Chapter 16: Sound 15-9 Standing Waves; Resonance 15-10 Refraction 15-11 Diffraction 16-1...

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Transcript of Chapter 16: Sound 15-9 Standing Waves; Resonance 15-10 Refraction 15-11 Diffraction 16-1...

Chapter 16: Sound

15-9 Standing Waves; Resonance15-10 Refraction15-11 Diffraction16-1 Characteristics of Sound16-3 Intensity of Sound: Decibels16-4 Sources of Sound: Vibrating Strings and Air ColumnsHW2: Chap.16:Pb2,Pb18,Pb24, Pb34,Pb39, Pb 62 , DUE Wed.28

https://www.youtube.com/watch?v=MoVz2ENJb8M

Longitudinal and transverse wave

Pb 11

A

1cm

0.25m The time the valley of the wavemoves is that t=0.25m/1.10m/s

Standing waves occur when both ends of a string are fixed. In that case, only waves which are motionless at the ends of the string can persist. There are nodes, where the amplitude is always zero, and antinodes, where the amplitude varies from zero to the maximum value.

15-9 Standing Waves; Resonance

15-9 Standing Waves; Resonance

The frequencies of the standing waves on a particular string are called resonant or natural frequencies.

They are also referred to as the fundamental and harmonics.

15-9 Standing Waves on a string

•For a given string, the wave speed is a constant, v=√F/µ

•Boundary Condition: Each end of the string must be a node

•Therefore, only certain wavelengths will fit on the string

Fundamental frequency

Second harmonic

Third Harmonic

Fundamental or first harmonic

The wavelengths and frequencies of standing waves are:

15-9 Standing Waves; Resonance

and

15-9 Standing Waves; Resonance

Example 15-8: Piano string.

A piano string is 1.10 m long and has a mass of 9.00 g. (a) How much tension must the string be under if it is to vibrate at a fundamental frequency of 131 Hz? (b) What are the frequencies of the first four harmonics?

If the wave enters a medium where the wave speed is different, it will be refracted—its wave fronts and rays will change direction.

We can calculate the angle of refraction, which depends on both wave speeds: Law of

Refraction

15-10 Refraction

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The law of refraction works both ways—a wave going from a slower medium to a faster one would follow the red line in the other direction.

15-10 Refraction

15-10 Refraction

Example 15-10: Refraction of an earthquake wave.

An earthquake P wave passes across a boundary in rock where its velocity increases from 6.5 km/s to 8.0 km/s. If it strikes this boundary at 30°, what is the angle of refraction?

When waves encounter an obstacle, they bend around it, leaving a “shadow region.” This is called diffraction.

15-11 Diffraction

The amount of diffraction depends on the size of the obstacle compared to the wavelength. If the obstacle is much smaller than the wavelength, the wave is barely affected (a). If the object is comparable to, or larger than, the wavelength, diffraction is much more significant (b, c, d).

15-11 Diffraction

Sound

https://www.youtube.com/watch?v=_vYYqRVi8vY

Sound can travel through any kind of matter, but not through a vacuum.

Sounds cannot travel in absence of matter.

The speed of sound is different in different materials; in general, it is slowest in gases, faster in liquids, and fastest in solids.

The speed depends somewhat on temperature, especially for gases.

16-1 Characteristics of Sound