phy 113 c general physics i 11 am – 12:15 pm tr olin 101 plan for lecture 16:

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10/22/2013 PHY 113 C Fall 2013 -- Lecture 16 1 PHY 113 C General Physics I 11 AM – 12:15 PM TR Olin 101 Plan for Lecture 16: Chapter 16 – Physics of wave motion 1.Review of SHM 2.Examples of wave motion 3.What determines the wave velocity 4.Properties of periodic waves

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PHY 113 C General Physics I 11 AM – 12:15 PM TR Olin 101 Plan for Lecture 16: Chapter 16 – Physics of wave motion Review of SHM Examples of wave motion What determines the wave velocity Properties of periodic waves. Some comments on Simple Harmonic Motion. k. m =1 kg. - PowerPoint PPT Presentation

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Page 1: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 110/22/2013

PHY 113 C General Physics I11 AM – 12:15 PM TR Olin 101

Plan for Lecture 16:Chapter 16 – Physics of wave motion

1. Review of SHM2. Examples of wave motion3. What determines the wave velocity4. Properties of periodic waves

Page 2: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 210/22/2013

Page 3: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 310/22/2013

Some comments on Simple Harmonic Motion

k

mktAtx

xmk

dtxddtxdmmakxF

2

2

2

2

2

ωthatprovided

)φω(cos)( :solution general

:equation aldifferenti

Suppose that you know: (in standard units)

x(t)=2 cos(2pt+3p)

What is k ? k = m(2p)2

m=1 kg

Page 4: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 410/22/2013

Some comments on Simple Harmonic Motion

k

mktAtx

xmk

dtxddtxdmmakxF

2

2

2

2

2

ωthatprovided

)φω(cos)( :solution general

:equation aldifferenti

Suppose that you know: (in standard units)

x(t)=2 cos(2pt+3p)

What is the frequency of oscillations ? w=2pf=2p f=1 Hz

m=1 kg

Page 5: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 510/22/2013

Some comments on Simple Harmonic Motion

k

mktAtx

xmk

dtxddtxdmmakxF

2

2

2

2

2

ωthatprovided

)φω(cos)( :solution general

:equation aldifferenti

Suppose that you know: (in standard units)

x(t)=2 cos(2pt+3p)

What is amplitude of the displacement ? xmax=2m

m=1 kg

Page 6: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 610/22/2013

Some comments on Simple Harmonic Motion

k

mktAtx

xmk

dtxddtxdmmakxF

2

2

2

2

2

ωthatprovided

)φω(cos)( :solution general

:equation aldifferenti

Suppose that you know: (in standard units)

x(t)=2 cos(2pt+3p)

What is the maximum velocity ? v(t)=-2(2p) cos(2pt+3p) vmax=4p

m=1 kg

Page 7: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 710/22/2013

Some comments on Simple Harmonic Motion

k

mktAtx

xmk

dtxddtxdmmakxF

2

2

2

2

2

ωthatprovided

)φω(cos)( :solution general

:equation aldifferenti

Suppose that you know: (in standard units)

x(t)=2 cos(2pt+3p)

What is the maximum acceleration ? a(t)=-2(2p)2 cos(2pt+3p) amax=8p2

m=1 kg

Page 8: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 810/22/2013

Some comments on Simple Harmonic Motion

k

mktAtx

xmk

dtxddtxdmmakxF

2

2

2

2

2

ωthatprovided

)φω(cos)( :solution general

:equation aldifferenti

Suppose that you know: (in standard units)

x(t)=2 cos(2pt+3p)

What is the displacement at t=0.3 s ? x(0.3)=2 cos(2p(0.3)+3p) =2(0.309)=0.618 m

m=1 kg

Page 9: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 910/22/2013

Some comments on driven Simple Harmonic Motion

k

)

)

)

mk

tmFtAtx

tFxmk

dtxd

dtxdmmatFkxF

2

220

02

2

2

2

0

ω where

sin/)φω(cos)( :solution general

sin :equation aldifferenti

sin

w

F(t)=F0sin(t)

Page 10: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1010/22/2013

Webassign question (Assignment 14)

Damping is negligible for a 0.175-kg object hanging from a light, 6.30-N/m spring. A sinusoidal force with an amplitude of 1.70 N drives the system. At what frequency will the force make the object vibrate with an amplitude of 0.430 m?

