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The prediction for the JIDC-2 was done assuming that the spacecraft spacecraft was at a celestial body with a zenith angle of 45$^{\circ}$. The offset of the transmitter was 5$^{\circ}$ west of zenith, which represents the worst case scenario. The expected noise was computed for an SNR of 6 dB, which is the SNR at which a valid MP target can be detected. The results are shown in the fifth column of Table 1.
From the results shown in Table 1, it is clear that for the scenarios tested, the results using equations (1) and (3) to predict the MP effects are quite comparable to the results from the simulations. The offset of the prediction for the Gravis results is a bit higher than the actual offset, but this is due to the fact that the zenith angle of the Gravis receiver is 45$^{\circ}$, which means that the MP effects are not properly predicted because of the loss of geometry effects in the geometrically distorted image.
The difference between the MP results computed by using equations (1) and (3) and the simulated (real) results is particularly striking in the Gravis case, indicating that equation (3) is preferable. This is due to the fact that the signal received by the Gravis is heavily attenuated, which reduces the MP effects compared to a situation in which a stronger signal is received.
In conclusion, the use of the Gravis simulator seems to be the better approach to perform the MP study of an EP.
SUMMARY AND CONCLUSIONS
=======================
The results of this study demonstrate that the emitted MP signal is influenced by the transmitting EP, if the transmitter power is greater than the receiving system gain, which is typical for the case of a spaceborne system. Hence, it is required for those types of systems to verify the MP behavior of their expected receivers and to predict how this behavior changes because of presence of an EP, which is the central goal of this
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