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The transfer function description of an FSSM encoder can be used to obtain the equivalent systematic form of a given non-systematic encoder [7]. This conversion method consists of converting the transfer function of a non-systematic form, as given in expression (11), into an expression of systematic form, like that of expression (24), by means of matrix operations. Example 6.4: Determine the equivalent systematic version of the convolutional encoder generated by the transfer function G(D) = G ns (D) = 1 + D 2 1 + D + D 2 The non-systematic convolutional encoder of the code described by this transfer function is shown in Figure 6.3. The transfer function should adopt the form of equation (24) to correspond to a systematic convolutional encoder. In this case the procedure is quite simple, because it only consists of dividing both polynomials of the transfer function by the polynomial 1 + D 2 . This procedure converts the transfer functions of the original convolutional code, which are in this case of FIR type, into transfer functions of IIR type. This division is done in order to make the matrix transfer function contain the identity submatrix, which in this example is G 11 (D) = 1. The resulting transfer function is G s (D) = 1 1 + D + D2 1 + D2

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2 A cell handover is the transfer of a user from one spot beam to another within the same satellite A satellite antenna directed to terminals is composed of a series of beams Such a decomposition of the satellite footprint allows reuse of the radio frequencies several times in its coverage area These handovers have no impact on intersatellite routing, but seriously impact on-board computations If a user is just on the border of the coverage area of a satellite, his/her connection time to an individual satellite can be extremely small Hence, in general, constellations are designed in such a way that the footprints overlap and extremely small connection times to an individual satellite never happen Nevertheless, the maximum connection time is still limited A user s trajectory, viewed from the satellite, will resemble a straight line crossing the center of the coverage area.

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Definition 5.3 (Discretization error) Assume that the system (5.I I ) , (5.12) has an exact in solution Y ( t ) the interval (0, T ) . Consider a partition 0 = t o < tl < t 2 < . . . < t K = T and let Y o Y 1 .,. . , Y be the approximate solution obtained by means ofthe one-step , method (5.18). The discretization error is defined as

The apparent (or relative) speed of the user is then the speed of the satellite This causes the following undesirable phenomena: visibility changes, varying topologies (ISLs changes), footprint handover, and need for rerouting 22312 Earth s Self-Rotation The Earth s self-rotation introduces some more complication in the system In Figure 225, we plot the maximum time between two satellite handovers against the altitude h and the elevation angle of a constellation, in two cases: 1 The Earth s self-rotation is not taken into consideration and the satellite s inclination can be arbitrary 2 The Earth s self-rotation is taken into account and the orbit of the satellite is equatorial 22313 Modeling the Network Mobility Notice that the maximum handover time, shown in Figure 225, can vary from some minutes up to several hours.

Also, inclined orbits can be used to exploit the Earth s self-rotation to increase the visibility period Hence, the mobility of the network can also vary a lot Roughly speaking, one can distinguish between low and high mobility, depending on the maximum handover time Low Mobility (periodic) In [5], the mobility of a satellite constellation is described in terms of finite state automation (FSA) by a series of states described along the time period in round robin fashion The main advantage of this model is that we have to consider only a finite set of configurations of the satellite constellation (in which the satellites are assumed to be immobile), and provide efficient routing solutions for each of them, inspired by classical telecommunication problems Low Mobility (aperiodic) It is worth observing that the periodicity assumption of the FSA model may be, in some cases, too strong.

This is essentially due to the combination of physical factors, such as the Earth s self-rotation, the satellite s speed, and the use of inclined orbits They make the system aperiodic for all practical purposes, ie, a satellite will find again the same position only after such a long time that too many intermediate states would be necessary In this case, a possible approach consists in taking a series of.

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