Lecture 12 13m
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Transcript of Lecture 12 13m
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Transverse waves
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Transverse waves on a string
T
x
y
x = y = 0
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Horizontal forces:
Vertical forces:
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Solution of the wave equation
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Boundary conditions
l
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Missing modes by arbitrary plucking
F
X
All those modes having a node at X would be missing.
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F
Arbitrary disturbance may be expressed by a Fourier series
with appropriate strengths of different modes.
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Reflection and transmission of waves
Y
X=0
TT
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Boundary conditions
X=0
Y
XNot possible
T
T
X=0
Y
XPossible
TT
X=0
Y
X
Not possible
TT
X=0
Y
X
Possible
T T
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1
1 1
i r
x xY f t f t
c c
2
2
t
xY f t
c
0 0( ) i r ti Y Y f t f t f t Boundary conditions at X=0 for all time:
120 0
( )i r t
cY Yi i f t f t f t
x x c
12
( )i r t
cf t f t f t K t
c
12
i r t
cf t f t f t
c As K=0,
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Reflection coefficient
At X = 0
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Transmission coefficient
At X = 0
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Stokes relations
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Note
But
At X=0 for all time
with and
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Setting
We also have
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Special cases
Case 1:
Change in sign of reflected pulse
Abrupt phase change of on reflection
1 2 1 2 12 0c c r
Case 2:1 2 1 2 12
0c c r
No change in sign of reflected pulse
No abrupt phase change on reflection
At the knot or joint (X = 0)
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Case 3: for both the cases
No phase change on transmission
Case 4: At a fixed knot/joint
Total reflection with an inversion of shape
Case 5: At a free end with
Total reflection without inversion of shape
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Case 6: Impedance matching at the joint
Total transmission without reflection