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Intermediate frequency amplifier theory of mind

The amplifier is one of the devices in electronics that are used in majorly every device. It is mainly used in devices that need signal amplification like audio, and power signals, etc. According to the output signal, it is categorized into 3 categories. In this article, we are going to discuss the definition , working, diagram , gain, efficiency , classification , etc in detail.

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Intermediate frequency amplifier theory of mind

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WATCH RELATED VIDEO: Module 7: Choice of Intermediate Frequency (IF)

Frequency Response of Amplifiers


If you're seeing this message, it means we're having trouble loading external resources on our website. To log in and use all the features of Khan Academy, please enable JavaScript in your browser. Donate Login Sign up Search for courses, skills, and videos. Science Electrical engineering Amplifiers Operational amplifier.

What is an operational amplifier? Virtual ground - examples. Current timeTotal duration Google Classroom Facebook Twitter. Video transcript - [Voiceover] We're gonna talk about the operational amplifier, or op-amp for short, and this is the workhorse of all analog electronics. The operational amplifier, it's a type of amplifier. An amplifier is anything that you put an electronic signal in, and you get out a larger version of the signal. So this will be an amplifier with some sort of gain, and if I put a signal x in here, usually a voltage or a current, then the signal that comes out here is A times x, and that's what we mean by amplification.

And a signal, that I've shown here as x, is anything that we're interested in, it could be a voltage or a current, and when we put it through an amplifier, we get a larger version of it.

So this is a really common activity in electronic design. Now, when we talk specifically about an operational amplifier, the symbol for that, we use for an operational amplifier, is a triangle. It has two inputs, one is the plus input, one is the minus input, and it has an output, and it also has two power supplies to it.

There's some sort of plus voltage that goes into it, and some sort of minus voltage. So this is the abstract symbol for an op-amp. So when we say the word op-amp, we have some specific properties in mind. One is op-amps have high gain. So in this case, the gain, usually with a symbol A, is something like 10 to the fifth to 10 to the sixth. Really, really high.

Another thing we think about when we talk about op-amps is that they're used for feedback circuits. And we'll talk about feedback in the next couple of videos and what that means, but that's the application that we use op-amps for. And the third that's distinctive about op-amps is that they have this kind of input. This kind of input here is referred to as a differential input.

So an op-amp usually has differential inputs, and that's as opposed to something we call a single-ended input, which will be just one wire. And what a differential input means, it says, we have, we can label the voltages here. We'll call this v out, we'll call this v plus, and we'll call this input v minus. And differential input means that v out equals the gain times v plus minus v minus.

So the output signal here is proportional to the difference in the voltage between these two signals here. So I wanna make a plot of this equation right here, just so we get a good idea of what it looks like.

And the axis here are v in and v out, where v in specifically equals v plus minus v minus. So that'll look like this, something like this, it's gonna be a very steep line, and the slope of that line, the slope of this line is A. So the slope is going to be 10 to the fifth or 10 to the sixth, something like that, very, very vertical. Now one of the properties of this is that v out cannot go above or below its power supply voltages.

So on this plot here, that's called saturation. If v out gets up to V plus, we say it saturates. It looks like this, it goes flat basically here and here, where this voltage value here is minus the power supply, and this voltage right here is the positive power supply. But over this range here, over this range in here between those two points, is quite linear. It goes through zero, and this is where we use it most of the time.

So now I wanna talk a little bit more detail about what this symbol means here and what's inside it, and how it's actually connected up in a circuit. So we talked about the voltage behavior of an op-amp. This is v plus, v minus, and v out. There's one thing more that we need to know, and that is the current, this current right here and this current right here, for an op-amp, an ideal op-amp, is zero, no current flows in here. So this op-amp is just sensing the voltages at these points but no current flows in.

So this is the second key property of an op-amp. The first one is the voltage behavior, v out equals the gain times v plus minus v minus. Another way we can write this is v out equals A times v in, where v in, of course, equals v plus minus v minus. So these are the two electrical properties that are gonna allow us to analyze these circuits.

Analyzing these circuits is actually gonna be pretty simple. So you're probably wondering, what is inside here, what's going on inside here? So what's inside here is, somewhere between 20 and 50 or so transistors and resistors, sometimes capacitors. These are really complex designs, and for right now, if we just concentrate on the two properties that we have here, we'll be able to use these circuits even without understanding exactly what's inside.

Suffice to say it's a differential amplifier with really high gain, and with just that knowledge, we can work out how these circuits work. So let me do a couple of more details on how this thing is actually hooked up. So we have a plus terminal and a minus terminal.

There's more terminals on this, there's a power supply like this, that's plus big V, and there has to be a minus supply, typically a minus supply, minus V, and there'll be a ground pin, there'll be a ground node on here, like that.

And when this is used in a circuit, there'll be, over to the side, there'll be two power supplies, and this will be 12 volts, 12 volts is a real typical value, and there'll be another one, and this is a plus 12 volts supply as well, and they'll be connected together, and this node right between them will be the ground node, that's the voltage reference, and these two guys will be hooked up like that, the two power supplies will be hooked up this way.

