Quiz 6 Solution: Differential Equations and Power Functions, Exercises of Calculus

The answer key for quiz 6, section b, which deals with solving a differential equation using power functions. How to find the solutions by identifying the possible values of the constants c and n that make the right side of the equation identically zero. Two methods are presented to find the general solution of the differential equation, and the document provides the steps to find the particular solution using each method. The document also discusses the implications of the solution and its relationship to the original differential equation.

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Answer Key for Quiz 6 (section B)
1. If y=Cxnfor some constants Cand nthen
dy
dx =C¡nxn1¢and d2y
dx2=Cn(n1)xn2
Plugging y,dy
dx and d2y
dx2into the differential equation
x2d2y
dx2+ 4xdy
dx + 2y= 0
we get
0 = x2¡Cn(n1)xn2¢+ 4x¡C nxn1¢+ 2Cxn
=Cn(n1)xn+ 4C nxn+ 2Cxn
=Cxn[n(n1) + 4n+ 2]
=Cxn¡n2n+ 4n+ 2¢
=Cxn¡n2+ 3n+ 2¢
=Cxn(n+ 2)(n+ 1).
Since xnonly equals zero at x= 0, there are only three ways to make the right side identically zero: we can
take C= 0, or n=1, or n=2. This shows that any function of the form y=C
xor y=C
x2is a solution
of the differential equation, but no other power function could be. In fact every solution of the differential
equation has the form
y=A
x+B
x2
for some constants Aand B.
2. Method 1: multiply the differential equation by e3tto get
e3tdx
dt + 3e3tx= 24e3t.
This makes the left side into the derivative of xe3t:
d
dt xe3t= 24e3t.
Therefore, if we integrate both sides with respect to twe get
Z24e3tdt =Zµd
dt xe3tdt =xe3t.
We can use the substitution u= 3tto do the integral on the left: du = 3 dt, so we have
xe3t=Z24e3tdt = 8 Ze3t3dt = 8 Zeudu = 8eu+C= 8e3t+C.
We can solve this for xby multiplying through by e3t:
x= 8 + C e3t.
Now plug in x= 12 and t= 0 to get
12 = 8 + C e0= 8 + C, so C= 4 and we finally have x= 8 + 4e3t.
pf2

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Answer Key for Quiz 6 (section B)

  1. If y = Cxn^ for some constants C and n then

dy dx

= C

nxn−^1

and

d^2 y dx^2

= Cn(n − 1)xn−^2

Plugging y, dydx and d

(^2) y dx^2 into the differential equation

x^2 d^2 y dx^2

  • 4x dy dx

  • 2y = 0

we get

0 = x^2

Cn(n − 1)xn−^2

  • 4x

Cnxn−^1

  • 2Cxn = Cn(n − 1)xn^ + 4Cnxn^ + 2Cxn = Cxn^ [n(n − 1) + 4n + 2] = Cxn^

n^2 − n + 4n + 2

= Cxn^

n^2 + 3n + 2

= Cxn(n + 2)(n + 1).

Since xn^ only equals zero at x = 0, there are only three ways to make the right side identically zero: we can take C = 0, or n = −1, or n = −2. This shows that any function of the form y = Cx or y = (^) xC 2 is a solution of the differential equation, but no other power function could be. In fact every solution of the differential equation has the form

y =

A

x

B

x^2

for some constants A and B.

  1. Method 1: multiply the differential equation by e^3 t^ to get

e^3 t^ dx dt

  • 3e^3 t^ x = 24e^3 t.

This makes the left side into the derivative of xe^3 t:

d dt

xe^3 t^ = 24e^3 t.

Therefore, if we integrate both sides with respect to t we get

∫ 24 e^3 t^ dt =

d dt xe^3 t

dt = xe^3 t.

We can use the substitution u = 3t to do the integral on the left: du = 3 dt, so we have

xe^3 t^ =

24 e^3 t^ dt = 8

e^3 t^3 dt = 8

eu^ du = 8eu^ + C = 8e^3 t^ + C.

We can solve this for x by multiplying through by e−^3 t:

x = 8 + Ce−^3 t.

Now plug in x = 12 and t = 0 to get

12 = 8 + Ce^0 = 8 + C, so C = 4 and we finally have x = 8 + 4e−^3 t.

Method 2: rearrange the differential equation to

dx dt

= 24 − 3 x and then to dt =

dx 24 − 3 x

To make the right side slightly nicer, multiply through by −3 to get

− 3 dt =

− 3 dx (−3)(x − 8)

dx x − 8

Then integrate both sides:

∫ − 3 dt =

dx x − 8 =⇒ − 3 t + C = ln |x − 8 |.

We have several options now.

Method 2a: plug in x = 12 and t = 0 to get

0 + C = ln | 12 − 8 | = ln 4, so C = ln 4.

This also tells us that we can remove the absolute values on x − 8; since it is positive at t = 0 it must stay positive, otherwise ln |x − 8 | would become infinite before x − 8 could become negative. So now we know

ln(x − 8) = − 3 t + ln 4,

and we can solve for x by exponentiating both sides:

eln(x−8)^ = e−^3 t+ln 4^ = e−^3 t^ eln 4^ which simplifies to x − 8 = 4e−^3 t.

So we get x = 8 + 4e−^3 t^ as before.

Method 2b: do the exponentiation step before plugging in. This gives

eln^ |x−^8 |^ = e−^3 t+C^ = e−^3 t^ eC^ which simplifies to |x − 8 | = Ke−^3 t,

where K = eC^ is a positive arbitrary constant. Plugging in x = 12 and t = 0 we now get

| 12 − 8 | = Ke^0 = K, so K = 4 and therefore |x − 8 | = 4e−^3 t.

This implies that either x − 8 = 4e−^3 t^ or x − 8 = − 4 e−^3 t.

But only the former can be right because in the latter x doesn’t equal 12 when t = 0. So once again we get x = 8 + 4e−^3 t.

Method 2c: as in method 2b, but at the stage where we rename eC^ as K, allow K to be a completely arbitrary constant and use that freedom to remove the absolute values. This gives x − 8 = Ke−^3 t, and when we plug in x = 12 and t = 0 we get K = 4 as before.