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Differentiation Equations course is one of basic course of science study. Its part of Mathematics, Computer Science, Physics, Engineering. This is assignment solution to help students for exercising problem. It includes: Problem, Set, Exponential, Growth, Decay, Circular, Frequency, Constant, Amplitude, Oscillate, Homogeneous, Curve, Imaginary, Axis, Asymptotic
Typology: Exercises
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Part I points: 29. 4, 30. 0, 32. 8, 33. 4.
Part II solutions:
et^. (This means that for any a < 1 < c, eat^ < |f (t)| < ect^ for large t.) They also
show a small oscillation of approximately constant amplitude and circular frequency 1. a b Examples: f (t) = aet^ + b sin(t) (a, b =≥ 0) with F (s) = +. s − 1 s^2 + 1
(2) {−1 + 4i, − 1 − 4 i}: For large t, these functions show exponential decay like e −t ,
and oscillate with circular frequency 4. Examples: f (t) = ae−t^ sin(4t) (a =≥ 0) with
4 a F (s) =. (s + 1)^2 + 16
(3) {− 1 }: For large t, these functions decay like e−t^ and do not oscillate. Examples: a f (t) = ae −t (a =≥ 0) with F (s) = s + 1
(4) No poles: For large t, these functions decay to zero faster than any exponential.
Examples: f (t) = aω(t − b) (a = 0≥ −
, b bs
� 0) with F (s) = ae−bt, or f (t) = a(u(t) − u(t − b))
(a = 0≥ , b > 0) with F (s) = a
s
e .
(b) (i) [4] Method I: For t > 0, w(t) is a solution to the homogeneous equation. The roots
must be − (^2) 1 ± (^2) 3 i, so p(s) = m
s − (− (^2) 1
s − (− (^2) 1 − (^2) 3 i)
= m(s 2 +s+ (^2) 5 ). To find m,
remember that w˙ (0+) = 1 (for a second order system). w˙ (t) = u(t)e−t/^2 ( 3 m 2 cos(3t/2)^ − (− 1 2 sin(3t/2)),^ so^ w˙ (0+)^ =^
3 2 ,^ m^ =^
2 3 ,^ and^ p(s) =^3
2 (s 2
(2/3)(s^2 + s + (5/2))
so p(s) = 2 3 (s
2
(ii) [4] {− 12 ± 32 i}.
3 / 2 (iii) [4] This is a throwback problem. The complex gain is W (i�) = , so ((5/2) − �^2 ) + i� 3 / 2 the gain is |W (i�) =| �^. This is maximized when the denominator, ((5/2) − �^2 )^2 + �^2
or its square ( 5 2 −^ �
(^2) ) (^2) + � (^2) , is minimized. The derivative with respect to � is
2( 5 2 −^ �
(^2) )(− 2 �) + 2�, which has roots at � = 0 and � = ±
2 is the worst
frequency.
(iv) [6] The yellow box lies in the plane above the imaginary axis. The base is the
amplitude response curve. The green box lies in the plane above the real axis. Its top
lies on the graph of |W (s) ,| and its base is the real axis. The red arrows lie above the
poles of W (s). The yellow diamonds are located at (±i�, |W (i�)|), and represent the
chosen value of the input circular frequency and the corresponding gain.
are given by x 1 = e−t^ and x 2 = e−^3 t^. (The order is not determined, and in fact any other
pair of linearly independent solutions count as “basic.”) x˙ 1 = −e−t^ , x˙ 2 = − 3 e−^3 t^.
p(s) = s^2 + s + 5 = (s + 1 )^2 + 9 has roots r = − 1 3 2 2 4 2 ±^2 i.^ Basic^ solutions^ are^ given^ by^ x^1 = e−t/^2 cos( 3 −t/^2 (−^1 2 t)^ and^ x^2 =^ e
−t/ (^2) sin( 3 2 t).^ (Same^ caveats^ as^ above.)^ x˙^1 =^ e^2 cos(^
3 2 t)^ − 3 sin( 3 t)). x˙ 2 = e −t/ 2 (− 1 sin( 3 t) + 3 cos( 3 2 2 2 2 2 2 t)).
0 1 0 1 (b) [4] , 5. − 3 − 4 − 2
The ray containing corresponds to − �
(c) [4] (^1) x 1 ; the ray containing corresponds − 3 to x 2.
1 x (d) [4] The solution passing through at t = 0 is where x is the solution to 0 x˙
x¨ + 4 ˙x + 3x = 0 with x(0) = 1, x˙ (0) = 0. The general solution x(t) = c 1 e −t
has x(0) = c 1 + c 2 and x˙ (0) = −c 1 − 3 c 2 , so c 1 + c 2 = 1 and −c 1 − 3 c 2 = 0. Thus
c 2 = − 2
(^1) and c 1 =^2
(^3) and x(t) = 1 2 (3e−t^ − e−^3 t), so u(t) = x
x ˙
t t
2
1 −
e e
− −
t t
e− e
3 −
t 3 t.
Description of the graph of x(t): For t << 0 it is very negative and increasing. x(t) = 0
for t = − ln 2 3. It reaches a maximum x(0) = 1, and then falls back through an inflection
point to become asymptotic to x = 0 as t � �.
3 e−(t−a)^ −3(t−a) (e) [4] u(t) = 1 (^2) − 3 e−(t−a)
e e−3(t−a)^
(f) [8]
The trajectory of interest is the spiral pass ing through (0, 1).
x(t) 0 The solution u(t) = passing through at t = 0 is given by the solution x(t) x˙ (t) 1
of x¨ + x˙ + 52 x = 0 with x(0) = 0, x˙(0) = 1. The general solution x(t) = e−t/^2 (c 1 cos( 32 t) +
c 2 sin( 3 2 t))^ has^ x(0)^ =^ c^1 and^ x˙ (0)^ =^
1 2 c^1 +^
3 2 c^2 ,^ so^ c^1 =^0 and� c^2 =^
2 − 3. Thus x(t) (^) �= 2 2 1 −t/ 2 3 sin(
3 2 t) 3 e−t/^2 sin( 2
(^3) t), x˙(t) = e−t/ (^2) (cos( 2
(^3) t) − 3 sin( 2
(^3) t)), and u(t) = e cos( 3 t) − 1 sin( 3 t)
2 3 2 This passes through the y axis when x(t) = 0, i.e. when sin( 3 2 t)^ =^ 0,^ which^ is^ when^ t^ is an integral multiple of 2 �/3.