
it was necessary to separate it was necessary to search from thin
02:54:44
lenses
02:54:53
[music]
02:54:56
but they made it shorter
02:55:02
I still don’t get it, it went there
02:55:27
Guys, help for my calculator
02:55:30
there is a video on my channel this year
02:55:34
came out where is the new one eat link to the new one
02:55:37
you can find a help calculator for the game here
02:55:41
find it and download and print this
02:55:44
demand
02:56:09
isosceles right triangle
02:56:11
a b c with an area of ​​50 square centimeters
02:56:17
50 centimeters square
02:56:20
located in front of a thin converging lens
02:56:23
so its side c lies on the main
02:56:25
optical axis of the lens focal length
02:56:28
50 centimeter lenses
02:56:33
the vertices of the right angle c lies further
02:56:36
the center of the lens is less than the vertex of an acute angle a
02:56:39
distance from the center of the lens to point a
02:56:41
equal to twice the focal length
02:56:44
lenses
02:56:46
da2 and that is that centimeters
02:56:52
[music]
02:56:55
construct an image of a triangle and
02:56:57
find the area of ​​the resulting figure
02:57:03
isosceles
02:57:04
isosceles triangle
02:57:11
So
02:57:14
tekz
02:57:18
well, it's isosceles
02:57:20
they don't honor
02:57:22
b here b it's double focus it's simple
02:57:28
focus
02:57:29
this means this one is better than the one she has here
02:57:33
the hypotenuse goes like this
02:57:46
df
02:57:49
maybe draw it like this in parallel
02:57:53
means the focal plane is like this
02:57:55
will intersect
02:57:59
this is how this case will go later
02:58:04
to find it let's show the red ones
02:58:08
top point
02:58:10
to find this we will build like this
02:58:13
additional constructions
02:58:16
that is, here we have. b-stroke and to buy a
02:58:23
. A
02:58:28
will be located here too on
02:58:31
the main optical axis and the stroke and here is our
02:58:35
triangle
02:58:38
Well, I actually built it
02:58:47
further
02:58:51
one on f equals 11 plus 1 on
02:58:57
f&f point n
02:59:00
11 to f minus 10 to
02:59:04
10 to minus 1 to 2 and
02:59:08
it turns out also 2nd in short
02:59:12
in general, this one. is also in
02:59:15
dual focus which is not surprising
02:59:21
now where is point b on what
02:59:24
distance
02:59:26
d b
02:59:28
equals
02:59:29
2f plus b since the area of ​​this
02:59:35
triangle 1 2 b squared
02:59:37
therefore b is the root of 2 c
02:59:43
that is, it would be the root of 2 by 50 that is
02:59:48
10 centimeters
02:59:52
that is, it turns out
02:59:56
102 to 50
02:59:59
plus 10 110 centimeters a
03:00:05
at point b
03:00:08
150
03:00:10
-1 on
03:00:11
[music]
03:00:13
110 we started to write down in general terms
03:00:16
naturally
03:00:17
at point b
03:00:19
1
03:00:24
we can do the math
03:00:40
crooked answer is enough here
03:00:43
75 third
03:00:46
centimeter
03:00:50
that's how I believe now
03:01:03
there was an area
03:01:07
I was like, okay, that’s probably all
03:01:10
that's right, that is, this is the distance
03:01:14
this is fb
03:01:19
it turns out that this one is rolling, let's go
03:01:22
I’ll denote this one by x and this one by y
03:01:26
here it rolls x is 2 and minus
03:01:31
fb
03:01:33
that is, this
03:01:37
102 is written to represent minus
03:01:41
275 third
03:01:47
different 25 thirds
03:01:50
centimeters
03:01:53
height y refers to b
03:01:58
just like but this is what I mean
03:02:01
little porridge you can't see it
03:02:09
also applies to
03:02:15
fbk d.b.
03:02:20
therefore y is equal to b fb by d b b
03:02:27
we have 10 fb
03:02:32
275 third and
03:02:34
db
03:02:38
110
03:02:42
we think
03:02:47
There is
03:02:50
more
03:02:52
divide by 3 divide by 110
03:02:58
8
03:03:00
too 23
03:03:03
Amazing
03:03:06
means area
03:03:09
Images
03:03:11
12
03:03:14
x y
03:03:17
1 2 25 thirds
03:03:21
at 25 thirds
03:03:32
approximately equal to 34 72 centimeters square
03:03:38
It is necessary to indicate the size
03:03:46
I area is not the same because
03:03:51
he's closer to us now ugh double focus
03:03:54
the area will become smaller
03:04:01
guys, this is a very big task
03:04:03
may be on the exam
03:04:05
please pay attention to it
03:04:38
the expert will not punish if the calculations are not all
03:04:41
no problem, the main thing is just yourself
03:04:44
keep an eye on the dimensions during the process
03:04:46
solutions
03:04:50
all the news
03:05:22
guys again for efficiency
03:05:24
of this six-hour stream was
03:05:26
you definitely need to decide about the maximum
03:05:29
tasks from last year's 6 hour
03:05:31
stream, that is, I have last year's
03:05:33
same stream, similar tasks there
03:05:37
only with others clean, that's a must
03:05:39
you decide about it
03:05:42
point for constructions before in general if in
03:05:44
the assignment has the wording to build
03:05:46
the image you built will be delivered to you
03:05:49
ball
03:05:51
The telescope has a lens with a focal length
03:05:53
1 meter distance
03:05:58
1 meter f1 thread and
03:06:03
eyepiece with focal length 5
03:06:05
centimeters
03:06:08
centimeters if you remove the screen from
03:06:12
eyepiece
03:06:13
up to a distance of one and a half meters
03:06:21
screen
03:06:25
fragrant not one and a half minutes of luck and it's like
03:06:28
f2 I'll write down
03:06:30
one and a half meters
03:06:33
then you can get an image of the sun
03:06:37
diameter 25 centimeters
03:06:44
25 centimeters
03:06:47
find the angular diameter of the sun from these
03:06:52
minutes round to the nearest whole number
03:06:55
just darning
03:06:59
children
03:07:02
angular diameter of the sun at what angle
03:07:07
falls
03:07:09
not very much and at what angle sometimes
03:07:12
cherry
03:07:13
look here you look at the sun
03:07:17
our sun is not like that
03:07:21
just imagine that the center is the main one
03:07:24
optical axis faces the bottom
03:07:26
sun
03:07:28
this
03:07:32
and here are the rays falling from some point
03:07:36
they are in the sun but essentially everything is under one
03:07:39
now let me draw it here
03:07:42
you have
03:07:45
this lens
03:07:51
and imagine that we are just from
03:07:53
the highest point to teach the rays we send here
03:07:55
only from the top create its key
03:07:57
falls like this
03:08:01
like this
03:08:05
so here it is
03:08:12
Of course we'll lose a lot of time then
03:08:15
it will be more clear for here and
03:08:25
what it seems
03:08:27
lens on a small scale if you
03:08:31
here to consider for the lens
03:08:33
it turns out the top
03:08:36
thing in the sun
03:08:38
falls under parallel rays to whom these
03:08:41
rays on a large format they seem
03:08:43
dad, in parallel, everyone will fall on the lens
03:08:46
it will feel like
03:08:49
parallel rays fall and they will
03:08:51
focus the focal plane too
03:08:53
indeed, if according to the thin formula
03:08:55
lenses at
03:08:56
us d tends to infinity
03:09:00
then where is the distance
03:09:03
the image comes into focus
03:09:06
that is, what does this all lead to?
