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Show that Ï•(x)=Ce3x+1is a solution tolocalid="1663944867164" dydx-3y=-3for any choice of the constant C. Thus,Ce3x+1 is a one-parameter family of solutions to the differential equation. Graph several of the solution curves using the same coordinate axes.

Short Answer

Expert verified

ϕx=Ce3x+1is a one-parameter family of solutions to dydx-3y=-3, for any choice of the constant C.

The graph for the solution curves is drawn.

Step by step solution

01

Taking the given function as y

First of all, take the given function as,ϕx=y

02

Differentiating the given function with respect to x

Differentiating ϕx=y=Ce3x+1, with respect to x,dydx=3Ce3x

03

Simplification of the differential equation obtained in step 2

dydx=3Ce3x+3-3dydx=3Ce3x+1-3dydx=3y-3dydx-3y=-3

Which is identical to the given differential equation.

Hence,ϕx=Ce3x+1 is a one-parameter family of solutions to dydx-3y=-3, for any choice of the constant C.

04

Representing the solution curves on a graph

When c=0

y=1(Represented with red colour)

When c=1

y=e3x+1(Represented with blue colour)

Whenc=-1

y=-e3x+1 (Represented with a blue-coloured dotted line)

When c=2

y=2e3x+1(Represented with orange colour)

Whenc=-2

y=-2e3x+1 (Represented with orange-coloured dotted line)

Graph representing the solution curves corresponding toc=0,±1,±2

Hence,Ï•(x)=Ce3x+1 is a one-parameter family of solutions todydx-3y=-3, for any choice of the constant C.

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Most popular questions from this chapter

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).

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

If it is, then solve it.

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

Consider the question of Example 5 ydydx-4x=0

  1. Does Theorem 1 imply the existence of a unique solution to (13) that satisfiesy(x0)=0?
  2. Show that when x0≠0equation (13) can’t possibly have a solution in a neighbourhood of x=x0that satisfies y(x0)=0.
  3. Show two distinct solutions to (13) satisfying y(0)=0 ( See Figure 1.4 on page 9).

Use the convolution theorem to find the inverse Laplace transform of the given function.

s+1(s2+1)2

In Problems 23-28, determine whether Theorem 1 implies that the given initial value problem has a unique solution.

ydydx=x,y(1)=0

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