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Page 1: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Strings

1

The two ends must be nodes (because they are fixed).

Nodes (N) and anti-nodes (A) are separated by λ/4

For the nth normal mode: L=n�

2We call this value :�n

�n=2L

n f n=v

�n=n

2Lv=

n

2L � T�=nf 1 n=1,2,3,...

Page 2: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Strings

2

Example 14.3

A middle C string on a piano has a fundamental frequency of 262 Hz and the A note has a frequency of 440 Hz.

[A] Calculate the frequencies of the next two harmonics of the C string.

f n=nf 1

f 2=2f 1=524Hz

f 3=3f 1=786Hz

Page 3: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Strings

3

Example 14.3

A middle C string on a piano has a fundamental frequency of 262 Hz and the A note has a frequency of 440 Hz.

[B] If the strings for the A and the C notes are assumed to have the same mass per unit length and the same length,

determine the ratio of the tensions in the two strings.

f 1A=vA

2L=

1

2L � T A� f 1C=vC

2L=

1

2L � T C�Note:

Velocity of the transverse wave for the A note is NOT the same as the velocity for the C note.

The wavelength of the fundamental is 2L in both cases.

Page 4: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Strings

4

Example 14.3

A middle C string on a piano has a fundamental frequency of 262 Hz and the A note has a frequency of 440 Hz.

[B] If the strings for the A and the C notes are assumed to have the same mass per unit length and the same length,

determine the ratio of the tensions in the two strings.

f 1A

f 1C

=� T AT C

Key: If one takes ratios of frequencies the common constants � and L get divided out.

So: and:T A

T C=f 1A

2

f 1C

2=

4402

2622=2.82

To tune it to A you will need to make the string ~ 3 times as taut.

Page 5: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Differences with Standing Waves in Strings and Pipes

5

Standing waves in strings are transverse waves

Standing waves in pipes are longitudinal sound waves

Note: You can only �hear� longitudinal waves, because transverse waves do not propagate through air or liquid, only through solid.

To �hear� the string, the transverse waves on the string have to excite longitudinal sound waves in the air which then reach your

ear drum �

Page 6: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Differences with Standing Waves in Strings and Pipes

6

Strings: Ends are always nodes

Pipes: � Closed ends are nodes� Open ends are anti-nodes

DidgeridooOne open end & one closed end

Bamboo fluteTwo open ends

Image from grapevineroad.orgImage from i235.photobucket.com

Page 7: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Pipes (Air Columns)

7

http://www.youtube.com/watch?v=QSXjpWUDvO4

Wikipedia: For humans, hearing is normally limited to frequencies between about 12 Hz and 20,000 Hz (20 kHz),

although these limits are not definite.

The didgeridoo fundamental frequency is closer to the bottom end � I estimate the one we heard to be about 80-90 Hz.

After hearing this, you decide to make yourself a didgeridoo with a PVC pipe from the hardware store.

How long should this pipe be in order to have a fundamental frequency of 80 Hz?

Page 8: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Open Pipes

8

The two ends must be anti-nodes.

Nodes (N) and anti-nodes (A) are separated by λ/4

For the 1st normal mode: L=�

2We call this value :�1

�1=2L

NAA

L

Page 9: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Open Pipes

9

The second normal mode has 1 anti-node in the centre as well.

Nodes (N) and anti-nodes (A) are separated by λ/4

For the 2nd normal mode: L=�

We call this value :�2

�2=L

N NAA A

L

Page 10: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Open Pipes

10

The third normal mode has 2 anti-nodes in the centre as well.

Nodes (N) and anti-nodes (A) are separated by λ/4

For the 3rd normal mode:L=3

2We call this value :�3

�3=2L

3

N NA AN AA

L

Page 11: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Open Pipes

11

For the nth normal mode, there will be n-1 antinodes in between.

Nodes (N) and anti-nodes (A) are separated by λ/4

For the nth normal mode: L=n�

2We call this value :�n

�n=2L

nf n=

v

�n=n

v

2L=nf 1 n=1,2,3,...

NA

NA

NA

NA

NAA

L

Page 12: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Notation

12

Standing Waves in (both-end) Open Pipes

First Harmonic: n = 1Second Harmonic: n = 2

Third Harmonic: n = 3

f n=v

�n=n

v

2L=nf 1 n=1,2,3,4,...

