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  • ruRussian
Download
00:00:02
of course, well known to all
00:00:04
professional designers of
00:00:05
radio electronics equipment and
00:00:07
experienced amateurs, they are also
00:00:09
well known and understandable, but for many
00:00:11
beginning radio amateurs and just people
00:00:13
interested in circuitry and
00:00:15
radio engineering, these words are not entirely
00:00:18
clear or completely incomprehensible, despite the fact
00:00:20
that they occur very often
00:00:21
in practice always,
00:00:23
as soon as we talk about radius spring
00:00:25
equipment, especially for radio receivers,
00:00:28
in this video we will try to
00:00:29
talk as firmly as possible about what a
00:00:32
superheterodyne is and how it works
00:00:35
[music]
00:00:39
hello everyone, basically the word su accept
00:00:43
for the sake of assigns this type of this type of
00:00:45
radio receiver device of a radio receiver
00:00:47
this architecture receiver circuits to
00:00:51
understand better how it works, why such an
00:00:53
architecture is needed at all,
00:00:54
let's first remember what a
00:00:56
radio receiver is in general, a radio receiver is a
00:00:58
device that performs three main
00:01:01
functions, amplification, filtering or
00:01:04
modulation, the
00:01:06
first radio receivers, the first receiving
00:01:08
devices were detectors, we
00:01:10
practically did not perform any amplification
00:01:12
due to their power supplies
00:01:15
While we won’t consider it, let’s
00:01:17
move on immediately to the next one for the sake of
00:01:19
the receiver that appeared later, these are
00:01:21
direct amplification receivers.
00:01:22
Actually, after them,
00:01:25
super local oscillators appeared, we can say why
00:01:27
they appeared. In an hour, it will become clear to us from
00:01:30
the features of the work, from the shortcomings of
00:01:32
this very feature of the operation of
00:01:35
direct amplification receivers,
00:01:36
as follows from its names
00:01:39
direct amplification receiver directly amplifies the signal,
00:01:42
that is, directly amplify the signal
00:01:45
received by the radio station, they do
00:01:47
not transform anything with it except
00:01:49
naturally demodulation, that is,
00:01:50
detection, that is, the received
00:01:53
signal, the useful signal of the radio station
00:01:56
is amplified directly at the frequency
00:01:58
at which the transmitting station is broadcasting, this is how
00:02:01
direct amplification receivers work
00:02:02
to make it easier understand, let's
00:02:04
look at an example using the example of a
00:02:06
receiver that receives a broadcast
00:02:09
signal in medium waves, broadcasts in the
00:02:11
range among the shaft, the new broadcast
00:02:13
range has a frequency overlap of
00:02:15
approximately equal to three, that is, from 500
00:02:18
kilohertz to 1600, that is, three times
00:02:21
the frequency changes the lowest purity
00:02:23
is less than the highest frequencies of this
00:02:25
range is about 3 times so the receiver,
00:02:28
in order to receive a signal from one station
00:02:30
somewhere in this frequency range, must
00:02:33
isolate the signal of this particular station
00:02:35
using certain filters that all other
00:02:38
signals from other stations it did not receive us,
00:02:40
amplify this signal or modulate in the
00:02:42
case of a medium crowbar broadcasting, that is,
00:02:45
to perform amplitude detection,
00:02:47
so it turns out that in such receivers,
00:02:50
the filter that selects our useful
00:02:52
signal must be tuned in frequency
00:02:54
from 500 kilohertz to 1600, that is, this
00:02:58
filter must be tuned over the entire
00:03:00
range, while the filter must
00:03:01
retain its other parameters
00:03:04
except the main frequency except
00:03:06
resonance frequency, so to speak,
00:03:09
that is, it must preserve the
00:03:11
passband, it must maintain the
00:03:12
transmission coefficient, this filter, if an
00:03:14
example from the filter is installed at the input of the
00:03:16
receiver, naturally
00:03:18
it consists of some kind of oscillatory circuits,
00:03:21
one or more. We are now
00:03:22
talking to you about the simplest
00:03:24
receivers that were around a long time ago at the beginning of the
00:03:27
last century, naturally, they had
00:03:29
filters on the circuits
00:03:30
and no filters were made on any other elements,
00:03:33
this filter,
00:03:34
if it consists of two circuits,
00:03:37
these two circuits must be
00:03:39
simultaneously synchronized, that is, there must
00:03:40
be a dual variable capacitor
00:03:42
if three The circuit filter consists of three
00:03:44
variable capacitors that must be
00:03:46
rebuilt. In principle, it is not difficult
00:03:47
to make a
00:03:48
double or slender
00:03:50
variable capacitor, but it is quite difficult to provide
00:03:52
all the other parameters of this filter over the
00:03:55
entire range, that is,
00:03:57
if we have this filter we will
00:03:59
pass some kind of band at a frequency of
00:04:01
500 kilohertz that when it is rebuilt with
00:04:03
only control capacitors at a
00:04:05
frequency of 1600 kilohertz, the passband of
00:04:08
