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PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

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Page 1: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

PHY138 – Waves, Lecture 4The Plan for Today:

Sound and Light Medical Applications of Ultrasound

Power and Intensity The Doppler Effect

Page 2: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Reading Assignment Next week’s reading is Knight Chapter 21,

Sections 21.1 – 21.8. There is a pre-class quiz on www.masteringphysics.com for this material due on Monday morning.

A www.masteringphysics.com Problem Set on Chapter 20 is due on Friday at 11:59PM.

A Written Team Problem Set is due next Friday, Nov.24 at 5:00 PM. It’s available in PDF Format on the Waves Class Summaries Page.

Page 3: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Sound and Light Sound is a pressure wave in a gas, liquid or

solid. Speed depends on material. Light is one type of electromagnetic wave. In a vacuum, all electromagnetic waves

(including light) travel at c = 3×108 m/s. In transparent media, light slows down. Index

of Refraction is n > 1. This reduces the wavelength, but does not

change the frequency!

Page 4: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

A light wave travels through three transparent materials of equal thickness. Rank is order, from the largest to smallest, the indices of refraction n1, n2, and n3.

A. n2 > n1 > n3 B. n3 > n1 > n2 C. n1 > n2 > n3

D. n3 > n2 > n1 E. n1 = n2 = n3

Page 5: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Reflection of Transverse Wave Pulse

A pulse traveling to the right on a heavy string attached to a lighter string

Speed suddenly increases

Page 6: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Reflection of Transverse Wave Pulse

A pulse traveling to the right on a light string attached to a heavier string

Speed suddenly decreases

Page 7: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Physics of Ultrasound Speed of sound in bone, flesh and blood

are all different When the speed of any wave suddenly

changes, there is a reflection and transmission

Ultrasound images are formed from reflected high frequency sound

Image resolution is set by wavelength, λ λ=v/f, so higher frequency yields smaller λ,

and better resolution

Page 8: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Speed of sound in humans

Tissue Sound Speed (m/s)

Air 350

Fat 1450

Brain 1540

Blood 1570

Bone 4080

Muscle 1585

Page 9: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Power and Intensity The Power, P, of any wave source is how

much energy per second is radiated as waves [units = Watts]

The Intensity, I, is the energy rate per area. This determines how loud (sound) or bright (light) the wave is.

I=P/a, where a is an area perpendicular to the wave direction.

At a distance r from a spherically symmetric source, the intensity is I=P/(4πr2)

Page 10: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Chapter 20, Problem 34 The sound intensity from a jack hammer

breaking concrete is 2 W/m2 at a distance of 2 m from the point of impact. This is sufficiently loud to cause permanent hearing damage if the operator doesn’t wear ear protection. What is the sound intensity for a person watching from 50 m away?

Page 11: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Doppler Effect

Page 12: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Valerie is standing in the middle of the road, as a police car approaches her at a constant speed, v. The siren on the police car emits a “rest frequency” of f0.

Which statement is true?

A. The frequency she hears rises steadily as the police car gets closer and closer.

B. The frequency she hears steadily decreases as the police car gets closer and closer.

C.The frequency she hears does not change as the police car gets closer.

Page 13: PHY138 – Waves, Lecture 4 The Plan for Today: Sound and Light Medical Applications of Ultrasound Power and Intensity The Doppler Effect

Valerie is standing still as a police car approaches her at a constant speed, v. Daniel is in his car moving at the same constant speed, v, toward an identical police car which is standing still. Both hear a siren.

Which statement is true?

A. The frequency Daniel hears is lower than the frequency Valerie hears.

B. The frequency Daniel hears is higher than the frequency Valerie hears.

C.The frequencies that Daniel and Valerie hear are exactly the same.

(Almost correct)

Actual Answer! Check eq.20.38

and 20.39!