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Fundamentals Of Differential Equations And Boundary Value Problems
Found in: Page 1
Fundamentals Of Differential Equations And Boundary Value Problems

Fundamentals Of Differential Equations And Boundary Value Problems

Book edition 9th
Author(s) R. Kent Nagle, Edward B. Saff, Arthur David Snider
Pages 616 pages
ISBN 9780321977069

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Short Answer

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), where yh ( 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 take yh=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 solution yh 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 get localid="1663920800433" vx

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

  1. Proved
  2. yh=±k.x-3
  3. dvdx=x6
  4. v(x)=x66
  5. Proved
See the step by step solution

Step by Step Solution

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" style="max-width: none;" 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

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.

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=0 then

yhdvdx=x2

Where yh=x-3 then

dvdx=x6

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

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 .

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.

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