ex3s.pdf

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18.03 Hour Exam III Solutions: April 26, 2006 1. (b) 6 6 6 6 2 2 or 2 2 1 1 1 2 k (b) δ (t) + δ t + δ t = δ t 12 12 + ··· 12 k=0 2. (a) The period of cos(nπt) is 2π/nπ = 2/n, and the least common multiple of these, for n 2, is 2. This is the minimal period. cos(2πt) cos(3πt) cos(4πt) cos(kπt) (b) x p = = (1) k 2 k1 (ω 2 n (2π) 2 ) 4(ω 2 8(ω 2 2(ω 2 n (3π) 2 ) + n (4π) 2 ) −··· n () 2 ) k=2 (c) There is resonance when ω n = for k = 2, 3, 4, . . .. (d) f (t) and cos(πt) are both even, so f (t) cos(πt) is even. Thus 1 1 1 f (t) cos(πt) dt = f (t) cos(πt) dt, and this is zero either because it computes the 0 2 1 Fourier coefficient of cos(πt) in f (t), which is zero, or by the orthogonality properties of the cosine functions, as written in the information page attached to the exam. 3. (a) The denominator s 2 + 4s + 104 = (s + 2) 2 + 100 [the value announced as a correction in the exam room] vanishes at s = 2 ± 10i, so this is where the poles of W (s) are. (b) The poles are relatively near to the imaginary axis, so |W () probably has near- | resonant peaks near ω = ±10. [The gain is an even function of ω, so sketching it for ω > 0 suffices.] The slope becomes zero when ω = 0 (because the function is even), and the graph falls off to zero as ω . for t < a (c) x = u(t a)e I (ta) = 0 e I (ta) for t > a 2 4. (a) (s 2 X (1)s 2) + 4(sX (1)) + 5X = or X = (s 2) + (2/(s 2 + 4)) s 2 + 4 s 2 + 4s + 5 (b) s = (s + 2) 2 (s + 2) 2 + 1 is the Laplace transform of e 2t (cos t 2 sin t) s 2 + 4s + 5 t t 5. (a) x = w(t) f (t) = w(t τ )f (τ ) = (t τ )e (tτ ) f (τ ) . This can also be 0 0 t written τe τ f (t τ ) . 0 d 1 1 (b) W (s) = L 1 [te t ]= = (s + 1) 2 , so W (1) = 1/4 and ds s + 1 t x p = W (1)e t = (1/4)e .

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Page 1: ex3s.pdf

� �

18.03 Hour Exam III Solutions: April 26, 2006

1. (b)

6 6 6 6

2 2 or 2 2

−1 −1

� � � � � � 1 2 � k∞

(b) δ(t) + δ t − + δ t − = δ t −12 12

+ · · · 12k=0

2. (a) The period of cos(nπt) is 2π/nπ = 2/n, and the least common multiple of these, for n ≥ 2, is 2. This is the minimal period.

cos(2πt) cos(3πt) cos(4πt) � cos(kπt)∞(b) xp = = (−1)k

2k−1(ω2 n − (2π)2)

− 4(ω2 8(ω22(ω2

n − (3π)2)+

n − (4π)2) − · · ·

n − (kπ)2)k=2

(c) There is resonance when ωn = kπ for k = 2, 3, 4, . . ..

(d) f(t) and cos(πt) are both even, so f(t) cos(πt) is even. Thus � 1 1 � 1 f(t) cos(πt) dt = f(t) cos(πt) dt, and this is zero either because it computes the

0 2 −1 Fourier coefficient of cos(πt) in f(t), which is zero, or by the orthogonality properties of the cosine functions, as written in the information page attached to the exam.

3. (a) The denominator s2 + 4s + 104 = (s + 2)2 + 100 [the value announced as a correction in the exam room] vanishes at s = −2 ±10i, so this is where the poles of W (s) are.

(b) The poles are relatively near to the imaginary axis, so |W (iω) probably has near­|resonant peaks near ω = ±10. [The gain is an even function of ω, so sketching it for ω > 0 suffices.] The slope becomes zero when ω = 0 (because the function is even), and the graph falls off to zero as ω → ∞.

for t < a (c) x = u(t − a)e I(t−a) =

0 eI(t−a) for t > a

2 4. (a) (s 2X − (−1)s − 2) + 4(sX − (−1)) + 5X = or X =

(−s − 2) + (2/(s2 + 4)) s2 + 4 s2 + 4s + 5

(b) s

=(s + 2) − 2 (s + 2)2 + 1

is the Laplace transform of e−2t(cos t − 2 sin t) s2 + 4s + 5

t t 5. (a) x = w(t) ∗ f(t) = w(t − τ)f(τ) dτ = (t − τ)e−(t−τ )f(τ) dτ . This can also be � 0 0

t written τe−τ f(t − τ) dτ .

0

d 1 1 (b) W (s) = L−1[te−t] = =

(s + 1)2 , so W (1) = 1/4 and −

ds s + 1 txp = W (1)et = (1/4)e .