The Gamma Function-Differential Equations-Assignemnt and Solution, Exercises of Differential Equations

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

2011/2012

Uploaded on 07/31/2012

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18.034 Problem Set #6
(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) = ettrdt.
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�� + ω2
y = h(t) sin t h(t c)sin t, y(0) = y(0) = 0,
where c > 0 is a constant and ω2 = 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 = 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 = (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 = a2 + b2
, a sin c b cos c; A = a2 + b2
, 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 2t.
0
(a) Show that the above integral equation is equivalent to the initial value problem
1
y�� + y = sin 2t, y(0) = 0, y(0) = 2.
(b) Solve the integral equation by using the Laplace transform.
It describes a direct current.
1
.
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18.034 Problem Set

(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

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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.

2

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