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0040B5BA 0040B5BE 0040B5C2 0040B5C5 0040B5C8 0040B5C9 0040B5CC 0040B5D0 54 58 6B 00 5B 00 41 00 46 00 51 00 41 41 push pop imul add inc add inc inc esp eax eax,dword ptr [eax],5Bh byte ptr [ecx],al esi byte ptr [ecx],dl // <---- HERE ecx ecx
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#include <stdlib.h> #include <stdio.h> int main( int argc, char *argv[] ) { int c; printf( Decimal Hex Character\n ); printf( ======= === =========\n ); for( c = 0x20; c < 256; c++ ) { switch( c ) {
As the electric eld intensity begins to grow, it will propagate in the z-direction at the propagation velocity, u p = c r , and it will travel a distance d p = c t p r before it reaches its maximum Ep. Thus, an electric dipole oscillator at a point z in the medium will experience a growth in electric eld intensity beginning at zero at time t1 = z r c and rising to Ep = Ep x by time t2 = z r c + t p ; i.e., the maximum will be delayed by an amount tp. This will in turn cause a delay in the response electric ux density in the same amount of time. The convolution integral is carried out in a manner similar to that for the step function and the results are shown in Figure 5.32. In Figure 5.32 we see that the main in uence of the more realistic ramp function is to delay the response in time but the absolute displacement is the same for both functions. This result implies that the electric dipoles formed by a ramp will occur later in time that those of a step function and thus the total eld formed by the incident electric eld intensity and that caused by the induced electric dipoles will occur later in time.
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