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Direct substitution of eqns (891) and (892) into eqn (893) shows that Ia = f1 f2 2 2 ( 1 2 + N1 1 N2 2 ) f1 f2 f1 f2 = Ia + 1984 ( 2 1 ) + 2 2 (N1 1 N2 2 ) f1 f2 Ia + (894) (895)

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decreases until it is comparable to the loss resistance R in the coil winding In either case, the situation can be schematically represented by an inductance in series with a resistance (Fig 13-10) If you know the values of XL and R, you can find the angle of lag, also called the RL phase angle, by plotting the point R + jXL on the RL plane, drawing the vector from the origin out to that point, and then measuring the angle of the vector, counterclockwise from the resistance axis You can use a protractor to measure this angle, or you can compute its value using trigonometry Actually, you don t have to know the actual values of XL and R in order to find the angle of lag All you need to know is their ratio For example, if XL = 5 and R = 3 , you get the same RL phase angle that you get if XL = 50 and R = 30 , or if XL = 20 and R = 12 The angle of lag is the same for any values of XL and R in the ratio 5:3

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2 Therefore, the variance of Ia at each epoch is approximately 8 ; however, the estimate contains the signi cant constant bias

2 f1

Pure Resistance As the resistance in an RL circuit becomes large with respect to the inductive reactance, the angle of lag gets small The same thing happens if the inductive reactance gets small compared with the resistance When R is many times greater than XL, the vector in the RL plane lies almost on the R axis, going east (to the right) The RL phase angle in this case is close to 0 The current is nearly in phase with the voltage In a pure resistance, with no inductance at all, the current is precisely in phase with the voltage (Fig 13-11) A pure resistance doesn t store and release energy as an inductive circuit does, so there is no sluggishness in it

(896) (897)

Eqns (896) and (897) are in the exact form considered in Example 54 Therefore, the solution is Ia (k) = Ia (k) B(k) where 1 Bk = Bk 1 + k Ia Ia Bk 1 (898)

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If you know the ratio of the inductive reactance to the resistance (XL/R) in an RL circuit, then you can find the phase angle Of course, you can also find the phase angle if you know the actual values of XL and R

starting at k = 1 with B0 = 0 The estimation error variance for B is 2 1 2 2 2 2 PB = 8(1 + ) k and for Ia (k) is PIa = 8 + , where = k and = 001 is the ratio of the phase noise to the pseudorange noise The desire to estimate the ionospheric delay was a primary motivation for the GPS system to incorporate signals on two frequencies The speci cation of the two frequencies involved a tradeo related to the frequency spacing If the frequency separation was too small, then measurement errors would be signi cantly magni ed as shown in eqn (888) and (894) However, if the frequency separation were too large, then separate antennas would be required to receive the two signals

This section develops the equations for the narrow-lane and wide-lane observables These variables are synthesized as linear combinations of the L1 and L2 measurements The interest in the wide-lane signal is that its wavelength is large enough that the wide-lane variable is often used to facilitate the problem of integer ambiguity resolution, see Section 89 The phase measurements of eqns (891 892) can be modeled as 1 N 1 2 N2 = = f1 ( + Ecm + 1 ) c f2 ( + Ecm + 2 ) c f2 Ia c f1 Ia c (899) (8100)

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