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The peak value of the electric field, in the light radiated by a point source of power P1 , at a point, distant r1 from the source, is E01. The corresponding value, for a point source of power P2 , at a point, distant r2 from the source, is E02. The ratio \((\frac{E_{01}}{E_{02}})\) equals

(1) \((\frac{P_1r^2_1}{P_2 r^2_2})^{1/2}\)

(2) \((\frac{P_2r^2_2}{P_1 r^2_1})^{1/2}\)

(3) \((\frac{P_1r^2_2}{P_2 r^2_1})^{1/2}\)

(4) \((\frac{P_1r^2_1}{P_2 r_2})^{1/2}\)

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 (3) \((\frac{P_1r^2_2}{P_2 r^2_1})^{1/2}\)

The peak value, of the electric field (E0 ) of an em wave, (at a point distant r from the source) is related to the power (P) of the source as

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