03:09:10
this ray doesn’t help you like that
03:09:13
refracted
03:09:14
Let's say this is where the focus is and
03:09:18
you will be focused here
03:09:21
image of the sun
03:09:22
first image layer understand
03:09:25
let's have it with us
03:09:29
there I don’t know what size we might need
03:09:32
and don't need it, let it be, let's give it
03:09:34
letter
03:09:36
b I'll call this the height will be b and
03:09:42
it turns out this is the angle you know
03:09:46
all angles
03:09:47
the angle at which the sun falls is and
03:09:50
is the angular diameter of the sun, that is, us
03:09:53
they ask you to find this very corner
03:09:58
and this angle is alpha
03:10:00
this one is rolling with
03:10:07
so this is tangent alpha tangent alpha
03:10:11
equals b divided by f everyone understands guys
03:10:15
that is, here we focused this
03:10:18
a little sun but so that this sun
03:10:22
then project it onto the screen we have
03:10:24
another lens and
03:10:26
here we are looking at this sun, well here
03:10:32
I don't know us anymore
03:10:35
the focus is different, of course, let it be f2
03:10:39
is here and
03:10:40
that's what we have in common
03:10:44
22
03:10:47
than it falls like that and
03:10:50
it falls like this
03:10:53
here we get a zoom
03:10:56
image of the sun
03:11:01
some bigger and
03:11:05
already the size of a large one
03:11:09
as big and in this case it turns out as much
03:11:14
divide by b is equal
03:11:24
f2
03:11:27
divide
03:11:29
f2 this is this distance
03:11:31
divide by
03:11:33
this is it, this is it now
03:11:35
the distance is where we are now
03:11:43
let's look at the conditions again
03:11:46
telescope has
03:11:48
focal length lens
03:11:51
1 meter distance and
03:11:56
eyepiece with focal length 5
03:11:58
centimeters
03:12:00
if you remove the screen
03:12:04
from the eyepiece
03:12:28
I'm missing something
03:12:52
maybe it's not necessary
03:12:59
f2 is
03:13:04
let it just let's ask
03:13:06
indicated by this distance d and
03:13:11
1 divide by f2
03:13:14
1 divided by d
03:13:17
plus 1 divided by f2
03:13:21
so now from here I can express b and
03:13:24
it is equal to f tangent alpha
03:13:27
I put it here and
03:13:30
from here I can express yes well everything everything
03:13:35
great 1 divided by f minus 1 personally
03:13:39
at 2
03:13:40
well, let's just count d small
03:13:44
one divisor by
03:13:47
f2 it turns out this
03:13:51
005 -1 divided by one and a half
03:13:57
let's calculate how much it will be
03:14:03
1
03:14:06
1 divided by 0 05 mm
03:14:12
long point laugh
03:14:23
so this is our distance and
03:14:27
now we have everything ready to set up
03:14:30
here this is this I put here and here
03:14:35
they're looking for so much space I haven't used it yet
03:14:38
to divide so the dashboard asks me to divide
03:14:42
on f tangent alpha
03:14:45
equals f 2 divided by d
03:14:49
that is, alpha is equal to the arctangent
03:14:54
at
03:14:59
d
03:15:02
ff2
03:15:03
well, let's substitute the numbers of arc
03:15:08
tangent
03:15:11
025
03:15:14
d0 0517
03:15:20
pff what do I have here here I have f1
03:15:24
I'm sorry I forgot to sign
03:15:29
pcs f-1
03:15:32
f1
03:15:34
1 on f2 one and a half
03:15:38
so let's see
03:15:48
the tangent will be
03:15:51
25
03:15:55
17
03:15:57
by one and a half
03:16:04
049
03:16:07
0 494 let's give the degree of this angle
03:16:12
sun we can get help
03:16:15
telescope
03:16:17
generally through a telescope into the sun through
03:16:21
It's better not to look at the telescope because
03:16:25
number of views in this case
03:16:27
will be limited to twice left and right
03:16:30
there will be nothing further to look at with the eye
03:16:36
we're keeping everything on schedule grandpa
03:16:39
in general, even close to the course of the webinar on 7
03:16:42
hours
03:16:46
So
03:16:55
there he asks for minutes
03:17:00
give the answer in a minute but really
03:17:03
these were the formulations before
03:17:05
now you can do whatever you want, but if in
03:17:07
minutes is 60 times more
03:17:11
that is
03:17:13
alpha let's do it the same
03:17:17
29 shot down 6 minutes
03:17:32
guys now I'll take this for a second
03:17:38
give me 5 seconds I'll be back
03:17:43
I'll even turn off the sound because we haven't yet
03:17:46
so close
03:19:10
I'm just going back dear
03:19:17
Here
03:19:22
high
03:19:28
because of you I want to take physics at least in
03:19:30
incomplete yes it doesn’t give a [ __ ] at all 0 not 0 no
03:19:34
if you work with me you
03:19:36
you will reach the peaks get there dear how
03:19:38
mountains
03:19:40
you will know yoga higher than the mountains
03:19:46
tax planning moving forward
03:19:58
And such a cool puzzle about a telescope
03:20:02
interesting
03:20:45
shocked until
03:20:51
How many
03:20:55
I
03:21:06
gentleman 7 problems on a diffraction grating and
03:21:09
how does 5 manage
03:21:12
let's get the frame
03:21:26
counter for ba ba shu
03:21:30
drink willingly
03:21:33
I only like tea
03:21:43
one second brothers
03:21:53
the years take their toll
03:21:56
I can't prophesy
03:22:14
I can't get coffee right down the line
03:22:17
stands on a diffraction grating
03:22:20
I won’t surround you in diffraction now
03:22:24
in detail
03:22:25
tell me something about how it is in general
03:22:28
some two sources which
03:22:31
fluctuates fluctuates with the same
03:22:35
frequency with identical phases in general
03:22:38
competitor coherent is called
03:22:40
common-mode sources there in general
03:22:43
they are all the same, if these
03:22:46
sources here they are, here they are
03:22:48
emit a wave like this into space and
03:22:51
this one emits a wave
03:22:53
turns out in . where is one wave
03:22:57
superimposed on the second, let's do some more now
03:23:00
this one draws at this point, let's say yes
03:23:04
here we will appear
03:23:08
maximum interference as you can imagine
03:23:10
here are two drops 2 drops owned
03:23:14
these waves are so fluctuating
03:23:17
overlap each other in these
03:23:20
points get such a maximum and
03:23:22
maximums if you put a screen here
03:23:25
this is already my enlightenment speaking here too
03:23:28
