Solved Problems for Assignment 8 - Elementary Differential Equations | Math 3, Assignments of Mathematics

Material Type: Assignment; Class: ELEM DIFF EQUATIONS; Subject: Mathematics; University: University of California - Irvine; Term: Winter 2006;

Typology: Assignments

Pre 2010

Uploaded on 09/17/2009

koofers-user-h4k
koofers-user-h4k 🇺🇸

5

(1)

10 documents

1 / 2

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
MATH 3D Homework 8 Name: Solutions
Feb. 28, 2006
Section 2.4 Problems
9. Find two linearly independent solutions of t2y00 2y= 0 of the form y(t) = tr.
Using these solutions, find the general solution of t2y00 2y=t2.
Solution (12 points): The ODE is an Euler’s equation, so we seek solutions
of the form y=tr. Plugging this into the differential equation, we have
t2r(r1)tr22tr=tr(r2r2) = tr(r+ 1)(r2) = 0.
Thus, two solutions are y1=t1and y2=t2. We seek a a particular solution ψ
of the form
ψ=u1(t)y1(t) + u2(t)y2(t).
However, we note that the differential equation is not in the correct form y00 +
p(t)y0+q(t)y=g(t), so we first fix this:
y00 2
t2y= 1.
We compute that
W[y1, y2] = det µy1y2
y0
1y0
2= det µt1t2
t22t= 3.
Now, recall that
u0
1=gy2
W=t2
3=u1=1
9t3
u0
2=gy1
W=t1
3=u2=1
3ln t.
So, the general solution is given by
y(t) = c1y1+c2y2+ψ
=c1t1+c2t21
9t3t1+1
3ln tt2
=c1t1+µc21
9t2+1
3t2ln t.
Notice that we could redefine ec2=c21
9.
Section 2.5 Problems
4. Find a particular solution of y00 +y0+y= 1 + t+t2.
Solution (13 points): The ODE is a constant coefficient problem, and the
righthand side is a polynomial. So, we judiciously guess that ψis a polynomial
pof some degree m. Let us determine the required degree.
Document URL: http://math.uci.edu/~pmacklin/Math3Dwinter2006.html
Date: February 28, 2006 Page 1 of 2
pf2

Partial preview of the text

Download Solved Problems for Assignment 8 - Elementary Differential Equations | Math 3 and more Assignments Mathematics in PDF only on Docsity!

MATH 3D Homework 8 Name: Solutions

Feb. 28, 2006

Section 2.4 Problems

  1. Find two linearly independent solutions of t^2 y′′^ − 2 y = 0 of the form y(t) = tr. Using these solutions, find the general solution of t^2 y′′^ − 2 y = t^2.

Solution (12 points): The ODE is an Euler’s equation, so we seek solutions of the form y = tr. Plugging this into the differential equation, we have

t^2 r(r − 1)tr−^2 − 2 tr^ = tr(r^2 − r − 2) = tr(r + 1)(r − 2) = 0.

Thus, two solutions are y 1 = t−^1 and y 2 = t^2. We seek a a particular solution ψ of the form ψ = u 1 (t)y 1 (t) + u 2 (t)y 2 (t). However, we note that the differential equation is not in the correct form y′′^ + p(t)y′^ + q(t)y = g(t), so we first fix this:

y′′^ −

t^2

y = 1.

We compute that

W [y 1 , y 2 ] = det

y 1 y 2 y′ 1 y 2 ′

= det

t−^1 t^2 −t−^2 2 t

Now, recall that

u′ 1 = −

gy 2 W

t^2 3

=⇒ u 1 = −

t^3

u′ 2 =

gy 1 W

t−^1 3

=⇒ u 2 =

ln t.

So, the general solution is given by

y(t) = c 1 y 1 + c 2 y 2 + ψ

= c 1 t−^1 + c 2 t^2 −

t^3 t−^1 +

ln tt^2

= c 1 t−^1 +

c 2 −

t^2 +

t^2 ln t.

Notice that we could redefine c˜ 2 = c 2 − 19.

Section 2.5 Problems

  1. Find a particular solution of y′′^ + y′^ + y = 1 + t + t^2.

Solution (13 points): The ODE is a constant coefficient problem, and the righthand side is a polynomial. So, we judiciously guess that ψ is a polynomial p of some degree m. Let us determine the required degree.

Document URL: http://math.uci.edu/~pmacklin/Math3Dwinter2006.html Date: February 28, 2006 Page 1 of 2

p′′^ is a polynomial of degree m − 2, p′^ is a polynomial of degree m − 1, and p is a polynomial of degree m. Therefore,

p′′^ + p′^ + p

is a polynomial of degree m. The righthand side is a polynomial of degree 2. So, as the left and right sides must be equal, m = 2, and so

p(t) = at^2 + bt + c.

Let’s plug this into the differential equation:

p′′^2 a +p′^ +2at + b +p +at^2 + bt + c t^2 + t = 1 = at^2 + (2a + b)t + (2a + b + c)

Two polynomials are only equal if the corresponding coefficients are equal. Therefore, we have three equations in three unknowns:

1 = a 1 = 2 a + b 1 = 2 a + b + c.

By the first equation, a = 1, by the second, b = 1 − 2 a = −1, and by the third, c = 1 − 2 a − b = 1 − 2 + 1 = 0. Therefore,

ψ(t) = p(t) = t^2 − t.

Completeness Points

(0 points) None this week.

Document URL: http://math.uci.edu/~pmacklin/Math3Dwinter2006.html Date: February 28, 2006 Page 2 of 2