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Satellite Orbit and Ephemeris Determination using Inter Satellite Links

Satellite Orbit and Ephemeris Determination using Inter Satellite Links

Satellite Orbit and Ephemeris Determination using Inter Satellite Links

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<strong>Inter</strong> <strong>Satellite</strong> <strong>Links</strong>Software Description5.3 Measurement SimulationMeasurements are computed from the geometric range or range rate <strong>using</strong> the true satelliteorbits <strong>and</strong> adding delays from the signal path, clock offsets <strong>and</strong> r<strong>and</strong>om errors. The computedrange is also used to derive the free distance attenuation of the signals. The followingmeasurement equation indicates the considered components of a pseudo range measurement.PR0 ρGeometric+ c⋅T( δTSat− δ Ground / Sat2 + δiono+ δ Tropo + δ Multipath ) + ε noise= Eq. 5.3-1The largest part is represented by the true geometric range. The delays, which are scaled withthe speed of light to obtain a distance, are• <strong>Satellite</strong> clock offset• Ground station clock offset or 2 nd satellite clock offset• Ionospheric delay• Tropospheric delay• MultipathThe two clock offsets are generated by initialising the clock offset variable of each satellite<strong>and</strong> ground station <strong>using</strong> a r<strong>and</strong>om number with• 3 milliseconds st<strong>and</strong>ard deviation for the satellite clocks.• 100 nanoseconds st<strong>and</strong>ard deviation for the ground station clocksThe errors introduced by the signal propagation path are considered by computingtropospheric <strong>and</strong> ionospheric delays from models. The last error contributor is the thermalnoise, which has been computed <strong>using</strong> the range dependent free distance attenuation.Under the assumption, that tropospheric <strong>and</strong> ionospheric delays can be removed to a certaindegree <strong>using</strong> models, only the residual errors of these contributor are considered in themeasurement noise, as indicated in the following equation.σ222( 0.2⋅ δ ) + ( 0. ⋅ ∆ ) + δ2 2Range = σThermal+ Tropo 5IonoMultipathEq. 5.3-2The simulated range measurements is then obtained byPR= PR 0 + RANDOM⋅σRangeEq. 5.3-3The error of a range rate measurement has been assumed to depend only on the thermal noise.σ2RangeRate= σ2ThermalEq. 5.3-4The measurement errors had been obtained bywherePRD = PR D 0 + RANDOM⋅σEq. 5.3-5RangeRateR. Wolf Page 75

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