there will be a maximum of conditions
03:23:30
maximum so that
03:23:32
the course of this wave or one of them here
03:23:35
a wave or two were different from each other
03:23:40
so that the stroke difference is equal to the length
03:23:44
waves if they differ by wavelength
03:23:47
then here is one wavelength and here is the second one
03:23:51
like this it comes then they are in this
03:23:53
point are amplified if the path difference
03:23:56
it will be like this they will strengthen each other
03:23:57
friend and these are the maximum conditions
03:24:00
interference that is
03:24:02
This
03:24:04
an integer number of waves or, in other words,
03:24:08
even number semi in he is a condition
03:24:12
maximum
03:24:15
if they come in antiphase
03:24:18
that is, here he is like this in
03:24:22
the opposite side
03:24:23
are there for this we have a difference
03:24:27
progress
03:24:28
should be equal
03:24:32
odd number of half-waves 2k + 1 or 2 k
03:24:36
-1 and note that here
03:24:42
the order of the maximum is to a
03:24:48
here it's a minimum order
03:24:52
it's simple
03:24:55
some odd number
03:24:57
treat it like a menu number no
03:25:00
it's just some odd number
03:25:02
think for yourself where the first one is
03:25:04
at least where 2 buckwheat
03:25:08
yes and this is the thing
03:25:12
called the wave path difference
03:25:15
difference
03:25:17
progress
03:25:19
waves
03:25:26
and this is the optical difference
03:25:30
wave progress
03:25:31
she
03:25:33
if you are among
03:25:35
it increases in rate
03:25:38
refraction times in the medium
03:25:43
wave progress
03:25:47
increases by n times the indicator
03:25:52
refraction times
03:25:56
So
03:25:58
Well, what did the project say, that is, if you are there
03:26:01
in the liquid you have these two points
03:26:03
are found then the wave input will be greater than
03:26:07
if you were just in a vacuum the same thing
03:26:09
does
03:26:11
their chok chok chok you are my teacher
03:26:20
so okay and you know it turns out if
03:26:28
so all conditions were not shown max conditions
03:26:31
let's talk about now
03:26:33
diffraction gratings
03:26:37
In general, you can talk about diffraction gratings
03:26:39
tell a lot and in detail
03:26:42
but this will probably be superfluous because
03:26:46
recent years diffraction gratings
03:26:48
occurs quite limited
03:26:50
range of tasks
03:26:52
means what you need to know
03:26:54
firstly, what is the lattice period?
03:26:58
distance but let's between the centers here
03:27:01
these cracks, this is called a period
03:27:04
lattice translation
03:27:06
gratings, of course you can think there
03:27:10
distance from the edge of this to the beginning of this
03:27:12
Well, there can be different calculations in general
03:27:14
the meaning does not change from this period
03:27:16
gratings
03:27:17
to find the lattice period you can
03:27:20
take the length of the lattice and divide by
03:27:23
number of lines or on the grid
03:27:30
n quantity
03:27:33
strokes and
03:27:37
it turns out that the period is the goal divided by
03:27:40
n and when some ray falls on you
03:27:48
Now, if we just have one beam first, let's
03:27:50
let's talk on the screen then you will have
03:27:54
get the maximum here here here here
03:27:57
be at maximum and
03:27:59
zero order to equal zero that is
03:28:02
here and white there, that's if you are white
03:28:05
it falls on the spectrum, but
03:28:08
here will be the maximum of the first
03:28:10
at some angle
03:28:13
name1 and d sine x
03:28:17
equal to 0 to
03:28:20
that is, it turns out that the sine of the angle
03:28:27
is proportional to the wavelength thus
03:28:30
it turns out that
03:28:33
red color will be refracted under
03:28:37
high angle
03:28:39
than some purple one from which
03:28:43
begins
03:28:46
this is this this is of the first order
03:28:49
just because of the wavelength because of the length
03:28:52
Will the waves have different angles?
03:28:57
Well, there we can go further
03:29:01
second order maximum blue here
03:29:04
there's red here
03:29:07
vodka equals 2
03:29:14
here the spectrum is also decomposed into
03:29:17
diffraction grating
03:29:19
actually about the diffraction grating here
03:29:21
this is the only formula you need
03:29:23
need to know for sine and calendo if
03:29:26
you have a diffraction grating on
03:29:31
a beam of rays falls on her and
03:29:36
there is a lens here
03:29:39
you're so [ __ ] what the hell and here you are
03:29:42
focal length
03:29:44
there is a screen
03:29:47
then I can of course explain in detail but
03:29:50
take it as if it's easy
03:29:55
you just have this ray
03:29:59
falls in the center and you also have fairies
03:30:04
only here there will be a distance
03:30:06
now that's it and everything is as usual
03:30:08
decide
03:30:10
can you describe in detail there?
03:30:12
happens but I don't want to spend it on it
03:30:13
time there in general everything is the same just
03:30:16
not this is the distance you take
03:30:17
the distance between the lens and the screen is
03:30:21
if we have a large number of rays
03:30:22
they will also be there first order second
03:30:25
third order and so on and they are like this
03:30:27
at certain angles they will be
03:30:30
this year 6 hours this school year
03:30:33
this is the last 6 hours before the exam then
03:30:35
very soon
03:30:42
I studied Mechanics and Mathematics and so there
03:30:45
it turns out that all the sections I studied in general
03:30:49
course
03:30:51
well I specialized in
03:30:54
mechanics
03:30:56
very specific mechanics on
03:30:58
hydromechanics that is, how are you at first
03:31:01
you just go through all the sections in love
03:31:04
any physics university and then you plunge
03:31:07
in some specific place here I am
03:31:09
mekhmat plunged because I was on
03:31:11
Department of Fluid Mechanics Yakunin plunged
03:31:14
everything related to liquid dipped yes
03:31:17
it turns out if you went to the department there
03:31:20
I don’t know elasticity, then that’s all you would do
03:31:22
connected with elasticity and all that, but
03:31:27
there are many of us departments
03:31:37
and what about this vodka?
