Initial Value - Math - Assignment Solutions, Exercises of Mathematics

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Math 334
Assignment 5 Solutions
1. Find the solution to the following initial value problems.
(a) y′′′ y′′ 4y+ 4y= 0; y(0) = 4, y(0) = 1, y′′(0) = 19.
(b) y′′′ 4y′′ + 7y6y= 0; y(0) = 1, y(0) = 0, y′′(0) = 0.
Solution
(a) The characteristic p olynomial for this d.e. is:
C(r) = r3r24r+ 4 = (r+ 2)(r1)(r2),
whose roots are r=2,1,2. The general solution to the equation is:
y(x) = c1e2x+c2ex+c3e2x.
Apply the initial conditions:
y(0) = 4
y(0) = 1
y′′(0) = 19
=
c1+c2+c3=4
2c1+c2+ 2c3=1
4c1+c2+ 4c3=19
=
c1=2
c2= 1
c3=3
Therefore the solution to the initial value problem is
y(x) = 2e2x+ex3e2x.
(b) The characteristic polynomial for this d.e. is:
C(r) = r34r2+ 7r6 = (r2)(r22r+ 3),
whose roots are r= 2,1±2i. The general solution to the equation is:
y(x) = c1e2x+ex(c2cos 2x+c3sin 2x).
Apply the initial conditions:
y(0) = 1
y(0) = 0
y′′(0) = 0
=
c1+c2= 1
2c1+c2+ 21/2c3= 0
4c1c2+ 23/2c3= 0
=
c1= 1
c2= 0
c3=2
Therefore the solution to the initial value problem is
y(x) = e2x2exsin 2x).
2. Find the general solution to the following system of two second order differential equations:
d2x
dt2x+y= 0, x +d2y
dt2y=e3t.
1
pf3
pf4

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Math 334

Assignment 5 — Solutions

  1. Find the solution to the following initial value problems.

(a) y

′′′ − y

′′ − 4 y

  • 4y = 0; y(0) = − 4 , y

′ (0) = − 1 , y

′′ (0) = −19.

(b) y ′′′ − 4 y ′′

  • 7y ′ − 6 y = 0; y(0) = 1, y ′ (0) = 0, y ′′ (0) = 0.

Solution

(a) The characteristic polynomial for this d.e. is:

C(r) = r

3 − r

2 − 4 r + 4 = (r + 2)(r − 1)(r − 2),

whose roots are r = − 2 , 1 , 2. The general solution to the equation is:

y(x) = c 1 e

− 2 x

  • c 2 e

x

  • c 3 e

2 x .

Apply the initial conditions:

y(0) = − 4

y ′ (0) = − 1

y ′′ (0) = − 19

c 1 + c 2 + c 3 = − 4

− 2 c 1 + c 2 + 2c 3 = − 1

4 c 1 + c 2 + 4c 3 = − 19

c 1 = − 2

c 2 = 1

c 3 = − 3

Therefore the solution to the initial value problem is

y(x) = − 2 e

− 2 x

  • e

x − 3 e

2 x .

(b) The characteristic polynomial for this d.e. is:

C(r) = r

3 − 4 r

2

  • 7r − 6 = (r − 2)(r

2 − 2 r + 3),

whose roots are r = 2, 1 ±

2 i. The general solution to the equation is:

y(x) = c 1 e

2 x

  • e

x (c 2 cos

2 x + c 3 sin

2 x).

Apply the initial conditions:

y(0) = 1

y ′ (0) = 0

y

′′ (0) = 0

c 1 + c 2 = 1

2 c 1 + c 2 + 2 1 / 2 c 3 = 0

4 c 1 − c 2 + 2

3 / 2 c 3 = 0

c 1 = 1

c 2 = 0

c 3 = −

Therefore the solution to the initial value problem is

y(x) = e 2 x −

2 e x sin

2 x).

  1. Find the general solution to the following system of two second order differential equations:

d

2 x

dt^2

− x + y = 0, x +

d

2 y

dt^2

− y = e

3 t .

Solution

Differentiate (1) twice with repect to t to get

x

(iv) − x

′′

  • y

′′ = 0.

Use (2) to eliminate y ′′ to get

x

(iv) − x

′′ − x + y = −e

3 t .

