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The Class A Amplifier With the previously mentioned component values, the amplifier circuits in Figs 24-1 and 24-2 operate in class A This type of amplifier is linear, meaning that the output waveform has the same shape as (although a much greater amplitude than) the input waveform For class A operation with a bipolar transistor, the bias must be such that, with no signal input, the device is near the middle of the straight-line portion of the IC versus IB (collector current versus base current) curve This is shown for an NPN transistor in Fig 24-3 For PNP, reverse the polarity signs With a JFET or MOSFET, the bias must be such that, with no signal input, the device is near the middle of the straight-line part of the ID versus EG (drain current versus gate voltage) curve This is shown in Fig 24-4 for an N-channel JFET For P channel, reverse the polarity signs In a class A amplifier, it is important that the input signal not be too strong An excessively strong input signal will drive the device out of the straight-line part of the characteristic curve during part of the cycle When this occurs, the output waveshape will not be a faithful reproduction of the input waveshape, and the amplifier will become nonlinear Class A amplifiers are supposed to operate in a linear fashion at all times The Class AB Amplifier Class A operation is inefficient because the transistor draws current whether there is a signal input or not For weak-signal work, efficiency is not too critical; the things that matter are the gain and

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(1153)

CHAPTER 11 AIDED INERTIAL NAVIGATION The direction cosine matrix is computed by integration of Rn b b b = Rn ib in b (1154)

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the sensitivity In power amplifiers, efficiency is more important, and gain and sensitivity don t matter as much When a bipolar transistor is biased close to cutoff under no-signal conditions, or when an FET is near pinchoff, the input signal always drives the device into the nonlinear part of the operating curve Typical bias zones for class AB are shown in Figs 24-3 and 24-4 A small collector or drain current flows when there is no input, but it is less than the no-signal current that flows in a class A amplifier This is called class AB operation It s more efficient than class A, but the gain and sensitivity are not as high There are two modes of class AB amplification If the bipolar transistor or FET is never driven into cutoff/pinchoff during any part of the signal cycle, the amplifier is working in class AB1 If the device goes into cutoff pinchoff for any part of the cycle (up to almost half ), the amplifier is working in class AB2 In a class AB amplifier, the output signal waveform is not identical with the input signal waveform But if the signal wave is modulated, such as in a voice radio transmitter, the waveform of the modulating signal comes out undistorted anyway Thus, class AB operation is useful in RF power amplifiers

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ib in where = [ ], b is de ned in eqn (1149), b = Rb n , and n in N in n = E = D + ie cos( ) + ie sin( ) (1155)

Navigation error arises due to initial condition error and the accumulation of instrumentation errors through the integration process The purpose of this section is to derive a state space model for the navigation error vector This section focuses on model development for the geographic frame mechanization approach as de ned in Section 113 The model developed in this section will have the form p Fpp v = Fvp F p Fpv Fvv F v 0 p Fp Fv v + Rn b F 0 0 0 Rn

(1156) The error vector is de ned as x = [ p, v, ] , where p = [ , , h] (1157) (1158) (1159)

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