03:31:40
this is the maximum number
03:31:44
in this case
03:31:49
Another lemon General Secretary will be absolutely gorgeous
03:31:55
Chelsea
03:31:59
let's decide
03:32:02
what is the probability of the task getting on
03:32:05
optical instruments
03:32:08
I don’t know the guys, they used to be very loved
03:32:11
give [ __ ] up every year
03:32:13
a camera, some kind of telescope, but
03:32:17
before this is about 10 years ago last years in
03:32:20
basically just gives some lenses
03:32:23
or there are lenses where something vibrates
03:32:26
this is how the pendulum remember we solved it
03:32:29
look at the lenses like this or come on, what?
03:32:32
It will be this year, I think it’s optical
03:32:34
devices are less likely
03:32:37
lenses are more likely but we'll see
03:32:40
what will happen in reality
03:32:41
maybe they will give a big refraction
03:32:44
probability
03:32:52
yes, well, since this is the number to the maximum
03:32:55
forever in general of course
03:33:01
we go further to the diffraction grating with
03:33:04
period 1, 2 micrometers
03:33:09
monochromatic light falls normally
03:33:12
highest diffraction order
03:33:14
the maximum that can be obtained for a given
03:33:16
system is equal to two
03:33:18
k maximum is 2 find the length
03:33:22
waves of monochromatic light
03:33:26
wavelength question
03:33:37
then look
03:33:39
here we have such a thing
03:33:42
d sine alpha equals potassium yes yes and
03:33:47
for all k the condition must be satisfied
03:33:51
that the sine is alpha of all visible to the sine
03:33:56
alpha is less than one because even if
03:33:59
is already equal to units if alpha is 90 degrees
03:34:02
then he goes into infinity and we don’t
03:34:05
we'll see this maximum so let's
03:34:07
from here we express sine alpha
03:34:10
market lam to devote to d it turns out kolyan
03:34:14
you need to divide by less than 1
03:34:18
therefore Linda is less than d divide
03:34:21
on to
03:34:29
before
03:34:31
what is this now
03:34:40
it turns out this is the inequality for k
03:34:46
maximum fulfilled
03:34:49
hence to
03:34:51
maximum lambda should be divided less
03:34:55
units a for k maximum plus one not
03:35:02
is carried out so that this is the maximum
03:35:05
order that is to maximum + 1 0 divide
03:35:10
etc. must be greater than or equal
03:35:12
unity so we can find with
03:35:15
you gap for linda linda
03:35:18
belongs to d divide
03:35:23
under d
03:35:27
divide by k maximum + 1 to d divide
03:35:33
on to maximum
03:35:35
that is
03:35:43
let's count
03:35:46
12
03:35:50
divide by 3
03:35:55
this is 400 nanometers
03:36:01
Don
03:36:04
12 divided to 600 by per meter
03:36:11
don't turn it on, that's it
03:36:23
monochromatic light falls normally
03:36:31
no more order find the wavelength
03:36:34
that's enough crookedly worded
03:36:37
conditions thanks to my curator
03:36:39
that is, it’s not clear what he’s asking for
03:36:43
find
03:36:46
what is the shortest wavelength greater in
03:36:49
in general what was
03:36:51
Magda and more diffraction order
03:36:54
maximum equal to two, our wavelength should be
03:36:57
from 400 including to 600 excluding in general
03:37:01
in this range any number is
03:37:03
answer
03:37:05
there is a micrometer clearly us 3d
03:37:13
how much time do you need to spend what is yours
03:37:16
the rate under you will happen in a month
03:37:19
somewhere
03:37:23
2 hours a day
03:37:26
Daria course pounds are given away for free
03:37:28
still
03:37:30
ok guys let's move on
03:37:44
why are we changing the sign there? Well, because
03:37:48
we won't see us even if
03:37:52
equal to one if the sine of the angle is equal
03:37:55
unit then at 90 degrees we are not
03:37:58
let's project this on the screen +
03:38:25
then yes you rolled down the truth you can
03:38:29
see my course padi you're here
03:38:31
old version and it was more complicated than
03:38:35
options
03:38:36
last year let's say last year yes
03:38:39
you have become lighter
03:38:43
diffraction grating with period 10
03:38:46
minus 5 meters
03:38:53
located parallel to the screen on
03:38:55
distance 0 75 meters and to it
03:39:04
the first order maximum will be
03:39:06
be observed at a distance of 3 centimeters
03:39:08
from the center deflationary pictures three
03:39:12
centimeter
03:39:14
what wavelength will the beam fall?
03:39:16
the light is on the normal and the angles are small
03:39:20
when angles and small sine alpha are approximately
03:39:23
equal to alpha approximately equal to tangent of olives
03:39:25
that is, here we have a diffraction grating
03:39:29
here is the first maximum
03:39:32
on the screen from 1 to the first and
03:39:38
it turns out d sine alpha equals k lambda
03:39:44
since sine is approximately equal to tangent de
03:39:47
tangent alpha calendar and tangent alpha
03:39:51
this is x1 per ale
03:39:56
that is, dx one by n is equal to k by linda
03:40:02
linda dx 1 divide by elka glinda
03:40:08
10 minus 5 by 003
03:40:12
to 075 to 1
03:40:18
Sanya already has 11 likes, simply gorgeous
03:40:23
gorgeous 10 minus 5 by 0 0 3 0 75
03:40:31
this is 400 nanometers for a wave
03:40:36
a good value means the answer is correct
03:40:41
more likely
03:40:44
to perk up like you more
03:40:47
tell me I'll eat
03:40:49
carbonated marzipan bar
03:40:52
classic of us wheel
03:40:55
this is not an advertisement
03:41:06
were so uncomfortable here came up with
03:41:11
I'm embarrassed by the score
03:41:22
I immediately started working harder by using my head
03:41:34
maybe there are sides to this
03:41:47
why do they write on game solvers that sine can
03:41:51
be equal to 1 such task
03:41:53
because I'm solving the exam
03:41:55
sometimes the solution is written by idiots
03:42:00
decided is time standards
03:42:04
there are errors and a lot of them
03:42:08
sometimes idiots not always but sometimes
03:42:11
idiot
03:42:24
how to charge the test with electric current
03:42:38
Well, what can we say about solving the Unified State Exam?
