(kx i t i kx i kx ik x ik ∫∫( 2
Problem 1
MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF OCEAN ENGINEERING
13.811 Advanced Structural Dynamics and Acoustics
Second Half - Problem Set 2 Solution
Using equation (2.52) from text and substituting the expression for p(x,y,0),
( ) P kx , ky =
Poe-it
(ei2kx + e-i2kx )e-ikx xe-ik y ydxdy
- -
=
Poe-it
(e-i(k x -2k ) x + e-i(2k +k x ) x )e-ik y ydxdy
- -
Using equation (1.5) from text,
( ) P kx , ky = 4 [ 2Poe-it ( kx - 2k ) + ( kx + 2k ) ] ( ky )
(1)
Using equation (2.50) and substituting equation (1) above,
1
p(x, y,z) =
=
= Where
I 1
=
[ ] 1
4 2
[4
- -
2 Poe -it
(kx
- 2k) + (kx
+ 2k)
(k y )eikz z ]eikx x eik y y dk x dk y
[ ] Poe-it (k x - 2k ) + (k x + 2k ) eikx xdk x (k y )ei(kz z+k y y)dk y
-
-
[ ] Poe-it (k x - 2k ) + (k x + 2k ) eikx xdk x I1
(2)
-
(k y )ei(kzz+ky y)dk y
-
Using sifting property of the delta function integral (equation (1.37) of text) and recognizing that k z = k 2 -k x 2 -k y 2 ,
2
I 1
=
ei k2 -kx2 z
(3)
Thus, substituting equation (3) above into (2) above,
p(x, y,z) =
[ ] Poe-it
(k x - 2k ) + (k x + 2k ) eikx xei
dk k 2 -kx 2 z x
-
Again, using sifting property of the delta function integral (equation (1.37) of text),
p(x, y,z) =
[ ] Poe-it ei2kxei -3kz + e-i2kxei -3kz
= Poe-ite- 3kz cos(2kx)
p Figure 1. shows the normalized pressure field 20log dB for normalized distance 0 kx 10 and 0 kz 10.
Po
3
p Figure 1. Normalized pressure field 20log in dB
Po for normalized distance 0 kx 10 and 0 kz 10.
4
Problem 2
Using equation (2.61) and let z = z' = 0,
.
W (kx , k y ,0)
=
kz ock
P(kx , k y ,0)
(1)
By recognizing the definition in equation (2.56) and substituting (1) above into the expression,
P(kx , k y ) P(kx , k y ,0)
P(
kx,ky )
ock
kz
.
W(
kx , ky ,0)
(2)
Using equation (2.50) and observing the form of the inverse 2-D Fourier Transform expression given in equation (1.17)
[ ( ) ] p(x,
y,
z
)
=
Fx
F -1 y
-1
P
kx , ky
eikz z
[ ( )] p(x,
y,0)
=
F F -1 -1 xy
P
kx
,
ky
(3)
5
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