Variation of Parameters. Here is another procedure for solving linear equations that is particularly useful for higher-order linear equations. This method is called variation of parameters. It is based on the idea that just by knowing the form of the solution, we can substitute into the given equation and solve for any unknowns. Here we illustrate the method for first-order equations (see Sections 4.6 and 6.4 for the generalization to higher-order equations).

(a) Show that the general solution to (20)dydx+P(x)y=Q(x) has the formy(x)=Cyh(x)+yp(x),whereyh ( 0is a solution to equation (20) when Q(x)=0,

C is a constant, andyp(x)=v(x)yh(x) for a suitable function v(x). [Hint: Show that we can takeyh=μ-1(x) and then use equation (8).] We can in fact determine the unknown function yhby solving a separable equation. Then direct substitution of vyh in the original equation will give a simple equation that can be solved for v.

Use this procedure to find the general solution to (21) localid="1663920708127" dydx+3xy=x2, x > 0 by completing the following steps:

(b) Find a nontrivial solutionyh to the separable equation (22) localid="1663920724944" dydx+3xy=0, localid="1663920736626" x>0.

(c) Assuming (21) has a solution of the formlocalid="1663920777078" yp(x)=v(x)yh(x) , substitute this into equation (21), and simplify to obtain localid="1663920789271" v'(x)=x2yh(x).

d) Now integrate to getlocalid="1663920800433" vx

(e) Verify thatlocalid="1663920811828" y(x)=Cyh(x)+v(x)yh(x) is a general solution to (21).

Short Answer

Expert verified
  1. Proved
  2. yh=±k.x-3
  3. dvdx=x6
  4. v(x)=x66
  5. Proved

Step by step solution

01

Step 1(a): Show that the general solution to (20)dydx+P(x)y=Q(x)   has the formy(x)=Cyh(x)+yp(x) 

Here dydx+P(x)y=Q(x) and yh=μ-1(x)

So the equation is

dyhdx=-μ(x)-2dμdx

For

dμdx=P(x)μ(x)dyhdx=-μ(x)-1P(x)dyhdx=-y(x)P(x)

Rearranging them dyhdx+y(x)P(x)=0

The solution is

localid="1663919860296" width="275">y(x)=1μ(x)μ(x)Q(x)dx+CCyh(x)+yp(x)=1μ(x)μ(x)Q(x)dx+Cyp(x)=v(x)yh(x)=v(x)μ(x)-1=1μ(x)μ(x)Q(x)dx+Cv(x)=μ(x)Q(x)dx

Therefore the general solution is localid="1663920004724" v(x)=μ(x)Q(x)dx

02

Step 3(b): Find the nontrivial solution

Here dydx+3xy=0

Rearranging them

-13ydy=dxxlny=lnx-3-C

Raising power e on both sides thenyh=±k.x-3

(k is arbitrary constants)

Therefore the nontrivial solution is yh=±k.x-3.

03

Step 3(c): Determine the value of  v'(x)

Since yp(x)=v(x)yh(x)and substituteyh=v(x)x-3 then

dypdx+3xyp=x2v(x)dyhdx+yhdvdx+3xyh=x2v(x)dyhdx+3xyh+yhdvdx=x2

From part (b) v(x)dyhdx+3xyh=0then

yhdvdx=x2

Where yh=x-3 then

dvdx=x6

Therefore the value is role="math" localid="1663920371908" dvdx=x6.

04

Step 4(d): Find the value v(x)

Integrate the value

dvdx=x6v(x)=x66

Therefore the value is role="math" localid="1663920445772" v(x)=x66.

05

Step 5(e): Verify that  y(x)=Cyh(x)+v(x)yh(x) is a general solution to (21)

Since

y(x)=Cyh(x)+v(x)yh(x)y(x)=Cx-3+x66Calculate

dydx+3xyCx-3+x66-3Cx-4+3xCx-3+12x2+12x2=x2

Therefore, this verifies the result.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

In Problems 9–20, determine whether the equation is exact.

If it is, then solve it.

et(y - t)dt +(1 +et)dy = 0

Let ϕ(x)denote the solution to the initial value problem

dydx=x-y,y(0)=1

⦁ Show that ϕ(x)=1-ϕ'(x)=1-x+ϕ(x)

⦁ Argue that the graph of ϕ is decreasing for x near zero and that as x increases from zero, ϕ(x)decreases until it crosses the line y = x, where its derivative is zero.

⦁ Let x* be the abscissa of the point where the solution curve y=ϕ(x) crosses the line y=x.Consider the sign of ϕ(x*) and argue that ϕ has a relative minimum at x*.

⦁ What can you say about the graph of y=ϕ(x) for x > x*?

⦁ Verify that y = x – 1 is a solution to dydx=x-y and explain why the graph of y=ϕ(x) always stays above the line y=x-1.

⦁ Sketch the direction field for dydx=x-y by using the method of isoclines or a computer software package.

⦁ Sketch the solution y=ϕ(x) using the direction field in part (f).

Question:(a) Use the general solution given in Example 5 to solve the IVP. 4x"+e-0.1tx=0,x(0)=1,x'(0)=-12.Also use J'0(x)=-J1(x) and Y'0(x)=-Y1(x)=-Y1(x)along withTable 6.4.1 or a CAS to evaluate coefficients.

(b) Use a CAS to graph the solution obtained in part (a) for.

In Problems 9-13, determine whether the given relation is an implicit solution to the given differential equation. Assume that the relationship implicitly defines y as a function of x and use implicit differentiation.

x2+y2=4,dydx=xy

Using the Runge–Kutta algorithm for systems with h = 0.05, approximate the solution to the initial value problem y'''+y''+y2=t;y(0)=1,y'(0)=0,y''(0)=1 at t=1.

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free