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Both the traditional leapfrog time-integration technique used by the nite-difference time-domain (FDTD) method and the Newmark-beta formulation used with the nite element time-domain (FETD) method have a temporal truncation error proportional to t 2 With explicit, and therefore, conditionally stable time-stepping methods such as the FDTD technique, the Courant condition on a uniform mesh with grid size constrains the time step according to c t / 3 for numerical stability purposes As noted above, if we assume a spatial sampling of 20 points per wavelength at the highest frequency of interest, then t 1/(20 3 f max ) and we see that we have a relatively high temporal sampling even at the highest frequencies Consequently, suf cient temporal resolution is normally not an issue with the traditional FDTD method.

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However, with unconditionally stable techniques, such as the FETD method based on the Newmark-beta formulation, additional care is required in the selection of the time step, because numerical stability no longer constrains how large the time step can be with these methods Therefore, accuracy limits the largest practical time step and the user must choose it appropriately Unconditionally stable formulations are particularly bene cial to practical applications having a mix of both coarse and ne geometrical details This is because the ne geometrical details will not force a further reduction in the time step, which is a signi cant bene t that is not possible with a conditionally stable formulation For example, for wideband antennas such as spirals, the complex and geometrically small details associated with the feed region will have no impact on the time step associated with an unconditionally stable formulation.

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As a simple guideline, de ning the time step for the unconditionally stable FETD method according to c t h max , where h max denotes the maximum spatially resolved edge length on the grid, has been found to provide a good balance of accuracy and ef ciency It is also important with time-domain simulations to let the solution reach a steady state, either through direct time marching or possibly by using a time extrapolation method [4] Premature truncation of the.

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5 eV versus 2 eV. As a result, the absolute magnitude of the spectrum in Fig. 8-18 is about 2 orders of magnitude more intense than one would expect from an operating ion thruster.

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where p is the frame error probability on the PCH and AGCH, Pk is the decoding success probability of the channel request that is spread into k bursts (3 50), M is the maximum number of retransmissions for channel request (1, 2, 4 or 7) and L is the maximum number of paging attempts (not speci ed). As described in Section 12.1, the data link layer increases transmission reliability with a send-and-wait ARQ protocol on the SDCCH and FACCH. That is, an information frame is retransmitted until both the frame itself and its acknowledgement are received correctly. Suppose that a signalling procedure consists of K information frame transmissions when all the frames are correctly received, and that a separate response frame carries the acknowledgement of each information frame. Then, the success probability of the procedure after N information frame transmissions (N K) is

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