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In Problems 13-20use (20)to find the general solution of the given differential equation on0,.

xy''+3y'+x3y=0

Short Answer

Expert verified

The general solutions of the given differential equation are

y=x-1C1J1/212x2+C2J-1/212x2andy=x-1C1J1/212x2+C2Y1/212x2

Step by step solution

01

Define Bessel’s equation.

Let the Bessel equation be x2y''+xy'+(x2-n2)y=0. This equation has two linearly independent solutions for a fixed value of n. A Bessel equation of the first kind, indicated by Jn(x), is one of these solutions that may be derived usingFrobinous approach.

y1=xaJp(bxc)y2=xaJ-p(bxc)

At , x = 0 this solution is regular. The second solution, which is singular at x = 0, is represented by Yn(x) and is called a Bessel function of the second kind.

y3=xacospπJpbxc-J-pbxcsinpπ

02

Determine the general form of the Bessel’s equation.

Let the given differential equation bexy''+3y'+x3y=0, that has a singular point at x = 0.

The equation becomes in the following form:

y''+1-2axy'+b2c2x2c-2+a2-p2c2x2y=0.......1

That yields,

xxy''+3xxy'+x3xy=0y''+3xy'+x2+0x2y=0........2

03

Find the value of constants.

Compare the equations (1) and (2).

Solve for a:

1-2a=3a=-1

Solve for:

2c-2=2c=2

Solve for:

b2c2=1b=12

Solve for:

a2-p2c2=0p1=12,p2=-12

04

Obtain the general solution.

There are two series which are linearly independent.

y1=x-1J1/212x2y2=x-1J-1/212x2

The general solution by using superposition principle is,

y=C1x-1J1/212x2+C2x-1J-1/212x2=x-1C1J1/212x2+C2J-1/212x2

There is another general solution obtained from the Bessel’s equation of second order. (i.e.) y=x-1C1J1/212x2+C2Y1/212x2.

Hence, the general solutions are y=x-1C1J1/212x2+C2J-1/212x2andy=x-1C1J1/212x2+C2Y1/212x2and .

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Most popular questions from this chapter

Cooling Fin A cooling fin is an outward projection from a mechanical or electronic device from which heat can be radiated away from the device into the surrounding medium (such as air). See Figure 6.R.1. An annular, or ring-shaped, cooling fin is normally used on cylindrical surfaces such as a circular heating pipe. See Figure 6.R.2. In the latter case, let r denote the radial distance measured from the center line of the pipe and T(r) the temperature within the fin defined for r0rr1 It can be shown that T(r) satisfies the differential equation

role="math" localid="1663927167728" ddrrdTdr=a2r(T-Tm)

where a2is a constant and Tmis the constant air temperature.

Suppose r-0=1,r-1=3, ,and Tm=70. Use the substitution w(r) =T(r)_70to show that the solution of the given differential equation subject to the boundary conditions

T(1)=160, T(3)=0 is

role="math" localid="1663926265607" T(r)=70+90K1(3a)Iv(ar)+I1(3a)Kv(ar)K1(3a)I0(a)+I!(3a)K0(a)where and I0(x) and K0(x)are the modified Bessel functions of the first and second kind. You will also have to use the derivatives given in (25) of Section 6.4.

In Problems 25-30 proceed as in Example 3 to rewrite the given expression using a single power series whose general term involves xk.

n=12nCnxn-1+n=06Cnxn+1

In Problems 25-30 proceed as in Example 3 to rewrite the given expression using a single power series whose general term involves xk.

n=2n(n-1)Cnxn+2n=2n(n-1)Cnxn-2+3n=1nCnxn

Bessel’s Equation

In Problems 1-6 use (1) to find the general solution of the given differential equation on(0,).

2.

localid="1664866362361" x2y''+xy'+(x2-1)y=0

How can the power series method be used to solve the non-homogeneous equationY"-xy=1about the ordinary point? Ofy''-4xy'-4y=ex? Carry out your ideas by solving both DEs.

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