wing resonance
TRANSCRIPT
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8/3/2019 Wing Resonance
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Luke Anderson
Differential Equations
Rick ReevesApril 20, 2006
Wing Resonance
1. A)
900y '' ( t) C 8100y ( t) = 1800sin(4 t) y ''C 9 y = 2 sin(4 t)
r2C 9 = 0 r=G 3yh = C1cos(3 t) C C2sin(3 t)
yp = A sin(4 t) C B cos(4 t)
y 'p
= 4 Acos(4 t) K 4 Bsin (4 t)
y ' 'p = K 16 Asin (4 t)K 16 Bcos (4 t)
K 16Asin(4 t) K 16Bcos(4 t) C 9 Asin(4 t)C 9 Bcos(4 t) = 2 sin(4 t)
K 7 Asin(4 t) K 7 Bcos(4 t) = 2 sin(4 t)
sin :K 7 A = 2, A =K 7
2
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cosine:K 7 B = 0, B = 0
yp =K 7
2 sin(4 t)
y ( t) =K 2
7 sin(4 t) C C1 cos (3 t) C C2 sin(3 t)
y ( 0) = 0, 0 = C1
y ' ( t) =K 8
7 cos (4 t) K 3 C1 sin (3 t) C 3 C1 cos(3 t)
y ' (0 ) = 0, 0 =K 8
7C 3 C2 , C2 =
8
21
y ( t) = 8sin(3 t)
21K 2
sin(4 t)
7
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f( t) = 1800sin(3 t)
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The main difference between the two forcing functions is that the first one has a shorter
period along with a higher frequency.
B)
900y ''C 8100y = 1800sin(3 t) y ''C 9 y = 2 sin(3 t)
from part A : yh = C1cos(3 t) C C2sin(3 t)
yp = A tsin (3 t) C B tcos(3 t)
y 'p = A sin(3 t) C 3 A tcos(3 t) C B cos(3 t) K 3 tBsin(3 t)
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y ' 'p = 3 A cos(3 t)
C 3 A cos(3 t) K 9 A t sin(3 t) K 3 B sin(3 t) K 3B sin(3 t) K 9 t B cos(3 t)
3 A cos(3 t) C 3 A cos(3 t) K 9 A t sin(3 t) K 3B sin(3 t) K 3 B sin(3 t) K 9 t B cos(3 t)C 9 A t sin(3 t) C 9 B t cos(3 t) = 2 sin (3 t)
6 A cos(3 t) K 6 B sin(3 t) = 3 sin(3 t)
sine : K 6 B = 2, B = K 3
cosine: 6 A = 0, A = 0
yp = K 3 t cos(3 t)
y ( t) = K 3 t cos(3 t) C C1cos(3 t) C C2sin(3 t)
y (0 ) = C1, C1 = 0
y ' ( t) = K 3 cos(3 t) C 9 tsin(3 t) K 3 C1sin(3 t)
C 3 C2cos(3 t)
y (0) = K 3C 3 C2 , C2 = 1
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y ( t) = K 3 tcos(3 t) C sin(3 t)
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As t grows large, there are subsequent larger displacements in the sinusoidal movement
(the amplitude steadily increases). The wings would snap once they are pushed beyond
their maximum tolerance for flexibility.
3. There were certain forces that we did not include in our model. We did not account for
friction from air, or within the wing itself (no damping). We did not include the force
due to lift, drag, or the weight of the plane itself.
An engineer would need to analyze the density and composition of the wings in use.
Analyze. He would need to take into account the thermal conditions of the material or
the environment in which the resonance occurs. Along the same lines, he would also
want to consider the altitude at which this occurs along with the air pressure and how
changes will affect the wing resonance. Also, it would be appropriate to analyze how
much displacement the wing is capable of. Finally, the speeds at which resonance occurs
should be analyzed.