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By L. Seiler (USAF)

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25 The co-plete pulse out to the con- The second is ductivity and allow the fields to fall off more slowly. in comnutinq the slew breakoowin of the small anqle approximation the Compton currents. The height of burst was varied fields 6 indicates that burst plotted is This data for the varicus yields. increases as the field strength For increases only for the larger yields. field strength decreases as the burst height of the hypothetical in curves Fig. in Fig. The neneral 200 Km, and 300 Kr. v 100 K-,, Fin.

When a secondary electron Is created, it has an energy somewhat higher than its ambient energy. The secondary electrons transfer this additional energy to air molecules through both elastic and Inelastic collisions. on tOw c a nanosecond. is approximately trons at sea level I0 cV or Using an exoonential 2 shakes at 20 Km and to over a microsecond at 50 YK. tion time in the 20 Km case height used for the exponential atmosphere is (Re' 1902 11). S• This scale height of 7 Km is Baum also shows If taken as 7 The scale This value

The secondary electrons transfer this additional energy to air molecules through both elastic and Inelastic collisions. on tOw c a nanosecond. is approximately trons at sea level I0 cV or Using an exoonential 2 shakes at 20 Km and to over a microsecond at 50 YK. tion time in the 20 Km case height used for the exponential atmosphere is (Re' 1902 11). S• This scale height of 7 Km is Baum also shows If taken as 7 The scale This value

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