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#1
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Hi,
I am looking for some help in understanding amplifier concepts (solid state only) and product specifications. I have searched for definitions and essays on the topic, but , having no electronics exposure, I find it hard to understand the concepts clearly. So if someone can please help: 1. What actually is amplification of a RF signal: is it the scaling up of the amplitude? I want to amplify a signal where the output has very low distortion and noise. It should be as close to the input signal as possible: 2. Does push-pull setup mean that it's a class AB amplifier in which two amplifiers amplify the same signal, but the opposite two halves of the input signal? If this is true, in an amplifier like this: http://www.communication-concepts.com/ar347.htm If two solid state amplifiers are rated at 600W each, and it's a push- pull arrangement, how come the output of this amplifier is 1000 watts (or 1.2 kw theoretically) If one Motorola amplifier is amplifying half the signal, the other amplifying the other half, wouldn't the total output be 600W for the whole signal? 3. In class AB amplifiers, is the output signal an exact replica (but amplified) version of the input signal? 4. What is an octave when dealing with amplifiers? 5. Is this communication concepts HF 1000 watt amplifier a class A, class AB, or class C amplifier? http://www.communication-concepts.com/ar347.htm 6. Does anyone know the detailed specs for this same communication- concepts 1000 watt HF amplifier? Specs like: a. Duty cycle b. Phase stability c. Phase change with power d. Gain flatness e. Pulse droop f. Harmonics g. Spurious h. Rise/fall times i. VSWR or load SWR j. Gate delay 7 Can this amplifier be "controlled" to give graded amplification less than 1000 watts specified, or will it work only at this maximum level? Any help is appreciated. Thanks Vijay |
#3
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I like Tim;s explanation, but since it isn't real clear where you are
heading, there are a couple other points I'd like to make. "Tim Wescott" wrote in message ... wrote: [ BIG CLIP ] In electronics, amplification of _any_ signal is it's scaling up in amplitude or power. Understand that theoretically, increasing the amplitude increases the power. The reality, especially with RF, and especially with solid state amplifiers, is not quite so simple. In order to transfer power from one RF stage to another, or from an output stage to an antenna, we need to match the input impedance of the following stage with the output impedance of the preceding stage. If the impedances don't match, not all the power will be transferred, and the portion that is transferred is likely to be distorted, perhaps badly. I turns out that the output impedance of a solid state amplifier is dependent on the output power, with higher power implying a lower impedance -- often quite low. Generally, our antennas, and most larger scale modules, have, by convention, a 50 ohm impedance. (Internal stages often do as well, but there is no reason a designer might not pick something else 'inside the box'). Normal practice is to follow the amplifier with a matching network (typically still inside the amplifier box, however), so that the amp you buy has a 50 ohm impedance output. This matching network actually distorts the signal, really, deliberately. The result is what we want for a typical RF amplifier application. Your question sounds a bit as if you might not be interested in the "typical" RF application, so the typical answers might not be quite what you are looking for. [ANOTHER BIG CLIP] We wish. Ideally, yes that is the case. Practically the output signal will be filtered, delayed, and distorted but not too much. And again, this linearity is right for typical applications, but again, for TYPICAL applications. Obviously, if an amplifier produces 1000 watts out with 100 watts drive, and it is linear, it will produce 500 watts out with 50 watts drive. But if you give it one watt drive, it might not produce 10 watts, and what it does produce might be quite distorted and masked with noise or other artifacts. Again, within reasonable limits, in typical applications, these things behave as you would expect. But in some odd application, or at the liimits of their useable range, the results might not be close enough to theoretical to satisfy you. The same is true if your input waveform is not what one would expect. For communications service, the expected waveform is really quite predictable, and the design of the impedance matching circuits makes assumptions about these waveforms. If your input waveform is far from what would be expected, then you might experience a lot of distortion of the input waveform, even though a non-critical look appears to be within the operating range. For example, if you were to drive that amp with a 50 MHz square wave, the output waveform would probably look more like a sine wave than a square wave. ... |
#4
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Thank you guys for the detailed explanations. The underlying concepts
are much clearer now vij |
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