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математика
Савватеев
движение прямой
математическое движение
отражение
перенос
параллельный перенос
100 уроков математики
физическое движение
движение
савватеев
100уроковматематики
геометрия
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  • ruRussian
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00:00:03
hello, today we will study
00:00:06
movements, what is movement,
00:00:09
physicists will tell you that movement is
00:00:12
the process of moving
00:00:14
some object in space, that is, the process itself is
00:00:19
looked at by mathematicians, but the concept of movement is
00:00:21
a little different for a mathematician,
00:00:24
movement is not a process, but roughly speaking
00:00:27
the result, that is, we look where the object
00:00:30
was at the beginning, look where it was at the end and
00:00:33
here is the result of the movement we call
00:00:36
movement, well let's give a strict
00:00:39
definition of what movement is, the
00:00:41
definition of movement is a transformation of
00:00:47
an object, that is, a change in its position
00:00:50
in space such that
00:00:54
no deformations occur, that is, the
00:00:57
distance between any two points of
00:00:59
the object
00:01:00
will be preserved if we change it at the beginning
00:01:03
and at the end it will be the same number,
00:01:05
in order to write this in a strict
00:01:07
mathematical form, we need to
00:01:10
resort to some
00:01:12
notation to terminology, first of all,
00:01:15
as in school mathematics, numbers are
00:01:19
sometimes called letters, especially when solving
00:01:21
equations x and y so further we will
00:01:24
call the movement
00:01:26
letters of the Latin alphabet, that is,
00:01:29
if we are referring to some kind of movement
00:01:31
that we are currently studying, well, let’s
00:01:33
call it, for example, a letter,
00:01:34
but we will also denote the points of the object with
00:01:38
some Latin letters
00:01:40
x and y and then what is movement
00:01:43
formally, movement is such a change in
00:01:48
position that for any this is
00:01:50
quarter as mathematicians say,
00:01:52
denoting the words any for any two
00:01:55
points from our object, the distance
00:02:02
that we will denote by the letter po
00:02:05
between the result,
00:02:10
that is, where the points ended up after the
00:02:13
same movement was applied to them
00:02:17
is equal to the distance between them before the
00:02:21
movement was applied movement can still
00:02:24
be understood drop dust cash register
00:02:26
a person comes and orders each point of
00:02:29
the object to move somewhere if such an
00:02:31
order is possible without changing the shape of the
00:02:33
object this is what we say that this order
00:02:35
is a movement let's give two
00:02:37
examples one example will be an example of
00:02:40
movement and another example will be, generally
00:02:42
speaking, an example of movement, a space that
00:02:45
is not movement, an example of movement,
00:02:48
then a plane flies from city to
00:02:50
city, here it was at the airport of one city,
00:02:52
stood at speed, flew all this time,
00:02:55
it did not change its position, that is, its
00:02:58
movement from the starting point to at any
00:03:00
point photographed during the flight,
00:03:02
as well as at the moment when he sat down, there will be a
00:03:05
transformation of movement, but if we
00:03:08
consider a bird that is flying,
00:03:11
then its movement from the point where it
00:03:13
sits to the point where the analyst
00:03:15
will not be movement because it has wings, it flaps its
00:03:19
wings and the distance there between the tip of the
00:03:21
wing, for example, and the tail will
00:03:24
change during such a flight, so
00:03:26
the movement of the bird, even the movement of the bird from the
00:03:29
moment when it was sitting to the moment when
00:03:31
it flies, is a transformation of an object, a
00:03:34
bird that is not a movement. Specifically,
00:03:38
you and I will first deal with
00:03:40
the movements of a straight line, what is a straight line from a
00:03:45
point From the perspective of mathematics, a straight line
00:03:47
is infinite in both directions, very
00:03:51
very thin, as mathematicians say, an
00:03:53
infinitely thin, even line
00:03:57
means that in order to imagine the movement of a
00:03:59
straight line, you need to imagine it from some kind of
00:04:03
material that does not allow
00:04:05
stretching, they do not bend, and if there is
00:04:09
such a wire and this wire
00:04:12
we want to somehow move the opportunity
00:04:14
to do this, well, in principle, you can
00:04:17
guess that we can take it as a
00:04:20
certain point and move the whole thing as a whole
00:04:23
to the right here is another point and
00:04:26
from point x. y y so this will move this
00:04:29
all the other points will also somehow move
00:04:32
this movement is called parallel
00:04:35
transfer and we will also give it
00:04:40
some of them we will give it a name we will designate
00:04:43
it for and to specify that
00:04:47
is, as if there is a name there is a surname
00:04:50
this surname is this indicating two points from
00:04:53
which to which should be transferred and I immediately
00:04:57
want to note that if we took some
00:05:01
other two points but at exactly the
00:05:03
same distance we moved a
00:05:08
straight line from point x3 point y stroke then this is
00:05:13
exactly the same movement as it
00:05:16
means exactly the same movement,
00:05:17
it means the order that is given to each
00:05:22
of the points on the left and right is the same
00:05:24
in general when they say that the movement is the
00:05:27
same, that two movements are equal to each
00:05:30
other, which means two movements are equal to that
00:05:31
group,
00:05:32
it means that any point is given the
00:05:34
same an order to move somewhere and
00:05:37
we can write down that these two
00:05:39
transfers are actually the same
00:05:40
transfer, okay, is it possible we are looking to
00:05:44
do something with this straight line, but if we strain
00:05:47
our imagination a little, we can
00:05:50
imagine what we took the straight
00:05:53
sharpening was reflected behind this point o and
00:05:58
like this, I was reflected, that
00:06:00
is, as if turned 180 degrees,
00:06:02
as a result the straight line as a
00:06:04
single whole coincided again with the
00:06:07
position it occupied before, but
00:06:10
now
00:06:11
all the points except point o changed their
00:06:13
position, namely they through .
