Advanced Engineering Mathematics
Advanced Engineering Mathematics
10th Edition
ISBN: 9780470458365
Author: Erwin Kreyszig
Publisher: Wiley, John & Sons, Incorporated
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1.6. FORCING TERMS: RESONANCES
30
25
25
20
20
15
시
10
5
0
α=0.02
α=0.01
α=0.00
115
0
0.2
0.4
0.6
0.8
1
w
Figure 1.26: The ratio of output to input amplitudes w/VD as a function of
the forcing frequency w for several choices of the damping factor a.
6. The Wronskian of two solutions Y₁(a) and Y2(x) to the homogeneous
equation (1.6.34) is
dy₁
dx
W(x) = Y₁(x) x 2 (x) – Y2(x) (x).
dY2
da
Show that it satisfies the equation,
-
dW
dx
-(x) = -a W(x).
Solve this equation with W(0) = Wo, and show that W(x) is never zero
if Wo 0. What conclusion can you draw from this result?
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Transcribed Image Text:1.6. FORCING TERMS: RESONANCES 30 25 25 20 20 15 시 10 5 0 α=0.02 α=0.01 α=0.00 115 0 0.2 0.4 0.6 0.8 1 w Figure 1.26: The ratio of output to input amplitudes w/VD as a function of the forcing frequency w for several choices of the damping factor a. 6. The Wronskian of two solutions Y₁(a) and Y2(x) to the homogeneous equation (1.6.34) is dy₁ dx W(x) = Y₁(x) x 2 (x) – Y2(x) (x). dY2 da Show that it satisfies the equation, - dW dx -(x) = -a W(x). Solve this equation with W(0) = Wo, and show that W(x) is never zero if Wo 0. What conclusion can you draw from this result?
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