Now use (1) to eliminate y from this equation to get

x

(iv) − 2 x

′′ = −e

3 t .

We now have a 4

th order o.d.e. in x only. The characteristic polynomial for the homogeneous equation

is C(r) = r

4 − 2 r

2

. The roots are: r = 0, ±

2, with 0 being a double root. Four linearly independent

solutions to the homogeneous equation are: { 1 , t, e

√ 2 t , e −

√ 2 t }. Since the forcing term e 3 t is not a

solution to the homogeneous equation, we look for a particular solution of the form φp(t) = Ae 3 t .

Plugging φp into the equation leads to A = − 1 /C(3) = − 1 /63. Therefore x(t) is:

x(t) = c 1 + c 2 t + c 3 e

√ 2 t

  • c 4 e

√ 2 t −

e

3 t .

We can now use (1) to solve for y as follows:

y(t) = x(t) − x

′′ (t) = c 1 + c 2 t − c 3 e

√ 2 t − c 4 e

√ 2 t −

e

3 t .

The general solution to the system of equations is

x(t) = c 1 + c 2 t + c 3 e

√ 2 t

  • c 4 e

√ 2 t −

e

3 t ,

y(t) = c 1 + c 2 t − c 3 e

√ 2 t − c 4 e

√ 2 t −

e

3 t .

  1. Consider the fourth order differential equation:

y

(iv) (x) − k

2 y

′′ (x) = g(x). (1)

(a) Find the general solution to the homogeneous equation.

(b) Show that a particular solution to Eq. (1) can be written in the form

φp(x) =

k 2

xg(x) dx −

x

k 2

g(x) dx +

e kx

2 k 3

g(x)e

−kx dx −

e −kx

2 k 3

g(x)e

kx dx.

(c) Show that the general solution in part (b) can be rewritten in the form

φp(x) =

∫ (^) x

0

g(s)G(x − s) ds,

where

G(ξ) =

k 3

(sinh kξ − kξ).

(d) Determine the simplest form of the general solution to Eq. (1) in the case g(x) ≡ 1.

Thus, a particular solution is given by

φp(x) =

k 2

xg(x) dx −

x

k 2

g(x) dx +

e kx

2 k 3

g(x)e −kx dx −

e −kx

2 k 3

g(x)e kx dx.

(c) We rewrite the particular solution above as follows:

φp(x) =

k 2

∫ (^) x

0

sg(s) ds −

x

k 2

∫ (^) x

0

g(s) ds +

e

kx

2 k 3

∫ (^) x

0

g(s)e

−ks ds −

e

−kx

2 k 3

∫ (^) x

0

g(s)e

ks ds

∫ (^) x

0

g(s)

s

k^2

x

k^2

e

kx e

−ks

2 k^3

e

−kx e

ks

2 k^3

ds

x

0

g(s)

x − s

k^2

e

k(x−s) − e

−k(x−s)

2 k^3

ds

∫ (^) x

0

g(s)G(x − s) ds,

where

G(ξ) =

e

kξ − e

−kξ

2 k 3

ξ

k 2

k 3

(sinh kξ − kξ).

(d) If g(x) ≡ 1, the particular solution becomes

φp(x) =

∫ (^) x

0

G(x − s) ds =

∫ (^) x

0

G(ξ) dξ =

k 3

∫ (^) x

0

(sinh kξ − kξ) dξ

k 3

cosh kξ

k

2

x

0

k 4 (cosh kx − 1) −

x

2

2 k 2

The general solution is

y(x) = φh(x) + φp(x) = c 1 + c 2 x + c 3 e

kx

  • c 4 e

−kx

k 4

(cosh kx − 1) −

x 2

2 k 2

This can be simplified:

y(x) = c 1 + c 2 x + c 3 e

kx

  • c 4 e

−kx

k 4

e kx − e −kx

x 2

2 k 2

c 1 −

k 4

  • c 2 x +

c 3 +

2 k 4

e

kx

c 4 −

2 k 4

e

−kx −

x 2

2 k 2

= b 1 + b 2 x + b 3 e

kx

  • b 4 e

−kx −

x

2

2 k^2

Thus, the simplest form for the general solution is

y(x) = b 1 + b 2 x + b 3 e kx

  • b 4 e −kx −

x

2

2 k 2