physics 1b03summer-lecture 9 wave motion energy and power in sinusoidal waves

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Physics 1B03summer-Lecture 9 Wave Motion Wave Motion •Energy and power in sinusoidal waves

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Page 1: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

Wave MotionWave Motion

•Energy and power in sinusoidal waves

Page 2: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

Energy in Waves

- as waves propagate through a medium, they transport energy

eg: ship moving up and down on a lakeeg: feeling sound waves at a rock concert

- hence, we can talk about energy and the ‘rate of energy transfer’

Page 3: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

Energy and Power

)(amplitudePower Energy, 2

A stretched rope has energy/unit length:

dx

dsdm

For small A and large , we can ignore the difference between “ds”, “dx” :

dm = μ dx (μ = mass/unit length)

Page 4: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

The mass dm vibrates in simple harmonic motion. Its maximum kinetic energy is dKmax = ½(dm)vmax

2

= ½(dm)(ωA)2

dE = ½(dm) ω 2A2

22

21

length)(unit A

E

The average kinetic energy is half this maximum value, but there is also an equal amount of potential energy in the wave. The total energy (kinetic plus potential) is therefore:

To get the energy per unit length (or energy ‘density’), replace the mass dm with the mass per unit length :

Page 5: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

Power: Energy travels at the wave speed v,

So

waves on a string,

lengthEnergy

vP

vAP 2221

Both the energy density and the power transmitted are proportional to the square of the amplitude. This is a general property of sinusoidal waves.

Page 6: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

Example

A string for which μ=5.0x10-2 kg/m is under tension of 80.0 N. How much power must be supplied to the string to generate sinusoidal waves at a frequency of 60Hz and with an amplitude of 6.0 cm ?

Page 7: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

Example

A sinusoidal wave on a string is described by the equation:

y(x,t) = (0.15m)sin(0.80x-50t)

where x is in meters and t in seconds. If μ=12.0g/m, determine:

a) the speed of the wave

b) the speed of particles on the wave at any time

c) the wavelength

d) the frequency

e) the power transmitted to the wave

Page 8: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

Concept Quiz

The sound waves from your 100-watt stereo causes windows across the street to vibrate with an amplitude of 1 mm. If you use a 400-watt amplifier, what sort of amplitude can you get from the windows?

A) 2mmB) 4mmC) 16 mm

Page 9: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

IntensityIntensity

I = Power per unit area

Unit: W / m2

(the area is measured perpendicular to the wave velocity)

Intensity ~ (amplitude)2

source

detectors (area A)

Page 10: Physics 1B03summer-Lecture 9 Wave Motion Energy and power in sinusoidal waves

Physics 1B03summer-Lecture 9

How would the intensity depend on distance from the source for:

1) waves spreading out equally in all directions in space? (This is called an“isotropic” source, or a source of “spherical waves”.)

2) Waves spreading out on a two-dimensional surface, e.g., circular ripples from a stone dropped into water?

How would the amplitude depend on distance?