)mktmFtAtx

2

220 ω sin/)φω(cos)(

w

) 00 amplitude sin)( XtXtx

0

022

00

//

mXF

mk

mkmFX

Page 11: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1110/22/2013

The wave equation

Wave variableWhat does the wave equation mean?Examples Mathematical solutions of wave equation and

descriptions of waves

2

22

2

2

xyc

ty

),( txyposition time

Page 12: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1210/22/2013

Source: http://www.eng.vt.edu/fluids/msc/gallery/gall.htm

Example: Water waves

Needs more sophistocated analysis:

Page 13: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1310/22/2013

Mechanical waves occur in continuous media. They are described by a value (y) which changes in both time (t) and position (x) and are characterized by a wave velocity c: y=f(x-ct) or y=f(x+ct)

Page 14: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1410/22/2013

Waves on a string:

Typical values for c:

3x108 m/s light waves

~1000 m/s wave on a string

343 m/s sound in air

Page 15: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1510/22/2013

Transverse wave:

Page 16: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1610/22/2013

Longitudinal wave:

Page 17: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1710/22/2013

General traveling wave –

t = 0

t > 0

Page 18: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1810/22/2013

iclicker question:

t=0t=1 s t=2s

Page 19: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 1910/22/2013

Basic physics behind wave motion --

example: transverse wave on a string with tension T and mass per unit length m

y

ABT

dtydx

xm

TTdtydm

xy

xyμ

μ

θsinθsin

2

2

AB2

2

qBy

x

BBB x

y θtanθsin

2

2

0 xy

xy1

xy

xLimABx

2

2

2

2

μ xyT

ty

Page 20: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2010/22/2013

The wave equation:

Solutions: y(x,t) = f (x ct)

2

22

2

2

xyc

ty

string) a(for

μ where Tc

function of any shape

) )

) ) )

) ) ) 22

22

2

2

2

2

2

22

2

2

2

2

Let :Note

cuuf

tu

uuf

tuf

uuf

xu

uuf

xuf

xu

uuf

xuf

ctxu

Page 21: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2110/22/2013

iclicker question Is it significant to write the wave equation with the special symbols?

A. YesB. No

2

22

2

2

xyc

ty

Page 22: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2210/22/2013

Examples of solutions to the wave equation:

Moving “pulse”:

Periodic wave:

)20),( ctxeytxy

) )φsin),( 0 ctxkytxy

“wave vector”not spring constant!!!

ωπ2π2λπ2

fT

kc

k

cTT

txytxy

λ φλ

π2sin),( 0

phase factor

Page 23: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2310/22/2013

cTT

txytxy

λ φλ

π2sin),( 0

Periodic traveling waves:

Amplitude

wave length (m)

period (s); T = 1/f

phase (radians)

velocity (m/s)

Page 24: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2410/22/2013

Snapshot of periodic wave at t=t0

Time plot of periodic wave at x=x0

l

1/f

f l = c

Page 25: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2510/22/2013

φ

λπ2sin),( φ

λπ2sin),( 00 T

txytxyTtxytxy leftright

Ttxytxtxy leftright

π2cosφλπ2sin2),(y),( 0

“Standing” wave:

Combinations of waves (“superposition”)

) ) BABABA 21

21 cossin2sinsin

: thatNote

Page 26: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2610/22/2013

Summary of wave properties:

constant) al(fundament /102.9979

:fields magnetic and electric coupled todue Light wave :Example

: density and pressureair with in waveSound :Example

:h mass/lengt and ion with tensstring aon Wave:Example

occurs. avein which w mediumand/or process on the depends speed Wave

8 smc

pcp

TcT

c

mm

Page 27: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2710/22/2013

Example from webassign:

Page 28: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2810/22/2013

cTT

txytxy

λ φλ

π2sin),( 0

Periodic traveling waves:

Amplitude

wave length (m)

period (s); T = 1/f

phase (radians)

velocity (m/s)

Page 29: PHY 113 C General Physics I 11 AM – 12:15 PM  TR  Olin 101 Plan for Lecture 16:

PHY 113 C Fall 2013 -- Lecture 16 2910/22/2013

Example from webassign:

0

0

0

2 :speed e transversmaximum

φλ

π2cos2),(

λ φλ

π2sin),(

yT

Ttxy

Tttxy

cTT

txytxy

p

p