So, with respect to ground, this node is at minus 12 volts and this node from ground is at plus 12 volts. And ground is right in the middle. And when we measure v out, we'll measure it with respect to this ground node. So this is the voltage where we measure plus or minus v out right there.

And what we're gonna do is we're gonna assume that all of this stuff is always hooked up, and we're just gonna use an even simpler symbol, just the three terminals like that, and you'll know that all of the rest of the power supply's hooked up that way.

And the thing to keep in mind is there's a large minus voltage, there's a large plus voltage, and the ground level, the ground node, is right in between, so positive voltage is high on the page, negative voltage is low on the page, and v out can go both positive and negative around ground.

So that's your voltage framework to keep in your head. And the op-amp that we've been looking at has a symbol like this, and we know that v out equals some huge gain times v plus minus v minus, so this is a differential input, here's v plus, here's v minus.

One way I think about this is to look at the way a change in voltage on the input modifies the output. Let me label v out here. So, if there's a change on the input, say v plus goes this way, because it's a plus sign, that means that v out goes this way. Now, if I change it over to v minus, v minus is on the negative input. If v minus goes up, then v out goes down, so that's the inverting, it's called the inverting input, and this is called the non-inverting input. So on a non-inverting input, up goes up, and on the inverting input, if you go up on the inverting input, you go in the opposite direction on the output.

Let's say that the positive input, the non-inverting input, went down this time, and that means what? That means that v out will go down, and just do the same thing over here, gonna run out of colors. Let's do the same thing for the inverting input. If the inverting input goes down, what does the output do?

It goes up, it goes in the opposite direction. That's the way to think about this symbol when you see it on a schematic page, is how do these signals translate through the device? Positive, non-inverting signals go in the same direction, inverting signals go in the opposite directions. Okay, and here's one final trick I wanna share with you, something to be aware of. You're gonna see a symbol like this on a page, the same op-amp. It's the same op-amp, but it's written on the page with the negative, with the inverting symbol on the top and the non-inverting symbol on the bottom.

So, as you look at a schematic that has an op-amp in it, one of the first things you wanna do is just glance and see what order these symbols are in.

Does it look like that or does it look like that? And keep that in mind as you're reading the circuit and trying to understand what it does. Okay, let's move on and build something with our op-amp. Non-inverting op-amp. Up Next.


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The characteristics of a wideband power amplifier are evaluated by its ability to achieve maximum power Broadband Matching, Microwave and RF Design: Networks Vol. The simulated return and insertion losses of the transformer are shown in Fig. The performance of the balun is simulated, and the results are: the single port power loss port-to-port conversion loss is less than 7 dB. Usually, it relates to the circuit gain or if the device calls for single or multiple microphones.

The AD is a complete IF limiting amplifier, providing both This is a stress rating only; functional operation of the.

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Guide to the study of. Read the Instructions to know how you can better use this work. Know how it is organized and which navigation tools are available. See how you can complement the study with the simulation of some of the circuits presented here. See the table of contents of this work. The table is organized through a pop down menu revealed when you place the cursor over the titles. Through the Index you can directly access each one of the sections and exercises of this work. The main text of this work is enhanced with several complementary texts, in order to help the reader about matters not directly studied here. These are matters which are supposed to be studied before or later. Through the main text there are several links to these texts but you can also access them through the table of Annexes, organized in a similar way as the main Index.

What is an operational amplifier?

intermediate frequency amplifier theory of mind

Amplifiers are one of those critical components that make modern life possible. From wireless communication to power electronics, amplifiers need to run stably and predictably for these products to work properly. Stability analysis is one of my favorite topics in physics and engineering, and it always tends to crop up in places you would least expect. One of these places is in amplifiers.

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RUPPL] 3,, A parametric amplifier broadly comprises a variable reactor or varactor in the form of a variable-capacitance diode, positioned in a resonant cavity provided with tuning means. An ultrahigh-frequency input signal to be amplified is coupled to the cavity so that the resulting variable electric field tends to vary the capacitance of the varactor at the input signal frequency.

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In electronics , frequency response is the quantitative measure of the output spectrum of a system or device in response to a stimulus, and is used to characterize the dynamics of the system. It is a measure of magnitude and phase of the output as a function of frequency , in comparison to the input. For a linear system , doubling the amplitude of the input will double the amplitude of the output, and summing two inputs produces an output that is the sum of the two corresponding outputs to the individual inputs. In addition, if the system is time-invariant so LTI , then the frequency response also will not vary with time, and injecting a sine wave into the system at a given frequency will make the system respond at that same frequency with a certain magnitude and a certain phase angle relative to the input. Thus for LTI systems, the frequency response can be seen as applying the system's transfer function to a purely imaginary number argument representing the frequency of the sinusoidal excitation.

As such for any electronic circuit, the behavior of amplifiers is affected by the frequency of the signal on their input terminal. This characteristic is known as the frequency response.

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Search Products:. Having a a gain factor of about 45, a 12AY7 has less gain than a 12AX7, which has a gain factor of about Pull out the V1 normal channel preamp tube — More preamp gain in vibrato channel. The voltage gains are thus Amplification factor is , which is highest of all audio triodes. The 12AT7 is a tube with gain factor

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