4. The distance d between the beetle and the scorpion is related to the transverse speed vt
and longitudinal speed v as
d vt tt v t
where tt and t are the arrival times of the wave in the transverse a
38.4
energy
hc
. 1 eV = 1.60 10 19 J . For a photon, E = hf = . h = 6.63 10 34 J s.
t
EXECUTE: (a) energy = Pavt = (0.600 W)(20.0 103 s) = 1.20 10 2 J = 7.5 1016 eV
IDENTIFY and SET UP:
Pav =
(6.63 10
36. (a) Eq. 37-36 leads to a speed of
v
c (0.004)(3.0 108 m/s) 1.2 106 m/s 1 106 m/s.
(b) The galaxy is receding.
37. We obtain
v
620 nm 540 nm
c
c 0.13c.
620 nm
43. (a) The work-kinetic energy the
9. (a) The rest length L0 = 130 m of the spaceship and its length L as measured by the
timing station are related by Eq. 37-13. Therefore,
L L0 1 (v / c) 2 130 m 1 0.740 87.4 m.
2
(b) The time interva
4. Due to the time-dilation effect, the time between initial and final ages for the daughter
is longer than the four years experienced by her father:
tf daughter ti daughter = (4.000 y)
where is Loren
19. (a) Using the notation of Sample Problem Pointillistic paintings use the diffraction
of your eye,
D
2(50 106 m)(1.5 103 m)
L
019 m .
.
122 d
.
122(650 109 m)
.
(b) The wavelength of the blue ligh
4. (a) Eq. 36-3 and Eq. 36-12 imply smaller angles for diffraction for smaller wavelengths.
This suggests that diffraction effects in general would decrease.
(b) Using Eq. 36-3 with m = 1 and solving
36. (a) On both sides of the soap is a medium with lower index (air) and we are
examining the reflected light, so the condition for strong reflection is Eq. 35-36. With
lengths in nm,
3360 for m = 0
14. (a) For the maximum adjacent to the central one, we set m = 1 in Eq. 35-14 and obtain
1
sin 1
0.010 rad.
m 1
100
m
d
1 sin 1
(b) Since y1 = D tan 1 (see Fig. 35-10(a), we obtain
y1 = (50
90. (a) Now, the lens-film distance is
F 1 1 I F 1 1 IJ
iG J G
H f p K H 5.0 cm 100 cmK
1
1
5.3 cm.
(b) The change in the lens-film distance is 5.3 cm 5.0 cm = 0.30 cm.
1305
40. We use Eq. 34-8 (and Fig. 34-11(d) is useful), with n1 = 1.6 and n2 = 1 (using the
rounded-off value for air):
1.6 1 1 16
.
pi
r
Using the sign convention for r stated in the paragraph following E
47. The law of refraction states
n1 sin 1 n2 sin 2 .
We take medium 1 to be the vacuum, with n1 = 1 and 1 = 32.0. Medium 2 is the glass,
with 2 = 21.0. We solve for n2:
n2 n1
FG
H
IJ
K
sin 32.0
sin 1
33. Let I0 be the intensity of the unpolarized light that is incident on the first polarizing
1
sheet. The transmitted intensity is I1 2 I 0 , and the direction of polarization of the
transmitted ligh
55. We use vS = r (with r = 0.600 m and = 15.0 rad/s) for the linear speed during
circular motion, and Eq. 17-47 for the Doppler effect (where f = 540 Hz, and v = 343 m/s
for the speed of sound).
(a)
38. The frequency is f = 686 Hz and the speed of sound is vsound = 343 m/s. If L is the
length of the air-column, then using Eq. 1741, the water height is (in unit of meters)
h 1.00 L 1.00
nv
n(343)
6. Let be the length of the rod. Then the time of travel for sound in air (speed vs) will
be ts / vs . And the time of travel for compressional waves in the rod (speed vr) will be
tr / vr . In these t
18. The volume of a cylinder of height is V = r2 = d2 /4. The strings are long,
narrow cylinders, one of diameter d1 and the other of diameter d2 (and corresponding
linear densities 1 and 2). The mass
51. (a) Setting h / p h /
b E / cg m c , we solve for K = E m c :
2
22
e
e
2
2
1240eV nm
2
hc
K me2 c 4 me c 2
0.511MeV 0.511MeV
3
10 10 nm
0.015 MeV 15 keV.
2
(b) Using the value hc 1240eV n