Basic Radio is a free introductory textbook on electronics based on tubes. See the editorial for more information.... |
![]() |
Home ![]() ![]() ![]() |
||||
See also: Harmonic Distortion versus Feedback Voltage | ||||
![]() ![]() ![]() ![]() ![]() ![]() ![]() |
||||
Distortion in Class A AmplifiersAuthor: J.B. Hoag
As already pointed out, the output wave-form of Class A amplifiers is the same as the input wave-form. In order that this be true, they must be operated strictly as linear devices, over a straight-line characteristic curve. It should be obvious from the preceding section that distortion will occur in Class A amplifiers if the input signal voltage is so great that the upper and/or lower knee of the characteristic curve comes into use. Referring to Fig. 12 B, it can be seen that a longer straight curve is to be had when the plate voltages on a given tube are greater. For this reason, the successive stages in a Class A amplifier sometimes use higher and higher plate voltages and correspondingly greater and greater grid voltages. It was shown in Sec. 12.3 that the dynamic curves of a tube are straighter over a greater range of grid voltages (and also have smaller slopes) than the static curves, especially when the plate circuit resistance is large. This means that voltage amplification is sacrificed in order to prevent distortion. Thus larger plate circuit resistances are used to reduce distortion in Class A amplifiers.
When properly operated, Class A amplifiers are characterized by low power output for a given size of tube, by small distortion compared with Class B or C amplifiers, by high power amplification and by low plate efficiency (20 to 35 percent).
|
||||
Home ![]() ![]() ![]() |