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When an ac voltage is placed across an inductor and starts to increase (either positively or negatively) from zero, it takes a fraction of a cycle for the current to follow Once the voltage starts decreasing from its maximum peak (either positive or negative) in the cycle, it again takes a fraction of a cycle for the current to follow The instantaneous current can t quite keep up with the instantaneous voltage, as it does in a pure resistance Thus, in a circuit containing inductive reactance, the current is said to lag the voltage in phase

(886)

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Eqn (885) is not usually used directly, because as shown in eqn (886), 2 the noise variance (ie, e ect of 1 and 2 on ) is approximately 9 The following two paragraphs discuss alternative approaches to the construction of ionospheric free pseudorange observables An estimate of the ionospheric delay can be computed as Ia = f1 f2 2 2 ( 2 1 ) f1 f2 (887)

Pure Inductance Suppose that you place an ac voltage across a coil, with a frequency high enough so that the inductive reactance, XL, is much larger than the resistance, R In this situation, the current is 1 4 of a cycle behind the voltage That is, the current lags the voltage by 90 , as shown in Fig 13-8 At very low frequencies, large inductances are normally needed in order for the current lag to be

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Direct substitution of eqns (883 884) into eqn (887) shows that Ia f1 f2 2 2 ( 2 1 ) f1 f2 = Ia + 1984 ( 2 1 ) = Ia + (888) (889)

a full 90 This is because any coil has some resistance; no wire is a perfect conductor If some wire were found that had a mathematically zero resistance, and if a coil of any size were wound from this wire, then the current would lag the voltage by 90 in this inductor, no matter what the ac frequency When the value of XL is very large compared with the value of R in a circuit that is, when there is an essentially pure inductive reactance the vector in the RL plane points straight up along the XL axis Its angle is 90 from the R axis, which is considered the zero line in the RL plane

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which shows that Ia is unbiased The variance of Ia at each epoch is 2 approximately 8 Because of the magni cation of the receiver noise, the ionospheric estimate of eqn (887) is not used directly to compensate the pseudorange measurement Instead, because Ia changes slowly with a correlation time of a few hours, while 1 and 2 have much shorter correlation times, Ia could for example be low pass ltered by a lter with a time constant of several minutes to greatly decrease the e ect of 1 and 2 while maintaining the time variation of Ia If we denote the ltered version of a as Ia then an ionosphere free pseudorange can be computed as I = 1 which has the error model = + Ecm + 1 where the ionospheric error has been (essentially) removed and the measurement noise has not been ampli ed The remaining common-mode errors could be removed via di erential processing Another approach is discussed subsequently Simultaneous L1 and L2 phase observables from the same satellite and receiver can be modeled as 1 1 2 2 = = f2 Ia + 1 + 1 N1 f1 f1 + Ecm Ia + 2 + 2 N2 f2 + Ecm (891) (892) f2 Ia f1 (890)

where 1 = fc1 and 2 = fc2 are the wavelength of the L1 and L2 carrier signals, respectively, and i is the combined e ect of multipath and receiver noise The subsequent analysis assumes that 1 and 2 are independent 2 Gaussian processes with variance Using the phase observables, the ionospheric delay can be estimated as Ia = f1 f2 2 2 1 1 2 2 f1 f2 (893)

Inductance with Resistance When the resistance in a resistance-inductance (RL) circuit is significant compared with the inductive reactance, the current lags the voltage by something less than 90 (Fig 13-9) If R is small compared with XL, the current lag is almost 90 , but as R gets larger relative to XL, the lag decreases The value of R in an RL circuit can increase relative to XL because resistance is deliberately placed in series with the inductance It can also happen because the ac frequency gets so low that XL

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