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How do we describe this? 10. Wave Motion

How do we describe this? 10. Wave Motion. An initial shape so can we just let the normal modes oscillate at n ? No! Because that initial shape can

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Wave equation needs two spatial and two temporal boundary conditions. Clamped string: y(0,t) = 0 “a certain point in space for all time” y(L,t) = 0 Two spatial boundary conditions Two temporal boundary conditions Initial shape: y(x,0) = “a certain point in time for all space” rather than an analogous second point in time (which could work), try this: Initial velocity:

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Page 1: How do we describe this? 10. Wave Motion. An initial shape so can we just let the normal modes oscillate at  n ? No! Because that initial shape can

How do we describe this?

10. Wave Motion

Page 2: How do we describe this? 10. Wave Motion. An initial shape so can we just let the normal modes oscillate at  n ? No! Because that initial shape can

An initial shape…

…so can we just let the normal modes oscillate at n?

No! Because that initial shape can do many things:

0 L

To get the answer right, we have to get all the boundary conditions right!

Page 3: How do we describe this? 10. Wave Motion. An initial shape so can we just let the normal modes oscillate at  n ? No! Because that initial shape can

2

2

22

2 1ty

vxy

Wave equation needs two spatial and two

temporal boundary conditions.

Clamped string: y(0,t) = 0 “a certain point in space for all time” y(L,t) = 0

Two spatial boundary conditions

Two temporal boundary conditions

Initial shape: y(x,0) = “a certain point in time for all space”

rather than an analogous second point in time (which could work), try this:

Initial velocity: 0,xy

Page 4: How do we describe this? 10. Wave Motion. An initial shape so can we just let the normal modes oscillate at  n ? No! Because that initial shape can

1

cossin,n

nnnn

n txv

Atxy

0,0 ty

0, tLy Lvn

n

0n

shape0, xy sAn '

The velocities tell you how the normal modes move

with different phase offset. But don’t do it this way!!!

0,xy

Page 5: How do we describe this? 10. Wave Motion. An initial shape so can we just let the normal modes oscillate at  n ? No! Because that initial shape can

1

sincossin,n

nnnnn tAtBxv

txy

1

sin0,n

nn Bxv

xy

1

sinn

nBxLn French’s Fourier series!

(spatial boundary conditions)

1

cossinsin,n

nnnnnnn tAtBxv

txy

0sin0,1

nnn

n Axv

xy

Initially at rest?Then An = 0

Page 6: How do we describe this? 10. Wave Motion. An initial shape so can we just let the normal modes oscillate at  n ? No! Because that initial shape can

0 10 20 30 40 50 60 70 80 90 100-0.1

-0.08

-0.06

-0.04

-0.02

0

0.02

0.04

0.06

0.08

0.1