LuiTi l 02RoilRi

i.e. the accelerated particle density in the source should exhibit a peak maximum at f 8(2P-l)(P- tRt(l + 0.2(Rp^RjR)

When the spectrum described by Eq. 4.6.34 is presented in the power form n(R) rc R ~Y, the variable power exponent y will be determined by the expression

Y = -^nn(R) = '34ß{RiljRoi))RlRi r - (ß - !). (4.6.36)

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