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Download "Использование Выпрямителя (Транзистор это просто 34)"

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выпрямитель
транзистор
полупроводник
уроки электроники
электроника для чайников
электроника
радиоэлементы
электричество
схема
электрические схемы
Выбор рабочей точки
радиотехника
радиоэлектроника
основы электроники
электроника своими руками
радиолюбитель
в помощь радиолюбителю
школа радиолюбителя
схемы радиолюбителей
для начинающих радиолюбителей
книги по радиоэлектронике
уроки радиоэлектроники
лекции по электронике
начинающий радиолюбитель
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  • ruRussian
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00:00:04
I believe that with the knowledge I have acquired
00:00:06
in the field of low frequencies, I can
00:00:08
now calculate all the elements of transistor amplifiers,
00:00:11
I have always admired your modesty, I
00:00:14
am not being ironic in this area, everything is simple and
00:00:16
clear when it comes to transformer
00:00:19
coupling, then I will finish reading the ratio of the numbers of
00:00:21
turns that gives the best matching of
00:00:23
cascades and believe me, extracting the
00:00:26
square root will not scare me, if
00:00:28
the question arises of a rheostat on capacitive
00:00:30
connections, then didn’t you study me
00:00:33
to determine the load straight line, I will
00:00:35
draw it in such a way that, being a tangent
00:00:37
hyperbola of the permissible power, it
00:00:39
will allow us to have the greatest amplitude of
00:00:41
signals at the output because the operating
00:00:43
point will be located in the middle, at the risk of
00:00:46
upsetting you, I must say that the
00:00:47
situation is not so simple at first
00:00:49
glance, you are right, but when calculating amplifiers,
00:00:51
you must also take into account the available
00:00:53
power band during the course, we will strengthen their frequencies, the
00:00:56
role of feedback, the permissible
00:00:58
distortion factor, and a host of other
00:01:01
circumstances, it’s enough to bombard me with
00:01:03
these requirements, I admit that
00:01:05
I sinned from an excess of naive pride and
00:01:07
nevertheless the matter looks quite
00:01:09
simple when we resort to the help of a
00:01:10
family of characteristics and the load
00:01:12
straight line, our input signal signal can be
00:01:15
considered as both voltage and current has the
00:01:17
right to occupy a part of the load straight line
00:01:20
limited by two points on one
00:01:22
side. I then begin to bend
00:01:24
characteristics a with another point b at
00:01:27
which the base current approaches zero, which,
00:01:29
as you know, is the cause of
00:01:31
nonlinear distortions,
00:01:32
undoubtedly, therefore the operating point p must be
00:01:35
chosen at an equal distance. for in this
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case the maximum amplitude of the input
00:01:39
signal will be p or pb, or rather the
00:01:43
difference between the corresponding
00:01:44
values ​​of the base current or base voltage
00:01:47
in my figure, this amplitude has a
00:01:49
value of the order of 200 75 millivolts, it
00:01:53
changes the collector current from 7 to 57 miles
00:01:55
amperes with an average current value of
00:01:58
32 milliamps. that is, the amplitude is 25
00:02:01
milliamps
00:02:03
wonderfully dislikes I hope that you are
00:02:04
completely satisfied that the operation of
00:02:06
your transistor is not quite as good as
00:02:09
everything goes well with a large signal,
00:02:11
just as much as I despair of the
00:02:14
exorbitant energy consumption with weak
00:02:15
signals or in the absence of an amplified
00:02:18
signal, whatever the amplitude of the
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current consumption it always
00:02:22
corresponds equally to point p a video of weak
00:02:25
signals, the operating point could be
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moved lower to another load
00:02:29
line corresponding to a lower current,
00:02:31
for example, to the point along the line, as a result,
00:02:33
energy consumption would be reduced and we
00:02:35
would save on batteries, which are
00:02:37
quite expensive, you want to
00:02:39
ruin the manufacturing companies no, but I
00:02:41
believe that when listening to a symphony, it is irrational
00:02:43
to use during pianissimo the same
00:02:45
power that is required by the moments of playing of the
00:02:47
entire orchestra; however, I do not see how it would be possible to
00:02:50
force the operating
00:02:52
point to move to the lower load
00:02:54
line in order to expend only the power
00:02:56
strictly necessary to reproduce
00:02:58
signals of different magnitudes without distortion.
00:03:00
avoiding waste
00:03:02
is commendable therefore I will gladly show you the
00:03:04
appropriate means so that your
00:03:06
operating point can move from one
00:03:08
load line to another you need to
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change the bias voltage it must
00:03:12
increase with the amplitude of the signal and it
00:03:14
must be the signal itself since the signal
00:03:16
is alternating current lighting is constant
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you know an excellent means for
00:03:21
converting alternating current into
00:03:22
direct current, this is the rectifier that
00:03:25
is used to obtain an alternating
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bias, here is a practical circuit of an
00:03:28
amplifier with a floating operating point, you
00:03:31
see that the amplified signals taken from the
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additional winding on the output
00:03:34
transformer are
00:03:35
rectified using a
00:03:36
semiconductor diode d they create a
00:03:40
voltage drop at the resistance outputs r which makes point x a more
00:03:43
or less negative capacitor c
00:03:45
heal the ripples of the rectified
00:03:47
voltage are also increased corresponds to the
00:03:49
average value of the amplified signal
00:03:51
up to this reminds me of the aru system there we
00:03:54
also met a capacitor which,
00:03:56
together with the resistance, gave the
00:03:58
aru system inertia to a flywheel-like
00:04:00
regulator, the comparison is very successful although
00:04:03
our device does not resemble as much as a
00:04:04
conventional ara as an ara working
00:04:07
inside out; here, too, the amplitudes of changes in the
00:04:09
amplified voltages are rectified, after
00:04:12
which they are used to control the
00:04:13
bias at the input; indeed, at the
00:04:15
beach, not at point x,
00:04:17
the resistance r2 and r3 are applied to a common point, which
00:04:20
connects the base to the negative pole of the
00:04:22
power source; the correct choice of the
00:04:24
values ​​of 3 resistances allows you
00:04:26
to make the bias proportional to the
00:04:28
amplitude of the signals, so the base
00:04:30
here becomes more negative
00:04:32
the stronger the signal, and but unlike the
00:04:34
familiar aru tube receivers,
00:04:37
increasing the negative bias in the
00:04:39
base circuit of the pnp structure transistor does
00:04:41
not close it, but opens it even more; it
00:04:44
increases the base and collector currents of your
00:04:46
circuit with a floating point bias, I
00:04:48
really like it. When I assemble
00:04:50
my receiver using transistors, I will
00:04:51
certainly install a beautiful
00:04:53
push-pull cascade at the output with this device
00:04:55
giving sliding bias voltage in a
00:04:58
push-pull circuit. My dear dislikes
00:05:00
can be done better, but more about this next
00:05:02
time, watch the continuation and
00:05:04
subscribe to our channel so you don't
00:05:06
miss new episodes

Description:

Выбор рабочей точки транзистора. Экономичная схема с плавающей рабочей точкой. Применение выпрямителей. _______________________________________________ Смотрите наши видео, в которых мы простым языком рассказываем о радиотехнике, электронике и радиоэлектронике! Наши уроки будут особенно полезны для начинающих радиолюбителей и студентов радиотехнических ВУЗов. В видеороликах мы даём основы электроники: определения, описания, схемы и принцип работы различных элементов радиотехники. В наших видео вы узнаете: что такое транзистор, диод, конденсатор, резистор, микросхема, электрический ток и много других разных интересных вещей и явлений, связанных с электроникой.

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