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for an ordinary discontinuity (finite jump) at some t = a(>0), the other conditions remaining gas in Theorem 1. then (see Fig i17) \left(1^{*}\right) \mathscr{L}\left(f^{\prime}\right)=s \mathscr{S}(f)-f(0)-[f(a+0)-f(a-0)] e^{-a s} \text { (c) Verify }\left(1^{*}\right) \text { for } f(t)=e^{-t} \text { if } 0

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