one-dimension wave
DESCRIPTION
One-Dimension Wave. 虞台文. Contents. The Wave Equation of Vibrating String Solution of the Wave Equation Discrete Time Traveling Wave. One-Dimension Wave. The Wave Equation of Vibrating String. u. T 2. Q. . P. . T 1. 0. l. x. x + x. Modeling of Vibrating String. u. T 2. Q. - PowerPoint PPT PresentationTRANSCRIPT
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One-Dimension Wave
虞台文
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Contents
The Wave Equation of Vibrating StringSolution of the Wave EquationDiscrete Time Traveling Wave
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One-Dimension Wave
The Wave Equation of Vibrating String
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Modeling of Vibrating String
.coscos 21 constTTT
2
2
12 sinsint
uxTT
0 l
u
PQ
T1
T2
x x+x
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Modeling of Vibrating String
.coscos 21 constTTT
2
2
12 sinsint
uxTT
0 l
u
PQ
T1
T2
x x+x
2
2
1
1
2
2
cos
sin
cos
sin
t
u
T
x
T
T
T
T
2
2
tantant
u
T
x
xx
u
tan
xxx
u
tan
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Modeling of Vibrating String
0 l
u
PQ
T1
T2
x x+x
2
2
1
1
2
2
cos
sin
cos
sin
t
u
T
x
T
T
T
T
2
2
tantant
u
T
x
xx
u
tan
xxx
u
tan
2
2
1
x x x
u u u
x x x T t
2
2
22
2 1
t
u
cx
u
2
2
22
2 1
t
u
cx
u
Tc2
Tc2
2
2
x
u
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1D Wave Equation
2
2
22
2 1
t
u
cx
u
2
2
22
2 1
t
u
cx
u
u(x, t) = ?
Boundary Conditions:
Initial Conditions:
ttlutu allfor 0),( ,0),0(
)()0,( xfxu )(),(
0
xgt
txu
t
0 l
u
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One-Dimension Wave
Solution of the
Wave Equation
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Separation of Variables
2
2
22
2 1
t
u
cx
u
2
2
22
2 1
t
u
cx
u
).()(),( tGxFtxu Assume
GFt
u
2
2
GFx
u
2
2
GFcGF 2
F
F
Gc
G
2
functionof t
functionof x
k
constantwhy?
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Separation of Variables
F
F
Gc
G
2
k
0 kFF 0 kFF
02 kGcG 02 kGcG
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Separation of Variables
0 kFF 0 kFF
02 kGcG 02 kGcG
).()(),( tGxFtxu
Boundary Conditions:0),( ,0),0( tlutu
0)()0(),0( tGFtu
0)()(),( tGlFtlu
Case 1:
Case 2:
G(t) 0
F(0) = 0F(l ) =0
不是我們要的不是我們要的
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Separation of Variables
0 kFF 0 kFF
Boundary Conditions:
F(0) = 0, F(l) =0
F(x) = ?
Three Cases: k = 0> 0
< 0
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k = 0
0 kFF 0 kFF
Boundary Conditions:
F(0) = 0, F(l) =0
F(x) = ?
0F
baxxF )(
a = 0 and b = 0
不是我們要的不是我們要的
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k =2 (>0)
0 kFF 0 kFF
Boundary Conditions:
F(0) = 0, F(l) =0
F(x) = ?
02 FF
xx BeAexF )(
A = 0B = 0
不是我們要的不是我們要的
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k = p2 (<0)
0 kFF 0 kFF
Boundary Conditions:
F(0) = 0, F(l) =0
F(x) = ?
02 FpFpxBpxAxF sincos)(
0)0( AF
0sin)( plBlF
0B npl
l
np
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k = p2 (<0)
0 kFF 0 kFF
Boundary Conditions:
F(0) = 0, F(l) =0
F(x) = ?
pxBpxAxF sincos)( l
np
xl
nxFn
sin)(Define
Any linear combinationof Fn(x) is a solution.
