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78. (a) Using Eq. 377, we expect the dilated time intervals to be
τγτ
τ
==
−
0
0
2
1(/)
.
vc
(b) We rewrite Eq. 3731 using the fact that period is the reciprocal of frequency
(
f
RR
=
−
1
and
f
00
1
=
−
):
β
R
R
f
f
cv
−
+
F
H
G
I
K
J
=
+
−
=
+
−
−
11
1
1
1
0
1
.
(c) The Doppler shift combines two physical effects: the time dilation of the moving
source
and
the traveltime differences involved in periodic emission (like a sine wave or
a series of pulses) from a traveling source to a “stationary” receiver). To isolate the
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This note was uploaded on 06/03/2011 for the course PHY 2049 taught by Professor Any during the Spring '08 term at University of Florida.
 Spring '08
 Any
 Physics

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