00:06:15
jumped over the same distance,
00:06:18
we will call such a transformation a
00:06:21
movement relative to a point,
00:06:24
well, you can. take some other place, this
00:06:28
will be a different transformation of the reflection
00:06:30
relative to another point, but something else needs to be
00:06:34
done with a straight line or there are no more
00:06:36
movements, that is, if we
00:06:38
changed the position of the straight line so that as a
00:06:41
whole it remained there, but the
00:06:44
points could change their position then
00:06:49
The question is, is it possible that the transformation
00:06:52
we made was some kind of
00:06:53
transfer and not reflection, the answer is no and
00:06:57
there is such a theorem, classification of
00:07:00
motion, any movement of a straight line is either
00:07:02
parallel translation or reflection, we
00:07:05
will prove this theorem
00:07:08
according to the previous one, the question may arise,
00:07:12
why not the straight line as a whole
00:07:15
is rotated by approximately 30 degrees or
00:07:17
90, this will also be a movement;
00:07:20
in fact, the distance between any
00:07:22
two points will be preserved with such a
00:07:24
transformation. The answer is this:
00:07:27
we are currently studying the movement of a
00:07:31
straight line that does not lie on a plane and in
00:07:33
space,
00:07:34
but the movement of a straight line in which it as well as
00:07:38
itself as a single whole remains in place,
00:07:40
that is, we are considering such
00:07:42
transformations of the line that its points can
00:07:44
change position, but at the same time, if we
00:07:47
look at it as a drawn
00:07:49
object, we will not see any changes, and
00:07:52
in this case there is really nothing
00:07:54
except translations and reflections It’s impossible to come up with
00:07:57
and you can even prove the point
00:07:59
that there is nothing and no movement is
00:08:01
interesting because you need to take their
00:08:05
composition, that is, they allow an
00:08:08
operation such as adding or multiplying
00:08:10
numbers, but only much more complex,
00:08:13
what is the composition of movements is simply
00:08:16
performing them one after another, for example
00:08:20
first they performed some kind of reflection of a
00:08:22
straight line relative to some point and
00:08:25
then a parallel translation
00:08:27
and vice versa began a parallel translation
00:08:30
and then the reflection that the result
00:08:32
was
00:08:33
our experience of communicating with numbers tells
00:08:37
us that there should be no difference,
00:08:39
that we say a + b so that plus a this is the
00:08:42
same number and also with multiplication,
00:08:44
but here a surprise awaits us, let's
00:08:48
study this surprise in more detail and so here
00:08:52
we have it drawn.
