Chapter 36373P36.65A hemisphere is too thick to be described as a thinlens. The light is undeviated on entry into the flatface. We next consider the light’s exit from thesecond surface, for which R=−600. cm.The incident rays are parallel, sop=∞.Then,npnqnnR1221+=−becomes01100156−−q..cmandq=10 7cm .FIG. P36.65P36.66(a)Ir==×=−P44504 1 60 10140222π...WmkW m2ej(b)Ir=469122..W47.20mmW m2af(c)111pq f:17200350m mqsoq=0368mandMhqp=′=− =−
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This note was uploaded on 12/14/2011 for the course PHY 203 taught by Professor Staff during the Fall '11 term at Indiana State University .