Page 13: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Pipes:One end open, one end closed

13

Open end: anti-nodeClosed end: node

Nodes (N) and anti-nodes (A) are separated by λ/4

For the 1st normal mode: L=�

4We call this value :�1

�1=4L

AN

Page 14: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Pipes:One end open, one end closed

14

Open end: anti-nodeClosed end: node

Nodes (N) and anti-nodes (A) are separated by λ/4

For the 2nd normal mode: L=3�

4We call this value :�3

�3=4L

3

AN

AN

Page 15: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Pipes:One end open, one end closed

15

Open end: anti-nodeClosed end: node

Nodes (N) and anti-nodes (A) are separated by λ/4

For the 3rd normal mode: L=5�

4We call this value :�5

�5=4L /5

AN

A ANN

Page 16: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Standing Waves in Pipes:One end open, one end closed

16

Open end: anti-nodeClosed end: node

Nodes (N) and anti-nodes (A) are separated by λ/4

In general for n = 1, 3, 5, 7 ....L=n�

4We call this value :�n

�n=4L /n

AN

A ANN

f n=v

�n=n

v

4L=nf 1 n=1,3,5,...

AN

Page 17: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Notation

17

Standing Waves in (both-end) Open Pipes

First Harmonic: n = 1Second Harmonic: n = 2

Third Harmonic: n = 3

f n=v

�n=n

v

2L=nf 1 n=1,2,3,4,...

Standing Waves in one-end-Open one-end-Closed Pipes

f n=v

�n=n

v

4L=nf 1 n=1,3,5,7,...

First Harmonic: n = 1Third Harmonic: n = 3Fifth Harmonic: n = 5

Only odd harmonics are present !

Page 18: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

The PVC Didgeridoo

18

We want the fundamental frequency to be 80 Hz.

One end of the pipe is effectively closed (at your mouth)

f n=v

�n=n

v

4L=nf 1 n=1,3,5...

L=v

4f 1

=343m.s

�1

320 s�1

=1.1m

Page 19: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

A PVC middle-C Flute

19

We want the fundamental frequency to be middle-C : 262 Hz.

You blow across the hole: so the hole is actually open to the atmosphere. So this would be a two-end-open pipe.

f 1=v

2L

L=v

2f 1

=343m.s

�1

2�262 s�1=0.65m

Page 20: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

�Beats�: The Sum of Two Sine Waves of Slightly Different Frequency

y1�t�=Asin �kx�1 t�

1=2 f 1 2=2 f 2 �=1�2=2� f 1� f 2�

y2 �t �=Asin �kx�2 t �

=A sin�kx�����t �

Page 21: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

�Beats�: The Sum of Two Sine Waves of Slightly Different Frequency

21

Page 22: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

�Beats�: The Sum of Two Sine Waves of Slightly Different Frequency

22

y1�t�=Asin �kx�1 t�y2 �t �=A sin �kx�2 t�= A sin �kx��

1���t �

0 . 5 1 . 0 1 . 5 2 . 0 2 . 5 3 . 0

� 1 0

� 5

5

1 0

0 . 5 1 . 0 1 . 5 2 . 0 2 . 5 3 . 0

� 1 0

� 5

5

1 0

+

Page 23: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

�Beats�: The Sum of Two Sine Waves of Slightly Different Frequency

23

y1�t�=Asin �kx�1 t�y2 �t �=A sin �kx�2 t�= A sin �kx��

1���t �

0 . 5 1 . 0 1 . 5 2 . 0 2 . 5 3 . 0

� 2 0

� 1 0

1 0

2 0

=

Page 24: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

How about Square Waves (instead of sines and cosines)?

24

Page 25: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

25

�0.09 A1 sin2�5f 1�t�0.0027 A1 sin2�7f 1� t

Page 26: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Constructing a Square Wave from a sum of sines...

26

Harmonics :f 1 ,3 f 1 y �t �=A1 sin2 f 1t�0.3�A1 sin2�3f 1�t

Page 27: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Constructing a Square Wave from a sum of sines...

27

Harmonics :f 1 ,3 f 1, 5f 1

y �t �=A1 sin2 f 1t�0.3�A1 sin2�3f 1�t

�0.09 A1 sin2�5f 1�t

Page 28: Standing Waves in Strings - Memorial University of ...anand/teaching/p1051ay/lectures/SoundWaves... · Differences with Standing Waves in Strings and Pipes 5 ... One open end & one

Constructing a Square Wave from a sum of sines...

28

Harmonics :f 1 ,3 f 1, 5f 1

y �t �=A1 sin2 f 1t�0.3�A1 sin2�3f 1�t

�0.09 A1 sin2�5f 1�t�0.0027 A1 sin2�7f 1� t