00:08:54
and we perform a reflection relative to
00:08:57
this point and then we perform a
00:09:01
parallel transfer of attention I write these
00:09:07
two operations are performed from right to left as in the
00:09:09
Hebrew my Arabic alphabet why
00:09:13
this is also a separate interesting point in
00:09:15
mathematics it will be more convenient to act this way
00:09:19
because
00:09:21
what it is these are two sequential
00:09:24
orders
00:09:26
that are given to the points we can take a straight line
00:09:30
there and substitute it into this order,
00:09:31
let’s say point x and see what happened to it
00:09:33
. Erica
00:09:35
let's generalize some other point to let's call some point
00:09:38
lying on this line beyond z and then if
00:09:43
I want to first make a reflection and then
00:09:45
a transfer, then I write that this is a transfer
00:09:51
performed on the result of the reflection of
00:09:55
point z, that is, on the new point that
00:09:57
was obtained as a result of the reflection of the point behind
00:10:00
this relative to the point o,
00:10:01
and it turns out that this composition of
00:10:04
movements is written as through brackets in the
00:10:08
same order, then here are the letters
00:10:09
indicating the transformation, here in the same
00:10:11
order it is clear that the composition of movements
00:10:14
will also be a movement, but if
00:10:17
the distances are preserved here too they
00:10:20
were preserved and as a result of these two
00:10:22
operations the distances cannot change,
00:10:24
therefore this is some kind of movement of a straight line and
00:10:28
as you and I already know, although we have not yet
00:10:32
proven any movements of a straight line except
00:10:34
translations and reflections do not exist,
00:10:37
therefore what we wrote down is this
00:10:39
composition, it is also must be either
00:10:41
figurative or reflection, let's
00:10:44
see how the points behave to
00:10:46
guess
00:10:47
what this composition is equal to, well, for example,
00:10:50
we can see where
00:10:55
it goes. and this is simpler because at the
00:11:00
beginning it does not go anywhere;
00:11:02
when reflected, it remains in place, but when
00:11:04
transferred,
00:11:05
it shifts by this vector, a
00:11:10
vector is called such segments are directed
00:11:13
from one point to another
00:11:14
by the same longer vector to the right, so
00:11:16
it has moved, here it has moved In
00:11:19
some . and their pin probably
00:11:24
gives us a hint, probably gives us a hint
00:11:27
that this transfer will probably be
00:11:29
this transformation, but before we
00:11:31
make such hasty conclusions, let’s
00:11:34
study the behavior of some other point,
00:11:38
let’s study the behavior of, for example, a dot
00:11:42
and a stroke at this point, what
00:11:45
will happen to it these here with this
00:11:48
composition in this order if there were 90
00:11:51
she went even further tied up this
00:11:53
frame but let's see what actually wo
00:11:56
n't happen with what will
00:11:58
happen when the sentence is reflected on will
00:12:00
jump here to the left exactly the
00:12:03
same distance and then with transfer,
00:12:05
it will go exactly to .
00:12:08
and so in fact, this is clearly not a transfer
00:12:12
because your 3 passed over, then they
00:12:15
passed into,
00:12:16
but if this is not a transfer, then apparently if that
00:12:19
theory is correct which we will prove,
00:12:20
this should be a reflection, the
00:12:22
question is regarding what point this
00:12:23
will be a reflection if we have it turned out
00:12:26
that the
00:12:28
o and a stroke swapped places, well, the answer
00:12:31
should be clear - this is exactly the
00:12:34
midpoint between these two points. and that
00:12:39
is, this transformation, as it
00:12:42
seems to us, will be a reflection from point a and
00:12:47
how can we calculate this point a if we know,
00:12:50
roughly speaking, the full names and surnames of
00:12:53
these two transformations, the answer is this: we
00:13:03
add a vector to the starting point relative to which the reflection passed with o on which there
00:13:07
was a transfer exactly half as much in the
00:13:10
same direction where the transfer was and
00:13:13
thus it turns out. regarding
00:13:14
which there will be a reflection, this is true, but this
00:13:16
must be strictly proven, of course, but
00:13:19
nevertheless, our guess is correct, so
00:13:22
as an exercise, I suggest that
00:13:25
listeners
00:13:26
swap these two transformations
00:13:28
and make sure that the result will be
00:13:31
different, namely, the result will also be
00:13:34
a reflection but relative to point a the stroke
00:13:38
that is halfway here, that
00:13:42
is, which is obtained by indenting to the left by
00:13:45
half the length of
00:13:46
the vector and, as mathematicians say,
00:13:48
by adding .
00:13:50
minus this vector in half,
00:13:54
so the movement may not be
00:13:56
permutations even in such a simple case
00:13:58
as when we move a straight line,
00:14:01
but nevertheless the arithmetic of the movement can
00:14:04
be constructed, we can even create
00:14:06
such a composition, a table of the composition of
00:14:09
movements where there will be reflection transfers, we will
00:14:11
write down in each case what will happen and
00:14:13
we will do this with you after we prove the
00:14:15
classification premises

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Движение в физике - это процесс, в движение в математике - это результат. Рассматриваем варианты движения прямой в уроке. Курс 100 уроков математики (плейлист обновляется): https://www.youtube.com/playlist?list=PLqBfxn8OBMGrsA_YynaQWqHKhL7kEvL4X =========================== CHILDRENScience - канал некоммерческого фонда "Дети и наука". Наша цель - улучшить качество школьного образования. Для этого мы привлекаем выдающихся учителей, создаем системные курсы из видеоуроков и заданий, готовим методические материалы для преподавателей. Подпишитесь на наш канал: https://www.youtube.com/channel/UCf053FwQD-hnTY7aaaWTaVQ?sub_confirmation=1 Наш сайт - https://classes.childrenscience.ru/seven_grade =========================== Мы в социальных сетях: Facebook - https://www.facebook.com/unsupportedbrowser Instagram - https://www.facebook.com/unsupportedbrowser VKontakte - https://vk.com/childrenscience

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