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The ephemeris parameters describe the orbit during a given interval of time (at least one hour) The ephemeris parameters are the parameters for an extension of the orbital model predicted by Kepler The extension is necessary to account for non-uniformities in the Earth gravitational eld The ephemeris parameters are determined by the control segment as a curve t to the measured satellite orbit The parameter toe is the reference time of applicability (local origin) of the ephemeris parameters The ephemeris parameters are de ned in Table C1 [6] These parameters are broadcast by the satellites and available after decoding on-board the receiver The units of the broadcast parameters are also de ned in the table The ECEF coordinates for the phase center of the satellite antenna can be calculated using a variation of the equations shown in Table C2 [131] The main inputs to these equations are the variable tsv and the satellite clock correction and ephemeris parameters de ned in Table C1 The satellite antenna phase center position is very sensitive to small perturbations in most ephemeris parameters The sensitivity of position to the parameters A, Crc , and Crs is about one meter/meter The sensitivity to angular parameters is on the order of 108 meters/semi-circle, and to the angular rate parameters is on the order of 1012 meters/semi-circle/second Because of this extreme sensitivity to angular perturbations, the values of all constants should exactly match those stated in Appendix A, from [6] The parameter IODE is an integer which allows the user to detect when a new set of ephemeris parameters is available By monitoring the IODE value for the incoming satellite signal relative to the IODE of the ephemeris data currently in use, the user can determine when to update the ephemeris model parameters A few comments are appropriate concerning Table C2 The variable tk is the actual total time di erence between the time t and the ephemeris reference time toe The calculation must account for beginning or end of week crossovers That is, if tk is greater than 302,400 seconds, subtract 604,800 seconds from tk If tk is less than -302,400 seconds, add 604,800.

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Parameter TGD IODC toc af 2 af 1 af 0 M0 n e A1/2 0 i0 IDOT Cuc Cus Crc Crs Cic Cis toe IODE

RF output for 10-W input, but a grounded-grid amplifier needs 50 W to 100 W of drive to produce 1 kW of RF output A grounded-grid amplifier has a significant advantage, however: it is less likely to break into unwanted oscillation than a grounded-cathode circuit

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Description Group Delay, sec Issue of Data, Clock Clock data reference time, sec sec Second order correction to satellite clock, sec2 sec First order correction to satellite clock, sec Constant correction to satellite clock, sec Mean anomaly at reference time, semi-circles Mean motion di erence from computed value, semi-circles/sec Eccentricity, dimensionless Square root of the semi-major axis, m Longitude of ascension node at reference time, semi-circle Inclination angle at reference time, semi-circle Argument of perigee, semi-circle Rate of right ascension, semi-circle/sec Rate of inclination angle, semi-circle/sec Amplitude of the cosine harmonic correction to the argument of latitude, rad Amplitude of the sine harmonic correction to the argument of latitude, rad Amplitude of the cosine harmonic correction to the orbit radius, m Amplitude of the sine harmonic correction to the orbit radius, m Amplitude of the cosine harmonic correction to the angle of inclination, rad Amplitude of the sine harmonic correction to the angle of inclination, rad Ephemeris reference time, sec Issue of Data, Ephemeris

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Plate Voltage The plate voltages (+600 V dc) in the circuits of Figs 29-4 and 29-5 are given as examples The amplifiers shown could produce 75- to 150-W signal output provided they receive sufficient drive and are properly biased An amplifier rated at 1-kW output would require a plate voltage of +2 kV dc to +5 kV dc In high-power radio and TV broadcast transmitters producing in excess of 50-kW RF output, even higher dc plate voltages are used

seconds to tk The equation for Ek must be solved iteratively Various iterative solution techniques are considered in [131] Table C3 [44] contains a complete example set of ephemeris parameters By using these ephemeris parameters in the equations of Table C2 the space vehicle (satellite) time o set and ECEF satellite antenna coordinates can be determined The results of these calculations are shown in Table C4

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Many TV receivers, and some desktop computer monitors, use cathode-ray tubes (CRTs) So do older oscilloscopes, spectrum analyzers, and radar sets

F e A sin(Ek ) af 0 + af 1 (tsv toc ) +af 2 (tsv toc )2 + tr tsv tsv ( A)2

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