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under certain special conditions described below Since it is not practical to include and explain many di erent simulated scenarios, the main objective of this section is to illustrate the methodology and to illustrate how the solutions to the full system relate to the solutions of the simpli ed system of Section 1151 It has already been stated that the vertical error dynamics are unstable and that they must be compensate with some form of error feedback Also, the vertical error dynamics are only weakly a ected by the other states Because the vertical error dynamics will be compensated, we assume that the vertical position and velocity errors are small and remove those states from the model Therefore, the state vector is x = [ , , vn , ve , The reduced model has 0 0 0 0 0 0 0

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1 Re N, E, D]

Problem 16-18 Suppose a resistor of 100 , a capacitor of 820 pF, and a coil of 100 H are in parallel The frequency is 100 MHz What is the complex impedance Proceed according to the above steps, as follows:

1 Re cos( )

1 Calculate G = 1/R = 1/100 = 0100 2 Calculate BL = 1/(628f L) = 1/(628 100 100) = 00159 3 Calculate BC = 628f C = 628 100 0000820 = 000515 (Remember to first convert the capacitance to microfarads, to go with megahertz) 4 Calculate B = BL + BC = 00159 + 000515 = 00108 5 Define G 2 + B 2 = 01002 + ( 00108)2 = 0010117 Then R = G/0010117 = 0100/0010117 = 988 , and X = B/0010117 = 00108/0010117 = 107 6 The complex impedance is R + jX = 988 + j107

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0 F54

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Problem 16-19 Suppose a resistor of 470 , a capacitor of 500 pF, and a coil of 100 H are in parallel What is their complex impedance at a frequency of 2252 MHz Proceed as before:

1 Re cos( )

0 0 0 0 0 N 0

1 Calculate G = 1/R = 1/470 = 0021277 2 Calculate BL = 1/(628f L) = 1/(628 2252 100) = 000707 3 Calculate BC = 628f C = 628 2252 0000500 = 000707 (Remember to first convert the capacitance to microfarads, to go with megahertz) 4 Calculate B = BL + BC = 000707 + 000707 = 000000 5 Define G 2 + B 2 = 00212772 + 000000 2 = 000045271 Then R = G/000045271 = 0021277/000045271 = 46999 , and X = B/000045271 = 000000/000045271 = 000000 6 The complex impedance is R + jX = 469999 + j000000 When we round it off to three significant figures, we get 470 + j000 This a pure resistance equal to the value of the resistor in the circuit

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The Colpitts Circuit The capacitance can be tapped, instead of the inductance, in the tuned circuit of an RF oscillator Such a circuit is called a Colpitts oscillator, and a P-channel JFET version is diagrammed in Fig 24-14 The amount of feedback is controlled by the ratio of the capacitances A variable inductor provides for frequency adjustment This is a matter of convenience, because it can be difficult to find a dual

0 0 2 D 0

2 D 0

variable capacitor that maintains the correct ratio of capacitances throughout its tuning range Using fixed capacitors eliminates this problem, and it costs less, too! Unfortunately, finding a good variable inductor for use in a Colpitts oscillator can be just about as hard as obtaining a suitable dual-gang variable capacitor A permeability-tuned coil can be used, but ferromagnetic cores impair the frequency stability of an RF oscillator A roller inductor can be employed, but these are bulky and expensive An inductor with several switch-selectable taps can be used, but this does not allow for continuous frequency adjustment Despite these shortcomings, the Colpitts circuit offers exceptional stability and reliability when properly designed, and is preferred by some engineers for this reason

The stationary error dynamics are important during system initialization It is the stationary system that will be brie y considered in this section

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