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N-channel, depletion-mode MOSFET and the circuit diagram would be the same For an N-channel enhancement-mode device, an extra resistor would be necessary, running from the gate to the positive power supply terminal For P-channel devices, the supply would provide a negative, rather than a positive, voltage Capacitor C1 and resistor R1 place the source at signal ground while elevating the source above ground for dc The ac signal enters through C2 Resistor R2 adjusts the input impedance and provides bias for the gate The ac signal passes out of the circuit through C3 Resistor R3 keeps the output signal from being shorted out through the power supply The circuit of Fig 23-11 is the basis for low-level RF amplifiers and oscillators The common source arrangement provides the greatest gain of the three FET circuit configurations The output is 180 out of phase with the input

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A (non-rotating) accelerometer with no applied forces is in free-fall with p = G; therefore, the accelerometer output is f = 0 An accelerometer in stable orbit around Earth, is also in free-fall It is constantly accelerating towards Earth with acceleration p = G; therefore, the accelerometer output is again f = 0 Consider an accelerometer at rest on the Earth surface In this case, the accelerometer is subject to the Earth s gravitational eld and is caused to rotate about the Earth at the Earth rate ie De ning the origin of the inertial frame to be coincident with the Earth center of mass, we have that p = ie ie p where ie = [ ie ]; therefore, the accelerometer output is f = ie ie p G, (1113)

which is the inertial force applied by the supporting structure to the case to maintain the case in a stationary Earth relative position When using an accelerometer, the user must compensate the speci c force output for the e ects of gravity To prepare for the subsequent analysis, de ne the local gravity vector as g = G(p) ie ie p (1114)

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is present along with susceptance, admittance vectors point at angles; they are neither vertical nor horizontal

The local gravity vector indicates the direction that a weight would hang at a location indicated by p Figure 112 shows the relation of these three accelerations The vector magnitudes are not drawn to scale In reality 1 ie ie p 300 G In this gure, and c denotes geodetic and geocentric latitude, respectively The speci c force vector can be represented in any desired frame of reference When this is done, the analyst should be careful with terminology and interpretation For example, the speci c force vector in the ECEF

which is the inertial acceleration minus gravity both represented in ECEF frame If we let pe represent the position vector in the ECEF frame, it is d2 important to note that Re pi = dt2 pe , see Section 1122 i

You ve seen how vectors add in the RX plane In the GB plane, the principle is the same The net admittance vector is the sum of the component admittance vectors

The purpose of this section is to derive an expression for the e ect of position error on the computed navigation frame gravity vector The second term in eqn (1114) is straightforward; therefore, this section focuses on the term G(p) = GM3 p p The analysis of this section will be used later in this chapter; however, on the rst reading of the chapter, the majority of this section may be skipped In that case, it is recommended that the reader proceed directly to the nal result of eqn (1122) and the discussion that follows it Denote the actual and computed vehicle locations relative to the Earth center of mass by p and p, respectively The error between these locations is p = p p Using the rst two terms in the Taylor s series expansion, we obtain the linear error model g = G(p) G( ) = p where G p =

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how to convert pdf to jpg in c# windows application

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