03:42:41
even if the compilers of the exam themselves
03:42:45
sometimes they write an official solution for this
03:42:49
which for for their tasks which they
03:42:52
came up with
03:42:53
which these too must come to terms with
03:42:56
experts with errors
03:42:59
imagine I just once had
03:43:02
access used to be given access to these
03:43:05
the solution that hippie and I provide
03:43:08
I personally found two errors
03:43:11
two problems that they solved incorrectly and
03:43:15
I immediately have a question: how
03:43:17
they checked it they checked it after all
03:43:22
by the right decision for they looked
03:43:25
does the deprivation of a student coincide with an infidel
03:43:28
decision
03:43:30
There is no clear answer to this question
03:43:33
we can because probably how much
03:43:36
there were so many experts and and and
03:43:39
the disagreements about this are kind of stupid
03:43:41
experts who themselves did not know how
03:43:44
decides collected just checked which
03:43:47
smarter experts probably somehow
03:43:50
checked in good faith but we are already
03:43:53
unfortunately all this is not known
03:43:57
this could happen right in the game
03:44:02
could it happen this year I don’t know
03:44:05
I can say with confidence that it was
03:44:08
unfortunately it was
03:44:15
so you can be an expert who is not
03:44:18
know how to solve a problem
03:44:21
expert doesn't really mean that you
03:44:24
good problem solver
03:44:28
that is, I streamed this with an expert
03:44:31
who trains other experts and
03:44:35
she runs the stream and I correct her
03:44:38
errors are wrong I explain why
03:44:41
wrong and she doesn’t understand right away
03:44:44
I play because of this because of this
03:44:47
she there it there to brought out some
03:44:50
formula once and told me that
03:44:54
potential energy when removed
03:44:56
the satellite will decrease where you are
03:45:00
she's like that
03:45:02
some substitutions are made, I explain
03:45:05
she still doesn’t understand how it is
03:45:08
sometimes they find it so absurd
03:45:10
an expert who trains other experts
03:45:13
but still sometimes
03:45:16
problem in the tasks she has a solution there
03:45:18
were also incorrect or beyond
03:45:21
school curriculum framework
03:45:23
an expert is not a sign of quality no matter how
03:45:26
Weird
03:45:29
So
03:45:31
[music]
03:45:49
And from oh caught up you immediately slowed down so much to and
03:45:53
it happens like this
03:45:56
trash of course can now be considered
03:45:58
the opportunity to appeal before
03:46:02
there may be problems with this appeal
03:46:05
for example this year I'll just show you
03:46:08
there was a bug when checking the task
03:46:12
in general, let's do less on optics
03:46:17
double I'll do it
03:46:19
that is, it goes something like this
03:46:23
Ray
03:46:25
then it refracts
03:46:28
then it is reflected and
03:46:31
we need to find the alpha angle there at night
03:46:36
it's natural there's something else here
03:46:38
there's a din there, in general, everything is given, here's a ray
03:46:41
it comes out like this
03:46:43
we need to find
03:46:46
there, well, let’s say he doesn’t know what angle
03:46:49
angle of incidence to beam to here
03:46:53
total internal reflection occurred
03:46:55
and we are asked to draw the course of the ray inside
03:46:59
damn I checked it later and went to look
03:47:03
conditions and even wrote it down in my
03:47:07
contact messages sent so as not to be
03:47:09
unfounded
03:47:10
I'll open it now and read it right away
03:47:13
it was written there
03:47:22
Zolotukhin
03:47:43
then right now
03:47:48
[applause]
03:47:52
someone far from mortal
03:48:02
make a drawing indicating the beam code
03:48:05
rays in the wedge make a drawing indicating
03:48:09
the course of the rays in the wedge you are looking at
03:48:12
it turns out that this beam is not in the danone knee
03:48:16
it's drawn there anyway, so in it
03:48:18
please draw this ray it's in
03:48:21
wedge this beam is in the wedge and this beam is in
03:48:27
wedge
03:48:30
[ __ ] this ray
03:48:32
in my opinion no, he is walking along the border
03:48:36
division of two environments
03:48:37
but since this is a corner I understand
03:48:41
refracted
03:48:44
then we cannot say that he is
03:48:47
in wedge actually actually
03:48:51
when your angle is full inside
03:48:53
reflections you have, this ray is generally here
03:48:56
does not work and all the power goes to reflection
03:48:59
that is, in my opinion it was necessary
03:49:02
draw a ray like this like this
03:49:03
reflected and moved on but they
03:49:07
implied that this beam is necessary
03:49:09
be sure to draw and show here
03:49:11
angle 90 degrees, well here it is and here it is
03:49:15
how were people supposed to know that
03:49:19
they meant for them this beam was in
03:49:21
wedge although this angle of refraction and
03:49:24
in general its power is zero but to me
03:49:27
It seems to me that this was a bastard
03:49:30
I filed an appeal for this
03:49:33
the fact that they reduced me for this is just laziness
03:49:37
there was more to do but in theory I can
03:49:39
sue to prove that for this
03:49:41
had no right to reduce because this
03:49:44
beam its power firstly 0 secondly
03:49:47
he is not in a wedge he is at the interface
03:49:51
you can still say but not in a wedge
03:49:55
yes, and in general this ray really
03:49:57
its power is zero so
03:50:00
the power is zero and it is not in the wedge and
03:50:03
they still reduce it for its absence
03:50:05
points this is wrong but now we know
03:50:08
what do they want in this kind of task?
03:50:17
here's how they wanted them to be decorated
03:50:20
I shouldn't have heard to draw the reflected
03:50:22
but it was necessary to have refractions of 90
03:50:25
draw such things in advance, of course
03:50:28
you are not a product
03:50:30
refers to inaccuracy of wording
03:50:32
verification inaccuracies
03:50:38
[music]
03:50:42
why was day 30 missed because in
03:50:47
this day
03:50:48
Russian Ben
03:50:51
noah and I these days when I will not lead
03:50:54
and dancing I will conduct open streams like this
03:50:56
don't worry
03:51:03
ok let's move on flat