this filter will change very much, and the
00:04:12
transmission coefficient of this filter will also change significantly;
00:04:14
moreover, the amplifier following the filter,
00:04:17
which will amplify the signal received and
00:04:19
the radio station, it will also be forced to
00:04:21
amplify in one case the signal
00:04:23
of the radio station to those broadcasting at a frequency of 500
00:04:25
kilohertz, and in another case, the signal of the
00:04:26
broadcasting station is not counted and the 1600
00:04:29
congress is different three times and
00:04:31
most likely the gain of this
00:04:33
amplifier will also be different for these
00:04:35
frequencies since the amplification elements
00:04:37
they always have
00:04:38
non-linear amplitude-frequency
00:04:40
characteristics do the amplifier is
00:04:41
quite complex, especially in those days
00:04:43
when
00:04:44
radio engineering was just emerging; receiver circuitry;
00:04:47
receiving
00:04:48
amplification elements; these
00:04:50
were naturally vacuum devices, that is,
00:04:51
radio tubes,
00:04:52
and they were, so to speak, very
00:04:55
frequency-dependent elements;
00:05:00
gain than at a frequency of
00:05:03
1600 kVA Hertz, and if the receiver had to
00:05:05
cover not only medium
00:05:07
waves but also short waves, for example, then even
00:05:08
more so at a frequency of 5 megahertz or three,
00:05:12
this receiver, or rather this amplifier on the
00:05:15
lamp had even less gain, that is, it
00:05:18
turns out that direct
00:05:20
amplification receiver there are several problems that
00:05:22
urs decide to eliminate without changing
00:05:24
the architecture of this receiver, it is almost
00:05:26
impossible or very difficult; moreover,
00:05:28
there is another problem that I did not
00:05:30
tell you, this is actually providing a narrow
00:05:33
bandwidth, that is, if the receiver
00:05:35
must provide bandwidth with a
00:05:38
width of, for example, 10 kilohertz
00:05:40
in the mid-wave range, it is very difficult to achieve
00:05:43
such a narrow bandwidth
00:05:45
using a double-loop filter at the
00:05:47
receiver input, especially at the
00:05:50
upper frequency range, and if this
00:05:52
receiver is also short-wave and
00:05:53
operates at frequencies of 3-5-10 megahertz, then
00:05:56
using a conventional double-loop or 3-
00:05:58
loop filter we rebuild it
00:06:00
naturally, such a narrow band
00:06:01
cannot be achieved at all, so in order to
00:06:04
solve all these problems, a superheterodyne was invented,
00:06:06
how world
00:06:08
radio engineering science came to this
00:06:10
idea, I won’t talk about this topic of a
00:06:12
separate conversation, I’ll talk about how
00:06:14
it works to solve all these
00:06:16
problems, super pour for the sake of
00:06:19
the signal that is not received is transferred along the spectrum to another
00:06:21
frequency, often called
00:06:23
intermediate;
00:06:25
all the main amplification,
00:06:27
filtering or modulation actually takes place on it,
00:06:29
that is, we can say that a
00:06:31
superheterodyne receiver is a receiver
00:06:33
for 1 virgin purity;
00:06:35
direct amplification receiver at one frequency, which is
00:06:38
called intermediate frequency;
00:06:40
everything happens on it the main gain is
00:06:43
filtering, as I already said, and before this
00:06:45
direct amplification receiver, which
00:06:47
operates at one single frequency
00:06:49
without tuning without any, and at this
00:06:51
frequency a filter is made that
00:06:53
provides a narrow passband,
00:06:55
the filter is made with optimal parameters
00:06:57
precisely for this frequency, the
00:06:59
amplifier in this
00:07:01
receiver is never tuned it is also made with optimal
00:07:03
parameters specifically for this frequency and the
00:07:05
frequency never changes, so the
00:07:07
amplifier always works on it. Before
00:07:10
this direct amplification receiver, a
00:07:11
converter is turned on that transfers the
00:07:13
spectrum from any part of the range to this
00:07:16
very frequency to the intermediate frequency,
00:07:19
this is all called a superheterodyne, so what about
00:07:22
reception? there is a transfer of the spectrum from the
00:07:25
frequency that emits the transmissions
00:07:28
that we receive
00:07:29
from the air using a receiving antenna to the
00:07:31
frequency at which the
00:07:33
main filtering amplification takes place, that is,
00:07:35
to intermediate states it happens
00:07:37
precisely with the help of a local generator
00:07:40
built-in generator in the receiver, this
00:07:42
generator is called a local oscillator and that’s it
00:07:45
where tier-1 generates a certain
00:07:47
high-frequency signal which is naturally not
00:07:49
equal to the received frequency of the receiver, and
00:07:51
this high-frequency
00:07:53
generator signal is mixed with the useful
00:07:56
signal that comes from the antenna, the
00:07:57
signal of the radio station that we want to
00:08:00
receive, as a result of mixing these
00:08:03
two signals, a third signal appears
00:08:05
equal to the intermediate frequency, which is
00:08:08
actually already and is amplified further in
00:08:10
this receiver, this is how a
00:08:11
superheterodyne works, it can be super, of course,
