this week – ch. 14 – waves next week – ch. 8 – gravity...

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This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity Homework due 11/26, 5 pm (both chapters) No labs or quiz next week Quiz this week – Oscillations [Natural frequency, relation between amplitude, velocity, acceleration, energy]

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Page 1: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

This week – Ch. 14 – WavesNext week – Ch. 8 – GravityHomework due 11/26, 5 pm (both chapters)

No labs or quiz next week

Quiz this week – Oscillations[Natural frequency, relation between amplitude, velocity, acceleration, energy]

Page 2: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

Resonance

  

md2xdt2

=F0cosDt−kx

Page 3: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

x=xdxh

md2xddt2

kxd=F0cosD t Driven

md2xhdt2

kxh=0 Homogeneous

xd=AdcosDt Driven

xh=Acos0 t

Page 4: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

Waves – Physical changes that move through space and change in time

LongitudinalConducting medium moves along wave direction.

Sound, p-waves

TransverseMedium moves perpindicular to wave direction

Water waves, light, radio, s-waves

Page 5: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,
Page 6: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,
Page 7: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

Wave Properties

Wavelength Wave number

FrequencyAngular Frequency

Period

Speed

m

k=2m−1

f Hz cycles /sec s−1 rad /sec

http://phet.colorado.edu/simulations/sims.php?sim=Wave_on_a_String

T=1f=2

s

v=f =

km /s

Page 8: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

Wave Speeds

Depend on medium “Stiffer” media havefaster waves. More massive media have slower waves.

vSOUND= P

=330m /s air ,STP

vSOUND=1500m /s water

vSOUND=5000m /s granite

vLIGHT=c=3×108m /s vacuum

vROPE=F m /s

Page 9: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

The four strings of a musical instrument are all made of the same material and are under the same tension, but have different thicknesses. Waves travel

A. fastest on the thickest string

B. fastest on the thinnest string

C. at the same speed on all strings

D. not enough information given to decide

Page 10: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

If you double the wavelength λ of a wave on a string, what happens to the wave speed v and the wave frequency f?

A. v is doubled and f is doubled

B. v is doubled and f is unchanged

C. v is unchanged and f is halved

D. v is unchanged and f is doubled

E. v is halved and f is unchanged

Page 11: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

Formulae for sinusoidal waves

y=Acosk x− t

y=Acos2x−2Tt

Page 12: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

A wave on a string is moving to the right. This graph of y(x, t) versus coordinate x for a specific time t shows the shape of the wave at that time.

What are the velocity and acceleration of a particle at point P on the string?

A. velocity is upward and acceleration is zero

B. velocity is downward and acceleration is zero

C. velocity is zero and acceleration is upward

D. velocity is zero and acceleration is downward

E. none of the above

Page 13: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,

A wave on a string is moving to the right. This graph of y(x, t) versus coordinate x for a specific time t shows the shape of the wave at that time.

What are the velocity and acceleration of a particle at point Q on the string?

A. velocity is upward and acceleration is zero

B. velocity is downward and acceleration is zero

C. velocity is zero and acceleration is upward

D. velocity is zero and acceleration is downward

E. none of the above

Page 14: This week – Ch. 14 – Waves Next week – Ch. 8 – Gravity ...kestrel.nmt.edu/~rsonnenf/phys121/lectures/F2008Class32.pdf · If you double the wavelength λ of a wave on a string,