For the following problems, verify the given solution and then, by method (e) above, find a second solution of the given equation

x2y''+(x+1)y'-y=0

Short Answer

Expert verified

The proof that of the solution of the differential is stated above and the second solution isy=xe1/x.

Step by step solution

01

Given information

The given differential equation is x2y''+(x+1)y'-y=0and the solution is u=x+1.

02

differential equation

A differential equation is an equation that relates one or more unknown functions and their derivatives.

03

solution of the equation

Consider the differential equation.

x2y''+(x+1)y'-y=0

The solution of the equation is,

role="math" localid="1664340789299" u=x+1

So,

y=A(x+1)y'=Ay''=0

04

consider left side of given equation

Consider the left-hand side of the given differential equation.

x2y''+(x+1)y'-y=x2(0)+(x+1)(A)-A(x+1)=0+A(x+1)-A(x+1)=0

So, u=x+1is the solution of the given differential equation.

Let,

y=uv=(x+1)vSo,

y'=(x+1)v'+vy''=v'+v'+(x+1)v''=(x+1)v''+2v'

05

equation can be written as

The differential equation can now be written as,x2(x+1)v''+2v'+(x+1)v+(x+1)v'-(x+1)v=0v'3x2+1+2x+v''x3+x2=0v''v'=-3x2+1+2xx3+x2dv'v'=-3x2+1+2xx3+x2

Write the expression in partial fraction form.

dv'v'=-3(x+1)-1x2-1x(x+1)=-3x+1-1x2-1x+1x+1

Integrate the above equation.

lnv'=-3ln(x+1)+x-1-lnx+ln(x+1)+lnKlnv'=lnK(x+1)2x-1+1xv'=Ke1/xx(x+1)2dvdx=Ke1/xx(x+1)2

06

solve further

Integrate both side of the equation.

v=-Kxe1/xx+1+C

ConsiderC=0.

v=-Kxe1/xx+1

Thus,

y=uv=-Kxe1/xx+1(x+1)=-Kxe1/x

So, the second solution of the above equation is,

y=xe1/x.

Therefore, the proof that of the solution of the differential is stated above and the second solution isy=xe1/x.

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Most popular questions from this chapter

In Problems 2 and 3, use (12.6) to solve (12.1) when f(t)is as givef(t)=e-t

In Problem 33 to 38, solve the given differential equations by using the principle of superposition [see the solution of equation (6.29)]. For example, in Problem 33, solve three differential equations with right-hand sides equal to the three different brackets. Note that terms with the same exponential factor are kept together; thus, a polynomial of any degree is kept together in one bracket.

(D2-1)y=sinhx

(a)Consider a light beam travelling downward into the ocean. As the beam progresses, it is partially absorbed and its intensity decreases. The rate at which the intensity is decreasing with depth at any point is proportional to the intensity at that depth. The proportionality constant μis called the linear absorption coefficient. Show that if the intensity at the surface is I0, the intensity at a distance s below the surface is I=I0eμs. The linear absorption coefficient for water is of the order of 10.2ft.1(the exact value depending on the wavelength of the light and the impurities in the water). For this value of μ, find the intensity as a fraction of the surface intensity at a depth of 1 ft, ft,ft,mile. When the intensity of a light beam has been reduced to half its surface intensity (I=12I0), the distance the light has penetrated into the absorbing substance is called the half-value thickness of the substance. Find the half-value thickness in terms of μ. Find the half-value thickness for water for the value of μgiven above.

(b) Note that the differential equation and its solution in this problem are mathematically the same as those in Example 1, although the physical problem and the terminology are different. In discussing radioactive decay, we call λthe decay constant, and we define the half-life T of a radioactive substance as the time when N=12N0(compare half-value thickness). Find the relation between λand T.

In problems 13 to 15, find a solution(or solutions) of the differential equation not obtainable by specializing the constant in your solution of the original problem. Hint: See Example 3.

14. Problem 8.

Verify the statement of Example 2. Also verify that y=coshxandy=sinhx are solutions of y''=y.

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