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Q14. Wave Motion
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Q14.Wave Motion

Jan 03, 2016

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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 Presentation
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Page 1: Q14.Wave Motion

Q14. Wave Motion

Page 2: Q14.Wave Motion

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 :

Page 3: Q14.Wave Motion

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 :

Page 4: Q14.Wave Motion

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

Page 5: Q14.Wave Motion

Tv

Larger T larger v

T Mg 1

2T Mg T Mg

Ans: 1 & 3 tied

Page 6: Q14.Wave Motion

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

Page 7: Q14.Wave Motion

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 :

Page 8: Q14.Wave Motion

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

Page 9: Q14.Wave Motion

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 :

Page 10: Q14.Wave Motion

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

Page 11: Q14.Wave Motion

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 :

Page 12: Q14.Wave Motion

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 )

Page 13: Q14.Wave Motion

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 :

Page 14: Q14.Wave Motion

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

Page 15: Q14.Wave Motion

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 :

Page 16: Q14.Wave Motion

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

Page 17: Q14.Wave Motion

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 :

Page 18: Q14.Wave Motion

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

Page 19: Q14.Wave Motion

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

: