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This is solved assignment of Differential Equations course. It can be helpful to engineering, computer science, physics and maths students. It was submitted to Prof. Dhanesh Bhatnagar at B R Ambedkar National Institute of Technology. It includes: Gamma, Function, Integral, Converges, Laplace, Transform, Full, Rectifier, Wave
Typology: Exercises
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(modified on April 8, 2009)
Due by Friday, April 10, 2009, by NOON
1. (Laplace transform of tr). The Gamma function is defined by the integral
∞ Γ(r + 1) = e−ttrdt. 0
(a) Show that the improper integral converges for all r > − 1.
(b) Show that Γ(r + 1) = rΓ(r) for r > 0. Show that Γ(1) = 1 , Γ(1/2) =
π.
(c) For r > − 1 show that L[tr] = Γ(r + 1)/sr+1^ , s > 0
2. (a) Find the solution of the initial value problem
y��^ + ω^2 y = h(t) sin t − h(t − c) sin t, y(0) = y�(0) = 0 ,
where c > 0 is a constant and ω^2 = 1.
(b) Show that y(0) = y�(0) = y��(0) = 0. Show that y and y�^ are continuous at t = c.
(c) Show that y��(c+) − y��(c−) = − sin c, which is 0 if and only if c = nπ for n an integer. This behavior is explained by that the function h(t − c) sin t is continuous at c if and only if sin c = 0.
3. Find the Laplace transform of a full rectified wave∗^ f (t) = | sin t|. 4. Find the solution of the initial value problem
y��^ + y = Aδ(t − c), y(0) = a, y�(0) = b,
where A, a, b, c are constant and c > 0.
(b) Show that y(t) = 0 for t ≥ c if and only if y(c) = 0 and
A = a^2 + b^2 , a sin c ≥ b cos c; A = − a^2 + b^2 , a sin c ≤ b cos c.
To interpret, these amplitudes A and locations of impulse c cancel the oscillation.
5. (The Volterra integral equation). Consider the integral equation
t (^1) y(t) + (t − s)y(s)ds = − 4
sin 2 t. 0
(a) Show that the above integral equation is equivalent to the initial value problem
1 y��^ + y = sin 2 t, y(0) = 0 , y�(0) = − 2
(b) Solve the integral equation by using the Laplace transform.
∗It describes a direct current. 1
6. Consider the Bessel equation of order zero
ty��^ + y�^ + ty = 0.
Note that t = 0 is a singular point and thus solutions may become unbounded as t → 0. Never theless, let us try to determine whether there are any solutions that remain finite at t = 0 and have finite derivatives there.
(a) Show that Y (s) = Ly satisfies (1 + s^2 )Y �(s) + sY (s) = 0.
(b) Using the binomial series for (1 + s^2 )−^1 /^2 for s > 1 show that
� (^) t^2 n y(t) = c
∞ ( 2
2 n
(n
n !)^2
n=
which is referred to as the Bessel function of the first kind of order zero. Show that y(0) = 1 and y has finite derivatives for all orders at t = 0.
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