00:08:14
where I’m looking for one with two stirrup
00:08:15
transformations,
00:08:16
that is, this whole scheme with transfer of the
00:08:19
amplification and filtering spectrum simply
00:08:21
happens several times, first at one
00:08:23
frequency, brings the spectrum amplified,
00:08:24
filtered, then transferred again to
00:08:27
another with the help of another local oscillator
00:08:28
can be later and on the third the essence does
00:08:31
not change from this, that is, a
00:08:32
superheterodyne receiver and such a
00:08:34
receiver in which the spectrum of the
00:08:37
useful signal from the air is transferred using a
00:08:39
mixer and a local oscillator
00:08:41
to an intermediate frequency, amplification occurs on it,
00:08:45
frequency tuning of such a receiver is already happening
00:08:47
not the restructuring of narrow-band filters
00:08:49
that provide the main filtering
00:08:53
in this receiver, but occurs due to the
00:08:54
frequency tuning of the local oscillator, that
00:08:57
is, the high-frequency generator 1 liter
00:09:00
1 is much easier to tune in frequency
00:09:02
than some complex multi-circuit
00:09:04
filter, especially as we know in
00:09:06
more modern in receivers,
00:09:08
multi-circuit filters are used,
00:09:09
quartz filters mf and a play filter are used, they
00:09:12
cannot be tuned in
00:09:13
frequency at all,
00:09:14
they are tuned to one of their own frequencies,
00:09:17
they have their own bandwidth and you
00:09:19
can’t influence it in any way,
00:09:22
so in order to rebuild the receiver with such a
00:09:24
filter, they rebuild it by frequency a
00:09:26
built-in generator called
00:09:28
a local oscillator, this local oscillator naturally in
00:09:30
modern receivers is already a
00:09:32
frequency synthesizer that has
00:09:35
great stability, but before it was
00:09:37
just a smoothly tuning generator
00:09:39
with a variable capacitor,
00:09:42
which by changing its capacitance changed the
00:09:44
resonant frequency of the circuit in this
00:09:46
generators, the generator
00:09:48
produced a signal of different frequencies, therefore
00:09:51
it turns out that in super heterodyne
00:09:53
receivers, the main filtering
00:09:56
takes place at the intermediate frequency; the
00:09:58
intermediate frequency does not change; it is
00:10:00
fixed; the filter of
00:10:02
this basic filtering itself, the main
00:10:04
selection, works at one frequency, will
00:10:05
provide one bandwidth; the
00:10:08
intermediate frequency amplifier also
00:10:10
always works at the same frequency and
00:10:12
no matter what frequency of
00:10:15
the range working we accept, the
00:10:18
bandwidth of the
00:10:19
receiver does not change; moreover, choosing a
00:10:22
suitable intermediate state that is convenient for us,
00:10:25
but we may not be able to provide the bandwidth we need,
00:10:27
for example, a receiver with a
00:10:29
frequency of 15 megahertz, it is quite difficult to make direct
00:10:32
amplification with a bandwidth of
00:10:34
10 kilohertz, that is, at
00:10:37
15
00:10:38
megahertz frequency, make a filter out of the circuits
00:10:41
that would provide a
00:10:43
passband of 10 kilohertz, the complexity of the
00:10:45
circuits will be a lot of filters, and
00:10:47
setting them up together is
00:10:49
also very difficult, so just to
00:10:51
prevent zeal, this problem is also
00:10:53
solved by transferring the spectrum to the region of the
00:10:56
river, it often happens 455 kilohertz, 465
00:11:00
sometimes 500 kilohertz in general Usually this is
00:11:03
hundreds of kilohertz and at this frequency it is convenient to
00:11:06
provide just amplification and filtering. I
00:11:11
probably couldn’t tell you very briefly about this. Moreover, there are
00:11:14
many other features of the operation of
00:11:15
this superheterodyne receiver, there are
00:11:18
mirror reception channels, there is a reception channel,
00:11:21
parasitic side effects on
00:11:24
local oscillator harmonics, and so on. similar things in
00:11:25
general, a superheterodyne receiver has many different problems,
00:11:27
but
00:11:30
I think this should be talked about separately
00:11:32
for now, my story about the work
00:11:34
soup to love the homeland receiver is finished
00:11:36
thank you for watching this video study
00:11:39
radio engineering circuit design design
00:11:41
listen to the broadcast
00:11:42
watch my video subscribe to the
00:11:44
channel on the VKontakte group facebook
00:11:46
Alexey Igonin was here, bye everyone

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Видео рассказ о том, что такое супергетеродинный приёмник, чем он отличается от приёмника прямого усиления. Видео может быть интересно для людей, начинающих изучать радиотехнику и электронику. Спасибо за просмотры и подписку! Для помощи каналу и благодарностей: ЯндекДеньги: 410017381931812 PayPal: [email protected] Пишите комментарии, подписывайтесь на мой канал, не пропустите новые видеоролики. Группа ВКонтакте: https://vk.com/igoninalexey Instagram: https://www.instagram.com/hamradio_from_russia/ Facebook: https://www.facebook.com/groups/savage19nnn/ Яндекс ZEN: https://dzen.ru/savage19

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