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erly account for the correlation in i,m , the algorithm described in Exercise B17 should be used instead, with R de ned as the (non-diagonal) measurement correlation matrix This section has discussed single di erences across satellites for simultaneous measurements from a single receiver Such satellite di erencing, when used, is usually implemented in the form of double di erencing This technique is discussed in Section 883 Double di erencing is one form of di erential GPS, which is discussed more generally throughout Section 88 8432 Receiver Clock Bias Dynamic Model

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Any transformer used in the 60-Hz utility line, intended to provide a certain rms ac voltage for the operation of electrical circuits, is a power transformer Power transformers exist in a vast range of physical sizes, from smaller than a tennis ball to as big as a room

Physically, as discussed relative to eqn (841), the clock bias develops as the integral of the clock oscillator frequency error f (t) This physical process suggests a two state clock model described as v1 v2 tr = = 0 0 [ 1 1 0 0 ]v v1 v2 + w wf (849) (850)

At the Generating Plant The largest transformers are employed at the places where electricity is generated Not surprisingly, high-energy power plants have bigger transformers that develop higher voltages than low-energy, local power plants These transformers must be able to handle high voltages and large currents simultaneously

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where v = [v1 , v2 ] and w and wf are the process noise driving the clock phase and frequency error states, respectively Assuming that the two noise processes are stationary, independent, and white with power spectral densities of S and Sf , respectively, then for = [w , wf ] S = Q = S 0 0 Sf (851)

This two state model corresponds well with the data presented in Figure 83 The frequency error is modeled as a constant plus random walk (ie,

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When electrical energy must be sent over long distances, extremely high voltages are used This is because, for a given amount of power ultimately dissipated by the loads, the current is lower when the voltage is higher Lower current translates into reduced loss in the transmission line Recall the formula P = EI, where P is the power (in watts), E is the voltage (in volts), and I is the current (in amperes) If you can make the voltage 10 times larger, for a given power level, then the current is reduced to 1 10 as much The ohmic losses in the wires are proportional to the square of the current Remember that P = I 2R, where P is the power (in watts), I is the current (in amperes), and R is the resistance (in ohms) Engineers can t do much about the wire resistance or the power consumed by the loads, but they can adjust the voltage, and thereby the current Suppose the voltage in a power transmission line is increased by a factor of 10, and the load at the end of the line draws constant power This increase in the voltage reduces the current to 1 10 of its previous value As a result, the ohmic loss is cut to (1 10)2, or 1 100, of its previous amount That s a major improvement in the efficiency of the transmission line, at least in terms of the loss caused by the resistance in the wires and it is the reason why regional power plants have massive transformers capable of generating hundreds of thousands of volts

slowly changing constant) The phase error is modeled as the integral of the frequency error (ie, ramp) plus a random walk This is shown in block diagram form in Figure 84

Figure 84: Continuous-time two state clock model For this clock model, 0 1 0 0 For the discrete-time sampling period Ts , the state space model is F= v1 (k + 1) v2 (k + 1) = 1 Ts 0 1 v1 (k) v2 (k) + d (852)

Because F2 is identically zero, Qd can be calculated exactly using the rst three terms of eqn (4119): cov( d ) = Qd =

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