03:51:06
monochromatic light wave with
03:51:08
frequency 4 to 10 14 hertz
03:51:12
at 10 14 hertz
03:51:16
falls normal to the diffraction
03:51:19
the grille is parallel to the grille behind it
03:51:22
a collecting lens with a focal length is placed
03:51:25
at a distance of 21 centimeters and you see
03:51:27
this is the same case when we have
03:51:30
diffraction grating then lenses then
03:51:33
there we almost score we perceive
03:51:35
as if everything is the same just here
03:51:39
the screen is at focal length
03:51:41
everything everything else is the same as it was
03:51:46
diffraction pattern is observed on
03:51:48
rear focal plane screen
03:51:50
distance between main ones maximum 1 2
03:51:52
about 16 millimeters
03:51:56
16 millimeters a
03:51:59
find the lattice period answer variable
03:52:02
besides [ __ ], we can assume that the angles
03:52:05
small
03:52:06
railings jokes questions so but cleanliness it
03:52:12
c divided by lambda means linda is everything
03:52:18
divide by it
03:52:20
now d
03:52:24
sine x
03:52:28
equal to Landeck and
03:52:32
sinus
03:52:34
approximately equal to tangent
03:52:38
which is equal to x divided by f that is
03:52:43
it turns out b x 1 divided by f equals lambda
03:52:48
d x 2 divided by f equals 2 lambda
03:52:54
hence
03:52:56
d x 2 minus x one
03:53:00
divide by f equals lambda but if you subtract
03:53:03
and lower upper, well, if you substitute
03:53:06
lamda how to highlight on it then we can
03:53:10
express dd is equal to ef divide but not
03:53:15
x 2 minus x1
03:53:19
cf not exam sex one so well
03:53:22
obtained when setting
03:53:24
d3 for ten in the eighth
03:53:27
on
03:53:28
021
03:53:31
on
03:53:32
4 to 10 to 14 and to
03:53:38
0 0 16 great let's count
03:53:47
it's all diffraction
03:54:06
You
03:54:07
[music]
03:54:09
at
03:54:13
I got it
03:54:18
984
03:54:21
micrometer
03:54:28
[music]
03:54:29
Alexander Voronov under what conditions
03:54:32
sine is approximately equal to tangent here you go
03:54:35
answered when the angle is up to 10 degrees
03:54:39
here the differences are minimal and
03:54:43
Let's say it's just sine 10 degrees 2
03:54:48
sine of 10 degrees is how much is it
03:54:56
sine 10
03:54:59
017 3648
03:55:03
I didn’t write down the meters now, but the tangent is 10
03:55:11
tangent 10
03:55:15
0176
03:55:17
33
03:55:20
before that is
03:55:23
differs already in thousandths in thousandths
03:55:26
units and radian measure of angle
03:55:31
is between them, that is, there is a sine
03:55:33
alpha is less than the radian measure of angle and
03:55:36
less than the tangent, that is, well, approximately
03:55:39
they can be considered very close
03:55:41
magnitudes but when more than ten
03:55:44
degrees it's already becoming a replacement there
03:55:46
let's say for sine 5 this is how much we have
03:55:50
hands sine 5
03:55:52
this is zero zero eight seven
03:55:56
156 a tan 5
03:56:04
This
03:56:06
008
03:56:10
75 but if there is such a thing then there is even one here
03:56:14
thousand do not coincide in general
03:56:17
It’s clear that the min angle the better
03:56:20
matches but for these up to 10
03:56:23
degrees this difference is minimal
03:56:28
I carried them to the chair
03:56:32
experiments well done beauty okay
03:56:34
let's move on
03:57:09
30 degrees can be considered a small angle but
03:57:12
not 30 is already a considerable sine there 30 1 2
03:57:17
tangent 30
03:57:20
057 well there already
03:57:23
not that [ __ ]
03:57:25
this is more than ten percent distinguishable
03:57:29
too big a difference
03:57:36
praise yourself more than 70 was in love
03:57:43
I like to chat I don’t like to decide what happens to me
03:57:47
do oneself
03:57:53
onto a diffraction grating with a period of 4
03:57:56
micrometer
03:58:01
A beam of light consisting of
03:58:03
from photons with momentum 264
03:58:08
by ten to minus 27
03:58:12
kilogram per meter per second
03:58:15
so let's discuss it means
03:58:19
photon energy can be described in two ways
03:58:23
ways or as much as on it, well, she
03:58:28
ht divide by linda or as an impulse
03:58:33
photon at the speed of light and
03:58:36
will someone tell me the speed of light where where
03:58:40
I'll tell you the speed of light in a vacuum
03:58:46
that is, let's say you're looking for
03:58:49
momentum in water you know you have momentum
03:58:53
some kind of energy in the water and you know
03:58:56
impulse in the water you take the impulse of yours
03:59:01
photon and multiply everything by the speed of light
03:59:03
anyway in a vacuum you don't reduce
03:59:06
speed of light n times if you
03:59:09
you're at 1 no, that's just speed
03:59:10
light in a vacuum as constant a
03:59:16
right here right here by the way if you
03:59:19
was in some environment then you should
03:59:23
the navel is already in place here already
03:59:27
depends on what environment you're in
03:59:30
you are, that is, well, generally speaking
03:59:32
allocate to linda
03:59:35
if you are
03:59:37
there is a vacuum then this is the goal moment
03:59:50
So
03:59:55
maximum 2 orders of magnitude at what angle
03:59:58
d sine film equals Linda by 2 uk a
04:00:05
equals 2.
04:00:08
it turns out if these are equated each other
04:00:11
friend p equals h divided by linda
04:00:17
then linda equals h divided by p minus
04:00:25
fer
04:00:27
as much as divide by n by k divide by d
04:00:33
free
04:00:35
arcsine
04:00:40
efficiency
04:00:41
fi
04:00:43
arcsine
04:00:46
66 for effectiveness 34 for
04:00:50
22, 64 by 10 to the minus twenty-seventh and
04:00:56
by 4 by 10 minus 6
04:01:14
6 6 by 10 to minus 34
04:01:22
you are trying 4 but 10 minus 7 and
04:01:29
4 is 10 minutes
04:01:42
7 degrees somewhere
04:02:54
large ones to ban and decided yes it’s not normal
04:02:57
So
04:02:59
guys, let's talk a little now
04:03:02
about interference on thin films
04:03:06
interference
04:03:09
on thin
04:03:11
films, that is, when it happens
04:03:14
when let's say you spilled gasoline in a puddle
04:03:19
it seems to you that gasoline is overflowing
04:03:22
let's think in different colors of the rainbow
04:03:26
why is this happening
04:03:29
it turns out that the beam falls there
04:03:34
some and
04:03:38
reflected first from the surface
