DlnnR 34RRR1

4uiTiRoi

(2). The case 8 = 1, * is arbitrary. Since in this case x- 8(1 8) = 0 and x is always > 0, we shall obtain instead of Eq. 4.6.20:

After integrating Eq. 4.6.30 from the initial value, we shall obtain

Whence, including Eq. 4.2.7 and Eq. 4.6.9, we obtain for the expected rigidity spectrum:

It can be seen from Eq. 4.6.33 that if P > l then at R >> Rj the accelerated particle spectrum may be presented in the form

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