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k = p2 (<0)
02 kGcG 02 kGcGl
np
02 GG n 02 GG n
l
cnn
tBtBtG nnnnn sincos)( *
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Solution of Vibrating Strings
2
2
22
2 1
t
u
cx
u
2
2
22
2 1
t
u
cx
u
).()(),( tGxFtxu
xl
nxFn
sin)(
tBtBtG nnnnn sincos)( *
l
cnn
,2,1 ,sin)sincos()( *
nxl
ntBtBtu nnnnn
1
*
1
sin)sincos(),(),(n
nnnnn
n xl
ntBtBtxutxu
1
*
1
sin)sincos(),(),(n
nnnnn
n xl
ntBtBtxutxu
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Initial Conditions
)()0,( xfxu
)(0
xgt
u
t
)(sin1
xfxl
nB
nn
01
*
0
sin)cossin(
tnnnnnnn
t
xl
ntBtB
t
u
)(sin1
* xgxl
nB
nnn
1
*
1
sin)sincos(),(),(n
nnnnn
n xl
ntBtBtxutxu
1
*
1
sin)sincos(),(),(n
nnnnn
n xl
ntBtBtxutxu
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Initial Conditions
)()0,( xfxu
)(0
xgt
u
t
)(sin1
xfxl
nB
nn
)(sin1
* xgxl
nB
nnn
l
n xdxl
nxf
lB
0sin)(
2
l
n xdxl
nxf
lB
0sin)(
2
0 l
f(x)
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Initial Conditions
)()0,( xfxu
)(0
xgt
u
t
)(sin1
xfxl
nB
nn
)(sin1
* xgxl
nB
nnn
l
nn xdxl
nxg
lB
0
* sin)(2
l
n xdxl
nxg
cnB
0
* sin)(2
l
n xdxl
nxg
cnB
0
* sin)(2
l
n xdxl
nxf
lB
0sin)(
2
l
n xdxl
nxf
lB
0sin)(
2
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The Solution
2
2
22
2 1
t
u
cx
u
2
2
22
2 1
t
u
cx
u
1
* sin)sincos(),(n
nnnn xl
ntBtBtxu
l
n xdxl
nxg
cnB
0
* sin)(2
l
n xdxl
nxf
lB
0sin)(
2
,2,1n
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Special Case: g(x)=0
2
2
22
2 1
t
u
cx
u
2
2
22
2 1
t
u
cx
u
1
* sin)sincos(),(n
nnnn xl
ntBtBtxu
l
n xdxl
nxg
cnB
0
* sin)(2
l
n xdxl
nxf
lB
0sin)(
2
,2,1n
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Special Case: g(x)=0
1
sincos),(n
nn xl
ntBtxu
l
cnn
)]sin()[sin(2
1cossin )]sin()[sin(
2
1cossin
11
)(sin2
1)(sin
2
1),(
nn
nn ctx
l
nBctx
l
nBtxu
lxxuxfxl
nB
nn
0 ),0,()(sin1
0 l
f(x)
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Special Case: g(x)=0)]sin()[sin(
2
1cossin )]sin()[sin(
2
1cossin
xxfxl
nB
nn ),(*sin
1
0 l
f*(x)
1
sincos),(n
nn xl
ntBtxu
l
cnn
11
)(sin2
1)(sin
2
1),(
nn
nn ctx
l
nBctx
l
nBtxu
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Special Case: g(x)=0
)](*)(*[2
1),( ctxfctxftxu )](*)(*[
2
1),( ctxfctxftxu
1
sincos),(n
nn xl
ntBtxu
l
cnn
11
)(sin2
1)(sin
2
1),(
nn
nn ctx
l
nBctx
l
nBtxu
xxfxl
nB
nn ),(*sin
1
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Interpretationf*(x) f*(xct)f*(x+ct)
)](*)(*[2
1),( ctxfctxftxu )](*)(*[
2
1),( ctxfctxftxu
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Example)](*)(*[
2
1),( ctxfctxftxu )](*)(*[
2
1),( ctxfctxftxu
0 l 0 l
0 l 0 l
0 l 0 l
0 l 0 l
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One-Dimension Wave
Discrete-Time Traveling Wave
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Discrete-Time Simulation
1 2 1
1 2 1
1 12 4 2