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New Century Senior Physics
Second Edition
Worked solutions
Chapter 18 - Light
from Richard Walding
Q1
Q2
Q3
Q4
Q5
Q6
Q7
Q8
Q9
Q10
Q11
Q12
Q13
Q14
Q15
Q16
Q17
Q18
Q19
Q20
Q21
Q22
Q23
Q24
Q25
ngd = nd/ng
Q26
(a) (i) nm = va/vm vm = va/nm = 3 x 108/1.78 = 1.68 x 108 m s-1
(ii) vm = = 3 x 108/1.2 = 2.5 x 108 m s-1
(iii) vm = = 3 x 108/2.1 = 1.43 x 108 m s-1
(iv) vm = = 3 x 108/1.42 = 2.11 x 108 m s-1
(b) The more optically dense is the one with the greatest refractive index (medium iii)
Q27
Q28
nm = a/m g = a/ng = 633 nm/1.5 = 422 nm
Q29
n = true depth/apparent depth
1.33 = true depth/50 cm
true depth = 1.33 x 50 = 66.5 cm
Q30
Q31
Q32
Q33
Q34
Q35
(a)
i 20 30 40 50 60 70 80r 10 15 20 24 27 30 31
sin r 0.17 0.26 0.34 0.41 0.45 0.50 0.52sin i 0.34 0.50 0.64 0.77 0.87 0.94 0.98
(b)
(c) linear (c-intercept = 0)
(d) sin i sin r
(e) sin i/sin r = n = 1.8988 (gradient)
(f) zircon n = 1.9
Q36
Q37
Q38
i 10 15 20 25 30 35 40r 13 22 30 38 47 57 70sin r 0.22 0.37 0.50 0.62 0.73 0.84 0.94sin i 0.17 0.26 0.34 0.42 0.50 0.57 0.64
Gradient = sin i/sin r = nkero/air
Gradient = y/x = (0.643 - 0.174)/(0.940 - 0.225) = 0.6861
Therefore nkero/air = 0.6861; or nair/kero = 1/0.6861 = 1.457
sin c = 1/nkero = 1/1.457 = 0.6861
c = sin-1 0.6861 = 43.3
Alternatively, solve equation for when sin r = 1 (that is, when r = 90)
y = 0.6861 x 1
y = sin i = 0.6861
c = sin-1 0.6861 = 43.3
Q39
Q40
Since the incident ray on the plastic block is 90o it passes into the block undeflected.
At the plastic /water interface the angle of incidence = 45o
n1 sin 1 = n2 Sin 2
1.62 sin 45 = 1.33 sin 2
2 = 59.5o
At the water/ air interface: the angle of incidence = 180 - 135 - 30.5 = 14.5o
n1 sin 1 = n2 sin 2
1.33 sin 14.5 = 1 sin 2
2 = 19.5o
Q41
Q42
Q43
It would appear transparent and wouldn’t be able to be seen as it doesn’t refract the light. You
could add a dye to make it less transparent, or you could use another plastic that had a
different refractive index to water, or use cardboard so that it would disintegrate when
exposed to water after a short time.