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March 25, 2014 Musical Instruments and Geometric Optics

March 25, 2014 Musical Instruments and Geometric Optics

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March 25, 2014 Musical Instruments and Geometric Optics. This is how the picture was taken. Two plane mirrors Were facing each other with The candle in between. Announcements & Reminders. To the teacher: Turn on the recording! To students: About equipment needed for L17. L149, Problem 1. - PowerPoint PPT Presentation

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Page 1: March 25, 2014 Musical Instruments and Geometric Optics

March 25, 2014

Musical Instrumentsand

Geometric Optics

Page 2: March 25, 2014 Musical Instruments and Geometric Optics

This is how the picture wastaken. Two plane mirrorsWere facing each other withThe candle in between.

Page 3: March 25, 2014 Musical Instruments and Geometric Optics

Announcements & Reminders• To the teacher: Turn on the recording!•  

• To students: • About equipment needed for L17

Page 4: March 25, 2014 Musical Instruments and Geometric Optics

B = 2683 Hzf = B/2 = 427.0 HzFrequency printed on tuning fork = 426. 6 Hz

L149, Problem 1

Page 5: March 25, 2014 Musical Instruments and Geometric Optics

B = 1608 Hzf = B/2 = 255.9 HzFrequency printed on tuning fork = 256 Hz

n1 = 256 Hz

n2 = 2x256 Hz n6 = 6x256 Hz

L149, Problem 2

Page 6: March 25, 2014 Musical Instruments and Geometric Optics

B = 9498 Hzf = B/2 = 1512 Hz

vsound = 344 m/s at 21 oC= v/f = 0.23 m

The wavelength is the length of the pipe. This requires the waveform shown to the right. n = 2

A N A N A

L149, Problem 3

Page 7: March 25, 2014 Musical Instruments and Geometric Optics

B = 1.502E4 Hzfn = B/2 = 2391 Hz

From the last problem,f2 = 1512 Hz.

Thus, f1 = f2/2 = 756 Hz.

n = 6

n = 2391 / 756 Hz = 3.16

This must be the3rd harmonic.

L149, Problem 4

Page 8: March 25, 2014 Musical Instruments and Geometric Optics

B = 2682 Hzfn = B/2 = 427 Hz

From the last problem,f1 = 756 Hz.

L149, Problem 5

The frequency is 0.56f1. Thisis approximately an octavelower and may be produced byclosing the end of the pipe asseen in P211.

Why isn’t the frequency exactly an octave lower than the fundamental of the open pipe? The effective lengths of the open and closed pipes may be different. For a closed pipe with a fundamental of 427 Hz, the wavelength is= (344 m/s)/(427 Hz) = 0.806 m. For the fundamental of a closed pipe Lc = /4. In this case, that gives Lc = 0.203 m. A smaller length would make sense, since closing the end prevents the waveform from extending beyond the end of the pipe.

Page 9: March 25, 2014 Musical Instruments and Geometric Optics

Harmonics of a Longer Toy Flute

Page 10: March 25, 2014 Musical Instruments and Geometric Optics

f1 = 546 Hz

Page 11: March 25, 2014 Musical Instruments and Geometric Optics

f2 = 1087 Hz (2f1 = 1092 Hz)

Page 12: March 25, 2014 Musical Instruments and Geometric Optics

n = 2 n = 4 n = 6 n = 8

Page 13: March 25, 2014 Musical Instruments and Geometric Optics

Waveforms and Frequency Spectra of Various Instruments

Page 14: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Justin Luo

Page 15: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Ashwin Monian

Page 16: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Hunter Denham

Page 17: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Jennie Cunningham

Page 18: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Hayden Rudd

Page 19: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Jesse Sykes

Page 20: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Will King

Page 21: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Will King

Page 22: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Charles Zhao

Page 23: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Arjun Adhia

Page 24: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Drew Smith

Page 25: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Trey Faddis

Page 26: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Param Sidhu

Page 27: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Hunter Denham

Page 28: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Kayla Howes

Page 29: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Michael Schroeder

Page 30: March 25, 2014 Musical Instruments and Geometric Optics

waveform by Jesse Sykes

Page 31: March 25, 2014 Musical Instruments and Geometric Optics

Mirror Diagnostic Questions

Page 32: March 25, 2014 Musical Instruments and Geometric Optics

The mirror is grayed out sothat you can’t see whetherit’s plane, convex, or concave.The object is the black, uprightarrow, and the image is thegray, inverted arrow.

1.Is the mirror plane or curved?

Page 33: March 25, 2014 Musical Instruments and Geometric Optics

The mirror is grayed out sothat you can’t see whetherit’s plane, convex, or concave.The object is the black, uprightarrow, and the image is thegray, inverted arrow.

1.The mirror is curved. (The object and image are different sizes.)

2.Is the image real or virtual?

Page 34: March 25, 2014 Musical Instruments and Geometric Optics

The mirror is grayed out sothat you can’t see whetherit’s plane, convex, or concave.The object is the black, uprightarrow, and the image is thegray, inverted arrow.

1.The mirror is curved. (The object and image are different sizes.)

2.The image is real. (Light rays actually converge at the position of the image.)

3.Is the mirror convex or concave?

Page 35: March 25, 2014 Musical Instruments and Geometric Optics

The mirror is grayed out sothat you can’t see whetherit’s plane, convex, or concave.The object is the black, uprightarrow, and the image is thegray, inverted arrow.

1.The mirror is curved.

2.The image is real.

3.The mirror is concave. (A convex mirror won’t produce a real image of a real object.)

Page 36: March 25, 2014 Musical Instruments and Geometric Optics

Everything is revealed here.

o = object distance i = image distance f = focal lengthM = magnification

Page 37: March 25, 2014 Musical Instruments and Geometric Optics

Where should the object beplaced so that the image isinverted and the same sizeas the object?

Page 38: March 25, 2014 Musical Instruments and Geometric Optics

Where should the object beplaced so that the image isinverted and the same sizeas the object?

The object must be placedat the center of curvatureof the mirror. This is twicethe focal length.

Page 39: March 25, 2014 Musical Instruments and Geometric Optics

1. Is the image real or virtual?2. What kind of mirror is it?

Page 40: March 25, 2014 Musical Instruments and Geometric Optics

1. The image is virtual. (It’s behind the mirror.)

2. The mirror is concave. (The image is larger than the object.)

Page 41: March 25, 2014 Musical Instruments and Geometric Optics

A convex mirror producesvirtual images smallerthan the object.

Hence the phrase, “Objects in the mirror are closer thanthey appear.”

Page 42: March 25, 2014 Musical Instruments and Geometric Optics

1. Is the image real or virtual?2. What kind of mirror is it?

Page 43: March 25, 2014 Musical Instruments and Geometric Optics

1. The image is virtual.2. The mirror is plane.

Page 44: March 25, 2014 Musical Instruments and Geometric Optics

1. Is the image real or virtual?2. What is the image distance?3. What is the magnification?

Page 45: March 25, 2014 Musical Instruments and Geometric Optics

1. The image is real. 2. The image distance is found using 1/i = 1/f – 1/o. The object distance and focal length are read from the scale. o = 12.0 cm and f = 10.0 cm. This gives i = 60.0 cm.

3. The magnification is –i/o = -5.00. This also equals the ratio of image height to object height. The negative sign indicates the inversion of the image.

Page 46: March 25, 2014 Musical Instruments and Geometric Optics

1. The image is real. 2. Compare I = 60.0 cm found in the previous slide to 59.9 cm above.

3. Compare M = -5.00 found in the previous slide to -4.99 above.