04:03:42
Well, the wavelength that passes is equal to or
04:03:45
zero is acceptable yes a
04:03:47
some ray passes inside
04:03:51
then they are reflected in the other direction and
04:03:54
comes out and both end up, so to speak,
04:03:57
eye and
04:04:00
it turns out that the first wave
04:04:03
wave input equaled el zero a
04:04:07
second or 0 + 2 d but not really
04:04:13
it's so simple, well, we think that the angle
04:04:15
small so just go back there
04:04:18
but there are some rules means first
04:04:21
rule you should remember when
04:04:24
reflected from
04:04:26
optically denser medium
04:04:32
environment
04:04:35
is happening
04:04:38
a loss
04:04:41
half waves a
04:04:46
less fetus and no loss occurs
04:04:48
accordingly let's see
04:04:51
refractive index of gasoline
04:05:00
[music]
04:05:03
1 and 8
04:05:09
1 and 8 a
04:05:12
near the water 1 and 33 there is deeper gasoline in the puddle
04:05:19
spilled out to show and refraction
04:05:22
big job there is a small one so he
04:05:24
top swim and
04:05:26
it turns out, well, gasoline definitely
04:05:29
higher refractive index than
04:05:31
air therefore when reflected from here at
04:05:35
we are losing semi waves
04:05:38
here we write minus lambda in half, but what about
04:05:41
happens here
04:05:44
it turns out
04:05:46
here
04:05:48
the environment is less dense than gasoline therefore
04:05:53
losses
04:05:55
Lambda won't be cut in half
04:05:58
here
04:06:00
but in an optically denser environment we have
04:06:05
the wave is increasing, that's why we are here
04:06:09
should write not 2
04:06:11
da2 gasoline smoke and
04:06:15
it turns out that you're looking at, let's say
04:06:18
petrol stain on top
04:06:20
the path difference in this case will be equal to
04:06:22
well, let me write it down in detail 0 +
04:06:26
2 gasoline smoke
04:06:31
minus or zero minus lambda anyhow
04:06:35
there is a stroke difference
04:06:37
equals 2 gasoline smoke plus lambda in half and
04:06:44
and if we choose the thickness of the puddle like this
04:06:47
so that it is equal
04:06:49
let's say when we have a difference in speed
04:06:52
equal to an integer number of waves is acceptable for
04:06:55
this dot will be red there
04:06:57
seem red here for the first
04:06:59
maximum let's say Linda is red
04:07:03
equals 2 gasoline smoke plus Linda red
04:07:07
in half and from here we can find
04:07:09
thickness
04:07:11
gasoline puddles that's when it comes to us
04:07:14
will appear red at some point
04:07:16
this is if we look from above there when under
04:07:18
the corners are a little different there already
04:07:20
works
04:07:23
sniffed some gasoline
04:07:26
so let's get it all together
04:07:31
solve this problem
04:08:01
between the edges there are 2 well sanded
04:08:04
thin flat glass plates
04:08:06
placed tone placed thin wire
04:08:08
diameter
04:08:10
0 0 5 millimeters
04:08:14
millimeters
04:08:18
opposite ends of the plates tightly
04:08:20
pressed against each other on top
04:08:21
plate parallel to its surface
04:08:23
a monochromatic beam of light falls
04:08:26
determine the distance between interview persons
04:08:29
ion classes that are observed on
04:08:31
plate 10 centimeters long
04:08:34
10
04:08:36
centimeters if the wavelength of light is 06
04:08:41
micro meters
04:08:45
these guys don't look like this from this drawing
04:08:49
It’s very clear what’s going on, but really
04:08:52
in fact
04:08:53
glass this table flock such a record
04:08:57
here's the fat [ __ ] fat one and here's the second one
04:09:01
glass plate is actually
04:09:05
The drawing should be perceived by you like this
04:09:07
so well, here’s some kind of heroin and
04:09:12
it turns out that
04:09:15
What causes interference?
04:09:16
here the beam falls
04:09:18
let's have a small drop angle done
04:09:21
how the beam falls
04:09:23
reflected in your eye
04:09:27
here the ray passes here it is reflected goes
04:09:33
you understand the eye, that is, he is still here
04:09:37
passes some distance here d but
04:09:41
these are igrek one igrek one a
04:09:45
let's just or them
04:09:47
that is, this is the course of the first wave
04:09:50
or zero since from optically less
04:09:54
dense medium the air is reflected here yes
04:09:57
here the air here is glass then losses
04:10:00
there is no half wave and the course of the second wave is from
04:10:04
optically less dense rows that is
04:10:06
it turns out or 0 plus 2y is not multiplied by
04:10:11
refractive index he ate air food
04:10:13
one minus half-wave loss and
04:10:17
it turns out that the path difference is equal to 2y
04:10:22
minus
04:10:23
lambda in half
04:10:25
that is, it turns out
04:10:28
then we have this difference in the course
04:10:32
equal to an integer number of wavelengths
04:10:38
then we will have a maximum at this point
04:10:43
it turns out well
04:10:46
there
04:10:48
even if equal to zero then we will have
04:10:51
the maximum is if zero is equal to oh 2y cm
04:10:56
if y is equal
04:10:59
Linda divide by 4 here is the first light one
04:11:04
we get a spot
04:11:06
if 2y equals minus lambda in half equals
04:11:12
linda that is y is equal to three quarters linda
04:11:16
the second bright spot turns out well and so
04:11:20
then add in total and by half
04:11:23
second
04:11:24
first
04:11:27
there
04:11:29
there will be a third
04:11:31
y5 lambda divide by 4 y
04:11:35
in short, half the wavelength was added
04:11:38
the third spot will be light, that is
04:11:41
you understand so for anyone we can
04:11:43
paint
04:11:44
it turns out how much they increase
04:11:47
here we have it here
04:11:50
there will be some maximum
04:11:54
then we moved here like this if we 0
04:11:59
hmm dropped to 4 here it will be 2 again
04:12:03
maximum then another 0 to 4 dropped
04:12:06
again you understand the maximum and this is it
04:12:10
when our path difference was zero
04:12:13
had her own 1 trace stain and she
04:12:16
was at a distance
04:12:19
quarter wavelength
04:12:21
next such bright spot will be on
04:12:24
full wavelength
04:12:28
you need half waves too, three quarters
04:12:37
So
04:12:40
to the audience half and half of course
04:12:55
what is Linda talking about here, divide by 4?
