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In the second approach, the forces and events that determine the motion of a particle retain their statistical nature so that the trajectory of each particle is different from that of any other in the gas In this second approach, at the basis of the so-called Monte Carlo models, macroscopic quantities like current or gas temperature are computed as an average of the behaviour of the population of the gas; a large number of particles must be simulated in order to get statistically meaningful results We rst describe deterministic models The models are classi ed by the type of equations (quantistic, semiclassical, mixed; Poisson s or Maxwell s equation); if semiclassical, by the number and type of included moments of Boltzmann s equation (hydrodynamic, energy-balance, drift-diffusion, etc.

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This was further supported by 1 H NMR (Section 3.6.4), by elemental analysis and by the fact that this would be an expected product of hydrolysis of HNBB.

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); by the number of dimensions (3D, 2D, quasi-2D, 1D); by the dependence on time (steady-state, time-dependent); and by the regime of validity (small-signal, large-signal, noise) The detailed description of the physical effects included in the different formulations, with the related accuracy, is beyond the scope of this book; therefore, not all possible combinations are described in the following but only some examples that are particularly meaningful for a circuit designer Let us now describe the semiclassical models The rst three moments of Boltzmann s equation are relative to the conservation of the number of particles, the conservation of their momentum and the conservation of their energy; each equation includes derivatives with respect to time and space.

Thermo-Physical and Ignition Properties of Polymers from Parts of a Minivana Tv (Td ) ( C) Head Liner 305 380 Instrument Panel 248 269 397 454 252 Resonator 296 447 572 Kick Panel Insulation 262 257 10 374 0.02 1.95 1.65 1.14 0.02 0.25 215 7 177 264 (continued overleaf ) 10 374 1.06 1.15 1.16 2.08 1.75 1.39 0.23 0.30 0.36 277 197 331 421 252 10 20 357 497 0.11 1.20 1.12 1.18 0.09 1.77 1.37 1.68 1.51 1.56 0.04 0.14 0.18 0.27 0.06 263 357 19 120 219 301 22 19 162 331 20 497 0.69 0.12 1.56 2.19 0.04 0.24 154 57 90 120 CHF (kW/m2 ) c (kJ/kg K)

If the time or space scale of the microscopic events is much smaller than that of the characteristic times or distances of the device, the importance of the corresponding terms is very small, and they can be neglected In this way, simpler expressions are derived Moreover, phenomena related to the energy of the particles are sometimes neglected, allowing the suppression of the energy conservation equation; phenomena like the velocity overshoot cannot be included in this case, but an additional simpli cation is obtained The equations are discretised in the space domain and in the time domain, if time dependence is included, so that the system of partial differential equations is replaced by a nite-difference equation system [4] The system is usually solved in the time domain, with similar schemes as those described for nonlinear circuits (Section 12).

frequency domain will distort the waveform of a broadband signal. More specifically in digital communication, a channel is considered frequency-selective if the multipath delays are distinguishable relative to the symbol period T s y m b o l :

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The choice of the space step in one or more dimensions (the mesh) and of the time step is critical, and many schemes have been devised for automatic adjustment ensuring numerical convergence Recently, a Fourier series approach has also been proposed, making use of harmonic balance or waveform balance techniques [5], that has demonstrated computation.