Physics 295 Solutions to problems in Chapter 37 P37.2 ybright L d m For m 1 , P37.5 3.40 103 m 5.00 104 m yd 515 nm L 3.30 m 1 In the equation d sin m 2 The first minimum is described by m0 and the tenth by m 9 : sin Also, 1 9 d 2 tan y L but for small , Thus, d d P37.23 9.5 5 890 1010 m 2.00 m (a) 3 sin tan 9.5 9.5 L sin y 1.54 103 m 1.54 mm 7.26 10 m The light reflected from the top of the oil film undergoes phase reversal. Since 1.45 1.33 , the light reflected from the bottom undergoes no reversal. For constructive interference of reflected light, we then have 1 2nt m 2 or m 2 1.45 280 nm 2nt m 1 2 m 1 2 Substituting for m gives: m 0, 0 1 620 nm (infrared) m 1, 1 541 nm (green) m 2, 2 325 nm (ultraviolet) Both infrared and ultraviolet light are invisible to the human eye, so the dominant color in reflected light is green . (b) The dominant wavelengths in the transmitted light are those that produce destructive interference in the reflected light. The condition for destructive interference upon reflection is 2nt m or m 2nt 812 nm m m Substituting for m gives: m 1, 1 812 nm (near infrared) m 2, 2 406 nm (violet) m 3, 3 271 nm (ultraviolet) Of these, the only wavelength visible to the human eye (and hence the dominant wavelength observed in the transmitted light) is 406 nm. Thus, the dominant color in the transmitted light is violet . P37.27 1 2nt m so 2 1 t m 2 2n Minimum 1 500 nm t 96.2 nm 2 2 1.30 P37.32 The condition for bright fringes is 2t 2n m n m 1, 2, 3, . From the sketch, observe that 2 R r 2 r 2 t R 1 cos R 1 1 2 2 R 2R The condition for a bright fringe becomes and , r2 1 m R 2 n Thus, for fixed m nr 2 constant Therefore, nliquid r f2 nair ri2 and nliquid 1.00 1.50 cm 2 1.31 1.31 cm 2
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