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parts layout diagram and capacitor code chart before installing them on the circuit board Go ahead and place a few of the capacitors at their respective locations on the PC board and solder them in place Remember to trim the extra component lead length with your end-cutters The magnetometer main circuit board utilizes three silicon diodes Diodes have polarity and they must be installed correctly for the circuit to operate correctly Each diode will have either a black or white colored band at one end of the diode body The colored band represents the diode s cathode lead, the opposite lead is the anode Remember the diode s electronic symbol is an arrow or triangle pointing to a vertical line The vertical line is the cathode of the diode Refer to the schematic and parts layout diagram when mounting the diodes onto the circuit board Place the diodes on the circuit board and solder them in place Trim the excess leads as necessary The magnetometer project employs a 10 MHz crystal which is connected to pin 16 of U1 The crystal has no polarity so it can be placed in either direction on the board Handle the crystal carefully so as to not break off the leads from the crystal body Before we begin placing the semiconductors on the PC board, you will want to refer to the semiconductor

3 3 3 0 9 9 0 27 27 3 81 78 2 234 236 2 708 706

ie, Rwg ( ) = 0012 ( )

None of the numbers in the bottom row are negative This tells us that 3 is an upper bound for the real roots To try the test root 3, we set up the array

(454)

3 3 # 0 # # 0 # # 3 # # 2 # # 2 # #

Table 18-2

3 3 3 0 9 9 0 27 27 3 81 84 2 252 254 2 762 764

Appending this state space realization model of eqn (349) yields x 0 1 0 0 v 0 0 g 0 = 0 1 0 20 R g 0 0 0 10 b

27

of the gyro error model to the error x 0 v 0 + 0 bg 1 wg (455)

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The numbers in the bottom row alternate in sign This indicates that 3 is a lower bound for the real roots 10 Here is an outline of the process for finding the rational roots of the equation 3x 5 3x 2 + 2x 2 = 0 All the coefficients, as well as the stand-alone constant, are integers, so we don t have to multiply the equation through by anything The integer factors m of the stand-alone constant are 2, 1, 2, and 1 The integer factors n of the leading coefficient are 3, 1, 3, and 1 All the possible ratios r = m/n are 2, 1, 2/3, 1/3, 2, 1, 2/3, and 1/3 We input rational numbers r of 2, 1, 2/3, 1/3, 2, 1, 2/3, and 1/3 to synthetic division arrays, and see if we get a remainder of 0 for any of them We get a remainder of 0 only when r = 1 Therefore, x = 1 is the only rational root of the equation

Note that the noise process and linear system must be speci ed jointly, since there are more degrees of freedom than design constraints Also, the selection of G(s) from the two factors of eqn (452) is not arbitrary The transfer function G(s) is selected so that its poles and zeros lie in the strict left half of the complex s-plane This results in a causal, stable linear system model Such a choice is always possible, when the spectral density

27

is the ratio of polynomials containing only even powers of s The interested reader is referred to the subject of spectral factorization When the driving noise is white and Gaussian, the process speci ed in eqn (454) is an example of a scalar Gauss-Markov process Higher order vector Gauss-Markov processes, such as the system of eqn (455), result when the correlation function is more complex Additional examples of simple Gauss-Markov process that are often useful in navigation system error model are discussed in Section 463

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