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Material Type: Exam; Professor: Fulling; Class: ADV ENGINEERING MATH; Subject: MATHEMATICS; University: Texas A&M University; Term: Unknown 1989;
Typology: Exams
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TRUE, because sin(4) ∼ 4 = O(). (More formally, divide the function by ^3 , getting
sin(4)
which approaches 4 as → 0 and hence is less than a constant for sufficiently small. (In fact, it is less than 4 for all , but that is more than we need to know.))
FALSE, because the extra factor ln ω goes to ∞ as ω → ∞.
FALSE. Although for each fixed t the function approaches 0 as does, that limit is not uniform. For any (no matter how small) we could find many value of t for which the sine factor equals 1 and the t^2 factor is arbitrarily large.
Regular perturbation theory, x ∼ x 0 + x 1 , leads to
0 = x 03 + O(^2 ) + x 02 + 2x 0 x 2 + O(^2 ) + 4.
^0 : x 02 + 4 = 0 ⇒ x 0 = ± 2 i.
^1 : x 03 + 2x 0 x 1 = 0 ⇒ x 0 (−4 + 2x 1 ) = 0 ⇒ x 1 = 2.
Thus x ∼ ± 2 i + 2. The other root must be large, so we expect x^3 ≈ −x^2 , hence x ≈ − 1 /. Therefore, set x ≡ x/, getting
x^3 + x^2 + 4^2 = 0.
Try x ∼ x 0 + ^2 x 2 (since there is no ^1 term in the equation), getting:
^0 : x 03 + x 02 = 0 ⇒ x 0 = − 1.
^1 : 3 x^20 x 2 + 2x 0 x 2 + 4 = 0 ⇒ x 2 = − 4.
Thus x ∼ −
401A-F03 Page 2
Since we are stopping at order , I will systematically discard all terms of order ^2 (without writing “+ · · ·”) and write “∼” instead of “=” to keep the equations legal.
Let τ ∼ (1 + ω 1 )t, (^) dtd ∼ (1 + ω 1 ) (^) dτd. Then
d^2 y dt^2
∼ (1 + ω 1 )^2
d^2 y dτ 2
∼ (1 + 2ω 1 )
d^2 y dτ 2
Now let y ∼ y 0 + y 1. Note first that this turns the derivative initial condition into
0 ∼ (1 + ω 1 )
dy dτ
dy 0 dτ
dy 1 dτ
(0) + ω 1
dy 0 dτ
And, the differential equation expands into
0 ∼ (1 + 2ω 1 )
d^2 y 0 dτ 2
d^2 y 1 dτ 2
d^2 y 0 dτ 2
d^2 y 0 dτ 2
d^2 y 1 dτ 2
Extract the terms of order ^0 from the DE and the IC:
d^2 y 0 dτ 2
dy 0 dτ
The general solution of the DE is y 0 = c 1 cos(2τ ) + c 2 sin(2τ ). Then the IC yield
1 = c 1 , 0 =
− 2 c 1 sin(2τ ) + 2c 2 cos(2τ )
0 = 2c^2.
Thus y 0 (τ ) = cos(2τ ).
Now the terms of order ^1 in the DE:
d^2 y 1 dτ 2
d^2 y 0 dτ 2
− y 03
= 8ω 1 cos(2τ ) − cos^3 (2τ ) = 8ω 1 cos(2τ ) − 14 cos(6τ ) − 34 cos(2τ )
(using the “Possibly useful information” at the last step). To avoid a secular term produced by the resonant forcing terms proportional to cos(2τ ), we must set 8ω 1 = 34. Thus ω 1 = 323. We now know that y 0 = cos
t