Solutions Test A - Advanced Engineering Mathematics | MATH 401, Exams of Mathematics

Material Type: Exam; Professor: Fulling; Class: ADV ENGINEERING MATH; Subject: MATHEMATICS; University: Texas A&M University; Term: Unknown 1989;

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Pre 2010

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Math. 401 (Fulling) 3 October 2003
Test A Solutions
The limit in question is 0+in all problems, unless otherwise stated.
“Up to [a certain order]” means “stop right before calculating the term of that order.”
“Up through [a certain order]” means do calculate a term of that order.”
1. (15 pts.) Pronounce each of the following assertions true or false, and write something to
explain your judgment.
(a) 2sin(4)=O(
3
).
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.))
(b) ω2ln ω=O(ω2)asω+.
FA L S E , because the extra factor ln ωgoes to as ω→∞.
(c) t2sin(3t)0uniformly in t.
FA L S E . Although for each fixed tthe function approaches 0 as does, that limit is not uniform. For
any (no matter how small) we could find many value of tfor which the sine factor equals 1 and the
t2factor is arbitrarily large.
2. (40 pts.) Find approximations to the roots of
x3+x2+4=0.
Stop each series after you have found two nonzero terms.
Regular perturbation theory, xx0+x1,leadsto
0=x0
3+O(2)+x
0
2+2x
0
x
2
+O(
2
)+4.
0:x
0
2+4=0 x
0=±2i.
1:x0
3+2x
0
x
1=0 x
0
(4+2x
1
)=0 x
1=2.
Thus x∼±2i+2.
The other root must be large, so we expect x3≈−x
2
, hence x≈−1/. Therefore, set xx/,
getting
x3+x2+4
2=0.
Try xx 0+2x 2(since there is no 1term in the equation), getting:
0:x0
3+x0
2=0 x
0=1.
1:3x
2
0
x
2
+2x
0
x
2+4=0 x
2=4.
Thus x∼−1
4.
pf3

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Math. 401 (Fulling) 3 October 2003

Test A – Solutions

The limit in question is  → 0 +^ in all problems, unless otherwise stated.

“Up to [a certain order]” means “stop right before calculating the term of that order.”

“Up through [a certain order]” means “do calculate a term of that order.”

1. (15 pts.) Pronounce each of the following assertions true or false, and write something to

explain your judgment.

(a) ^2 sin(4) = O(^3 ).

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.))

(b) ω−^2 ln ω = O(ω−^2 ) as ω → +∞.

FALSE, because the extra factor ln ω goes to ∞ as ω → ∞.

(c) t^2 sin(3t) → 0 uniformly in t.

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.

2. (40 pts.) Find approximations to the roots of

x^3 + x^2 + 4 = 0.

Stop each series after you have found two nonzero terms.

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

3. (45 pts.) Find a solution up through order  by the Poincar´e (distorted-time) method:

d^2 y

dt^2

+ 4y + y^3 = 0, y(0) = 1,

dy

dt

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

  • 4(y 0 + y 1 ) + y 03

d^2 y 0 dτ 2

  • 2ω 1

d^2 y 0 dτ 2

d^2 y 1 dτ 2

  • 4y 0 + 4y 1 + y 03.

Extract the terms of order ^0 from the DE and the IC:

d^2 y 0 dτ 2

  • 4y 0 = 0, y 0 (0) = 1,

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

  • 4y 1 = − 2 ω 1

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

]