04:12:59
further Linda in half le onde in half
04:13:01
ribbon in half
04:13:03
goes down
04:13:06
why did I say all this, I forgot
04:13:12
that means 2 is
04:13:15
4 4
04:13:20
up to 8 Linda in half I add
04:13:24
so it was given to me
04:13:27
What
04:13:31
so that it is not given
04:13:34
A
04:13:38
interference distance
04:13:40
stripes that is, I need to find this
04:13:43
there will always be a distance
04:13:44
identical this is a question this is a question
04:13:50
she would be here, she would be here, everywhere
04:13:54
will be b
04:13:57
it turns out
04:13:59
this angle is alpha this angle is alpha with one
04:14:02
side tangent is equal to lambda in half
04:14:06
divide by b
04:14:08
on the other side of tangent alpha
04:14:12
it is impossible to say that it is exactly approximately equal
04:14:16
d divide by
04:14:21
Well, it’s clear that the diameter is this plus
04:14:26
this one, since the corner is small, we
04:14:30
we can roughly assume that
04:14:32
this is it
04:14:35
what is this thing just if down
04:14:38
lower approximately equal to the radius and there you go
04:14:43
this
04:14:44
that is, it turns out yes divided by r is equal to
04:14:47
Linda divided by 2 b, that is, b is equal to
04:14:53
lambda el divide by 2d that is b equals
04:14:58
0 6 by 10 minutes 6 by 0 1 divide by 2 by
04:15:05
0 0 5 by 10 minus 3
04:15:27
tags
04:15:29
0 6 to 10 to the minus sixth
04:15:33
by 0 1 by 2 by 0 0 5 to 10 to minus
04:15:40
third
04:15:51
600
04:15:58
the distance between these interference
04:16:00
stripes
04:16:03
[music]
04:16:05
0 6 millimeters
04:16:10
almost half a mile to just over half a mile
04:16:13
millimeters
04:16:20
can be seen
04:16:24
can be seen
04:16:27
like on the line only twice as often
04:16:34
tags well let's move on
04:16:58
why is lambda in half they are lambda in 4 too
04:17:02
look between
04:17:05
you should write here there
04:17:08
y1 and y2
04:17:12
y3 here y there three let's say different
04:17:16
from y 2 0 hmm in half that's where any y
04:17:22
minus y to minus 1 will differ by
04:17:25
lambda in half no matter what number you take
04:17:31
this is possible in general terms in principle
04:17:34
let's write down the fungus
04:17:36
This
04:17:42
lambda divide by 4 +
04:17:47
divide the kolyans in half and
04:17:53
it turns out that the fungus minus y to -1 is
04:17:58
Linda divide by 4 + kolyans in half
04:18:02
minus lam by divisor 4 plus to us and to
04:18:08
-1 Linda hit and
04:18:12
here if you open the bracket it turns out
04:18:14
just lambda in half, well, probably for
04:18:16
it is better to write down the design in general terms
04:18:18
to show that this is for anyone
04:18:20
the maximum will be fulfilled
04:18:31
With
04:18:38
ok
04:18:40
it will be on X
04:18:42
more and more details
04:18:46
there will be 2 6 hour streams on X, well one
04:18:50
6-hour optical one 6-hour optical
04:18:53
quantum i holes
04:18:56
xx more details
04:19:10
he's great Alexey Kleva Kleva for what
04:19:15
I came in okay, I’m erasing this from
04:19:18
damn it's funny there are so many people already
04:19:21
released a strong prepared for and
04:19:23
ban and
04:19:25
Very nice
04:19:34
see old faces
04:19:36
or rather old Nicky
04:20:07
you became his no number one he is not
04:20:10
I'll like it
04:20:13
sometimes it's really painful and unpleasant
04:20:16
well what can you do
04:20:20
our faces are still on the Maidan, so many wrinkles
04:20:23
on our faces
04:20:32
really sane why 6 hours quantum
04:20:35
when mechanics 4
04:20:37
mechanics actually 8 hours
04:20:44
called clearing of optics
04:20:46
reducing light reflection from
04:20:48
optical refractive surfaces
04:20:50
systems for example from a lens
04:20:53
camera for this on the surface
04:20:55
lens applies a thin film with
04:20:58
refractive index different from
04:20:59
refractive index of lens glass
04:21:01
and select its thickness to a certain
04:21:03
So what is the minimum thickness?
04:21:06
have this film in order to
04:21:08
minimize the reflection of light in
04:21:10
most sensitive to the eye
04:21:12
human yellow-green part of the spectrum
04:21:15
at wavelength in air 560-560 0
04:21:18
meters, they write 500
04:21:25
if the refractive index of the film at
04:21:27
this wavelength is equal to 1
04:21:31
494
04:21:33
what shade of color does it have?
04:21:37
the enlightened have the enlightened
04:21:39
lenses light incident on the lens
04:21:42
can be considered almost normal
04:21:44
spalletti means you're filming something
04:21:49
for example, porn, a ray is falling
04:21:54
refracted and
04:21:58
in theory
04:22:00
reflects, that is, it is reflected here and here
04:22:03
reflected
04:22:05
right here
04:22:07
one of the lights is reflected and
04:22:11
you want as little as possible
04:22:15
reflected so that as much as possible
04:22:17
got inside the lenses and got caught
04:22:21
to this and to
04:22:23
on film stayed on film for this
04:22:27
we need to choose the thickness this way
04:22:30
so that the wave path difference
04:22:34
equaled an odd number of half a vol
04:22:37
there is so that del del is so that we have
04:22:40
there was interference
04:22:42
you know guys, let's think about it
04:22:45
there's a loss happening here
04:22:47
half-waves uniquely when reflected here
04:22:51
also there is a loss because 1 and 4
04:22:55
a.n. glass
04:22:59
1 and 5 y
04:23:02
the glass is shorter there
04:23:05
more than 14 and it turns out that or 1 is
04:23:10
0 0 minus the strap in half
04:23:12
l2 is or zero minus lambda in half and
04:23:16
plus two more days of film and
04:23:21
the difference in wave path is obtained
04:23:24
equals 2 smoke films
04:23:27
then it comes out
04:23:29
what if we choose the thickness like this
04:23:33
so that we have here
04:23:38
we take an odd number of half-waves in a given
04:23:41
case 1 interference minimum when
04:23:44
we simply have equal conditions according to the gender wave
04:23:48
at least we will succeed
04:23:51
extinguished and eventually
04:23:54
we won't see this reflection
04:23:58
it turns out that we are asked to find this d d d
04:24:01
then it will be equal to Linda divided by 4 n
04:24:05
films that is al dente yes yes yes then
04:24:10
There is
04:24:11
560 here minus 9
04:24:14
4 by 1 and 4
04:24:18
5 6
04:24:21
01 micrometer
04:24:25
I hope I counted correctly or
04:24:29
wrong
04:24:32
100
04:24:33
on on 0 1 and when they got together
04:24:39
[music]
04:24:45
boob and fly
04:24:49
titya sounds cooler
04:24:57
How did we understand that we need at least a puddle?
04:25:01
coating the optics for a larger signal
04:25:04
from what we shoot reached the film
04:25:07
they were the ones reflected from the lens to
04:25:11
more saturated more light entered
04:25:14
the more light comes in the more
04:25:16
we will have a saturated image
04:25:31
damn what not or sura attacked
04:25:35
By the way, I didn’t observe any jambs for or sura
04:25:39
I observed problems with his predecessor
04:25:43
which resource wrote crap there and I
04:25:47
I wanted and sura too once I once
04:25:49
I came in somehow, but the ban solved the problem, but
04:25:51
I decided correctly so
04:25:53
I personally don’t want it, it’s your initiative
04:25:57
purely, in general the desk courses are [ __ ] but
04:26:00
resource
04:26:02
normal what
04:26:05
so [ __ ] me well checklist I can't stand it
04:26:08
these are the sales methods ports are easy
04:26:11
disgusting it's just [ __ ] [ __ ] up
04:26:15
checklist I'm allergic to checklists
04:26:19
top 10 form that's how I heard it
04:26:22
right this
04:26:24
I start beating people when I check in
04:26:28
my brother will suit me live with everyone
04:26:30
paired don't want top 10 formulas that
04:26:33
solve 90 percent of the exam in physics
04:26:36
I want to bend it right away, it’s good that’s so
04:26:39
people on the street don't approach me anymore
04:26:41
been sitting for a long time
04:26:45
By the way, I forgot to write about those
04:26:52
about the shade
04:26:55
comes out in the yellow-green part of the spectrum
04:26:59
every hunter wants to know where
04:27:02
pheasant sitting

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