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From eqn (3104), the vertical channel error dynamics can be represented as 0 1 h h = vn 2 2GM vd 0 vd 2 3

(Re +h) (Re +h)

output Resistances are in ohms Capacitances are in microfarads ( F) Inductances are in microhenrys ( H)

2GM (Re +h)3

Resistances are in ohms Capacitances are in microfarads ( F) if less than 1, and in picofarads (pF) if more than 1 Inductances are in microhenrys ( H)

vn 2 (Re +h)2

Due to the pole with positive real part,

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dition to a tuning control, or resonant circuit that adjusts the output of the amplifier to the operating frequency, there is a loading control that optimizes the signal transfer between the amplifier and the load (usually an antenna) The main drawback of a tuned PA is that the adjustment takes time, and improper adjustment can result in damage to the transistor If the tuning and/or loading controls are out of kilter, the efficiency of the amplifier will be extremely low (sometimes practically zero) while the dc collector or drain power input is high Solid-state devices overheat quickly under these conditions A tuned RF PA, providing a few watts output at 10 MHz or so, is shown in Fig 24-11 The transistor is the same type as for the broadband amplifier discussed previously The tuning and loading controls (left-hand and right-hand variable capacitors, respectively) should be adjusted for maximum RF power output as indicated by an RF wattmeter

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the vertical error dynamics are unstable Some form of feedback error mechanism such as altimeter or GPS aiding is required to stabilize the vertical errors 11512 Lateral Error Channel channel error dynamics can be represented 0 v + 1 0 0 0 1

(1181)

Once you know how amplifiers work, it s easy to understand oscillators All oscillators are amplifiers with positive feedback In radio communications, oscillators generate the waves, or signals, that are ultimately sent over the air Audio-frequency oscillators find applications in such devices as music synthesizers, modems, doorbells, sirens, alarms, and electronic toys

For the discussion to follow, in this simpli ed model, v represents north velocity error, represents latitude error, and represents east tilt error Due to the fact that the error dynamics in this simpli ed model are independent of the position error , this model can be decomposed as v and = 0

Positive Feedback Feedback can be in phase or out of phase For a circuit to oscillate, the feedback must be in phase (positive) Out-of-phase (negative) feedback reduces the gain of an amplifier In fact, negative feedback is used in some amplifiers to prevent oscillation

g 0

1 0 0 1

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The output of a common emitter or common source amplifier is out of phase from the input If you couple the collector to the base through a capacitor, you won t get oscillation It is necessary to reverse the phase in the feedback process in order for oscillation to occur In addition, the amplifier gain must be high, and the coupling from the output to the input must be good The positive feedback path must be easy for a signal to follow Most oscillators are common emitter or common source amplifier circuits with positive feedback The output of a common base or common gate amplifier is in phase with the input But these circuits have limited gain, and it s hard to make them oscillate Common collector and common drain circuits don t have enough gain to make oscillators

(1182)

Feedback at a Single Frequency The frequency of an oscillator is controlled by means of tuned, or resonant, circuits These are usually inductance-capacitance (LC ) or resistance-capacitance (RC ) combinations The LC scheme is common in radio transmitters and receivers; the RC method is more often used in audio work The tuned circuit makes the feedback path easy for a signal to follow at one frequency, but hard to follow at all other frequencies As a result, oscillation takes place at a predictable and stable frequency, determined by the inductance and capacitance, or by the resistance and capacitance

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