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18 In a common base circuit, the output is taken from (a) the emitter (b) the base (c) the collector (d) more than one of the above 19 Suppose that the input signal to a transistor amplifier results in saturation during part of the cycle This produces (a) the greatest possible amplification (b) reduced efficiency (c) avalanche effect (d) nonlinear output impedance 20 Suppose that the gain of a transistor in a common emitter circuit is 100 at a frequency of 1 kHz, and the gain is 707 at 335 kHz The gain drops to 1 at 210 MHz The alpha cutoff frequency is (a) 1 kHz (b) 335 kHz (c) 210 MHz (d) impossible to define based on this data

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The topic of attitude estimation is widely studied, eg [14, 40, 41, 42, 45, 46, 49, 82, 85, 91, 120, 132, 135, 136, 145] The main references for this chapter were [78, 143, 144] Because the approach of this chapter uses the Earth s gravitational and magnetic elds, successful operation is limited to the vicinity of the Earth Similar approaches using star sightings can be developed for space vehicles

other major category of transistor is the field effect transistor (FET ) There are two main types of FET: the junction FET (JFET ) and the metal-oxide FET (MOSFET )

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The topic of this chapter is aided inertial navigation Inertial navigation itself is a large topic with a signi cant body of related literature The presentation herein begins with a discussion of gravity and de nition of the concept of speci c force Both of these concepts and their interrelation are critical to inertial navigation Next, the chapter discusses the kinematics of inertial navigation in various reference frames The input variables to the kinematic models are accelerations and angular rates The acceleration vector is computed from a measured speci c force vector by compensating for gravity and instrument errors The dynamic evolution of the INS error state is a topic of detailed study The chapter includes a detailed derivation of a state-space model, analytic analysis of simpli ed models, simulation analysis of the full linear state-space model, and derivation and discussion of instrument error models Finally, the chapter concludes with sections that discuss initialization, INS aiding, and error state observability

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In a JFET, the current varies because of the effects of an electric field within the device Charge carriers (electrons or holes) flow from the source (S) electrode to the drain (D) electrode This results in a drain current, ID, that is normally the same as the source current, IS The rate of flow of charge carriers that is, the current depends on the voltage at a control electrode called the gate (G) Fluctuations in gate voltage, EG, cause changes in the current through the channel, which is the path between the source and the drain The current through the channel is normally equal to ID Small fluctuations in EG can cause large variations in ID This fluctuating drain current can produce significant fluctuations in the voltage across an output resistance

The purpose of this section is to distinguish between inertial and noninertial forces and to de ne the concept of a speci c force

N-Channel versus P-Channel A simplified drawing of an N-channel JFET, and its schematic symbol, are shown in Fig 23-1 The N-type material forms the channel, or the path for charge carriers The majority carriers are electrons The drain is placed at a positive dc voltage with respect to the source In an N-channel device, the gate consists of P-type material Another section of P-type material, called the substrate, forms a boundary on the side of the channel opposite the gate The voltage on the gate produces an electric field that interferes with the flow of charge carriers through the channel The more negative EG becomes, the more the electric field chokes off the current through the channel, and the smaller ID becomes A P-channel JFET (Fig 23-2) has a channel of P-type semiconductor The majority charge carriers are holes The drain is negative with respect to the source The more positive EG gets, the more the electric field chokes off the current through the channel, and the smaller ID becomes

Newton s law of gravitation states that the force of gravitational attraction of mass m1 on m2 is de ned by F12 = Gm1 m2 p12 p12 3 (111)

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