Electromagnetic Theory of Light Part I
Electromagnetic Theory of Light Part I
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(77) which can be interpreted as follows : " When the solution for the light- vector s is a complex quantity or expression, the resultant intensity will be proportional to the product of that quantity and its conjugate complex quantity. " Confirmation of given Solution. We can confirm that the expression (75) for s is a solution of the differential equation (72), on replacing there s by that expression and performing the differentiations indicated. To confirm that the surface condition (73) is ...fulfilled, we put = Q and 2?r in the respective solution (75) for s, and we have, since then 7 = 7' and o- = o-', -j, . Lirct / /g. . Nv% /^ . 7ry2 >.
s = a iV * J e-*y\ a a = arctan z/x (cf . The above relations between oj, z and r, ), we have *d 9, x = (arctan ^) = which expressions evidently reduce to the following on the obstructing screen, that is, f or
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To quickly assess the difficulty of the text, read a short excerpt:
(77) which can be interpreted as follows : " When the solution for the light- vector s is a complex quantity or expression, the resultant intensity will be proportional to the product of that quantity and its conjugate complex quantity. " Confirmation of given Solution. We can confirm that the expression (75) for s is a solution of the differential equation (72), on replacing there s by that expression and performing the differentiations indicated. To confirm that the surface condition (73) is ...fulfilled, we put
s = a iV * J e-*y\ a a
What to read after Electromagnetic Theory of Light Part I?
You can find similar books in the "Read Also" column, or choose other free books by Charles Emerson Curry to read online
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