q14.wave motion
DESCRIPTION
Q14.Wave Motion. The displacement of a string carrying a traveling sinusoidal wave is given by. At time t 0 the point at x 0 has velocity v 0 and displacement y 0 . The phase constant is given by tan :. v 0 / w y 0 w y 0 / v 0 w v 0 / y 0 y 0 / w v 0 - PowerPoint PPT PresentationTRANSCRIPT
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Q14. Wave Motion
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1. The displacement of a string carrying a traveling sinusoidal
wave is given by
1. v0 /y0
2. y0 / v0
3. v0 / y0
4. y0 / v0
5. v0 y0
, sinmy x t y k x t
At time t 0 the point at x 0 has velocity v0 and
displacement y0. The phase constant is given by tan :
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0 sinmy y
0 cosmv y
0
0
tany
v
, sinmy x t y k x t
, cosmv x t y k x t
1. The displacement of a string carrying a traveling sinusoidal wave is given by
, sinmy x t y k x t
At time t 0 the point at x 0 has velocity v0 and displacement y0.
The phase constant is given by tan :
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2. The diagram shows three identical strings that have been put
under tension by suspending masses of 5 kg each. For
which is the wave speed the greatest ?
1. 1
2. 2
3. 3
4. 1 and 3 tie
5. 2 and 3 tie
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Tv
Larger T larger v
T Mg 1
2T Mg T Mg
Ans: 1 & 3 tied
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3. The tension in a string with a linear density of 0.0010 kg/m is
0.40 N. A 100 Hz sinusoidal wave on this string has a
wavelength of :
1. 0.05 cm
2. 2.0 cm
3. 5.0 cm
4. 20 cm
5. 500 cm
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Tv
1v T
f f
0.401
0.2 20100 0.0010 /
Nm cm
Hz kg m
3. The tension in a string with a linear density of 0.0010 kg/m is
0.40 N. A 100 Hz sinusoidal wave on this string has a
wavelength of :
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4. Suppose the maximum speed of a string carrying a sinusoidal
wave is vs. When the displacement of a point on the string
is half its maximum, the speed of the point is :
1. vs / 2
2. 2 vs
3. vs / 4
4. 3 vs / 4
5. 3 vs / 2
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sinmy y k x t cosmv y k x t
s mv y
1
2 my y 1sin
2k x t
2
1 3cos 1
2 2k x t
3 3
2 2m sv y v
4. Suppose the maximum speed of a string carrying a sinusoidal wave is vs.
When the displacement of a point on the string is half its maximum, the
speed of the point is :
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5. Two sinusoidal waves have the same angular frequency, the
same amplitude ym, and travel in the same direction in the
same medium. If they differ in phase by 50°, the amplitude
of the resultant wave is given by :
1. 0.64 ym
2. 1.3 ym
3. 0.91 ym
4. 1.8 ym
5. 0.35 ym
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1
2
sin
sinm
m
y y
y y
Amplitude
50
180
1 2 sin sinmy y y 2 sin cos2 2my
k x t
2 cos 1.812m my y
5. Two sinusoidal waves have the same angular frequency, the
same amplitude ym, and travel in the same direction in the
same medium. If they differ in phase by 50°, the amplitude
of the resultant wave is given by :
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6. The sinusoidal wave y(x,t) ym sin( k x – t ) is incident
on the fixed end of a string at x L. The reflected wave is
given by :
1. ym sin( k x + t )
2. –ym sin( k x + t )
3. ym sin( k x + t – k
L )
4. ym sin( k x + t – 2
k L )
5. –ym sin( k x + t + 2
k L )
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0, sinrefl my x t y k x L t t
Let the time of incidence be t0
0 0 0, sin 0 ,in m refly L t y k L t y L t
0sinmy k x t k L t
sin 2my k x t k L
0k L t
6. The sinusoidal wave y(x,t) ym sin( k x – t ) is incident
on the fixed end of a string at x L. The reflected wave is
given by :
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7. Standing waves are produced by the interference of two
traveling sinusoidal waves, each of frequency 100 Hz. The
distance from the 2nd node to the 5th node is 60 cm. The
wavelength of each of the two original waves is :
1. 50 cm
2. 40 cm
3. 30 cm
4. 20 cm
5. 15 cm
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1 siny A k x t
In order to have a standing wave, these waves must travel in opposite directions.
2 siny A k x t
1 2 sin cos2 2
y y A t k x
Distance from the 2nd node to the 5th node is 60 cm :
260 5 2cm
40 cm
7. Standing waves are produced by the interference of two traveling sinusoidal
waves, each of frequency 100 Hz. The distance from the 2nd node to the
5th node is 60 cm. The wavelength of each of the two original waves is :
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8. A stretched string, clamped at its ends, vibrates in its
fundamental frequency. To double the fundamental
frequency, one can change the string tension by a factor of :
1. 2
2. 4
3. 2
4. 1 /
2
5. 1 /
2
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2T v
Clamped at ends & fundamental mode fixed
v fk
2T f
2 4f f T T
8. A stretched string, clamped at its ends, vibrates in its
fundamental frequency. To double the fundamental
frequency, one can change the string tension by a factor of :
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9. A 40-cm long string, with one end clamped and the other free
to move transversely, is vibrating in its fundamental standing
wave mode. If the wave speed is 320 cm/s, the frequency is
:
1. 32
Hz
2. 16
Hz
3. 8
Hz
4. 4
Hz
5. 2
Hz
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320 /
24 40
cm svf Hz
cm
One end clamped and the other free to move transversely.
Fundamental standing wave mode 4 L.
9. A 40-cm long string, with one end clamped and the other free
to move transversely, is vibrating in its fundamental standing
wave mode. If the wave speed is 320 cm/s, the frequency is
: