Nonhomogeneous Differential Equations — Question 3

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Question 3

For y″+2y′+y=e−ty''+2y'+y=e^{-t} on ℝ\mathbb R, two proposed particular solutions are p(t)=12t2e−t,p̃(t)=e−t(12t2+3−2t).p(t)=\tfrac 12t^2e^{-t},\qquad \widetilde p(t)=e^{-t}(\tfrac 12t^2+3-2t). Two solvers write y=p+(A+Bt)e−ty=p+(A+Bt)e^{-t} and y=p̃+(α+βt)e−ty=\widetilde p+(\alpha+\beta t)e^{-t}.

Tasks

  1. Verify both particular solutions and explain why their difference must be homogeneous.

  2. Derive the exact relation between the two pairs of homogeneous constants. Do the two formulas describe different solution sets?

  3. Solve y(0)=2y(0)=2, y′(0)=−1y\prime(0)=-1 in both representations and verify the data.

  4. For the selected solution on t≥0t\ge 0, determine positivity, monotonicity and its limit. Explain why the particular and homogeneous pieces are not uniquely determined by the trajectory.

Original worksheet page 1: question and worked solution for 3-8-003
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Question 3 – Solution

Strategy. Changing the particular solution transfers a homogeneous term between the two pieces without changing the full solution.

Step 1: Verify efficiently. For any twice differentiable FF, differentiation gives (Fe−t)″+2(Fe−t)′+Fe−t=e−tF″.(Fe^{-t})''+2(Fe^{-t})'+Fe^{-t}=e^{-t}F''. Both supplied polynomials have second derivative 11, so both are particular solutions. Their difference (3−2t)e−t(3-2t)e^{-t} has zero residual, either by this identity or by subtracting the two forced equations.

Step 2: Match coefficients. Equality of the two representations is equivalent to A=α+3,B=β−2.\boxed{A=\alpha+3,\qquad B=\beta-2.} This is an invertible reassignment of constants, so the two formulas describe the same complete solution family.

Step 3: Impose the data. In the first representation, y(0)=Ay(0)=A and y′(0)=B−Ay'(0)=B-A, because p(0)=p′(0)=0p(0)=p'(0)=0. Thus A=2A=2, B=1B=1, while the second representation has α=−1\alpha=-1, β=3\beta=3. Both give y=e−t(2+t+12t2).\boxed{y=e^{-t}(2+t+\tfrac 12t^2).} Its initial value is 22. Differentiation gives y′=−e−t(1+12t2)y'=-e^{-t}(1+\tfrac 12t^2), whose value at zero is −1-1, as required.

Step 4: Interpret the complete trajectory. The derivative follows from subtracting the full polynomial when differentiating its exponential factor: y′=e−t[(1+t)−(2+t+12t2)]=−e−t(1+12t2).y'=e^{-t}[(1+t)-(2+t+\tfrac 12t^2)]=-e^{-t}(1+\tfrac 12t^2). For t≥0t\ge 0, y>0y>0 and y′<0y'<0; the polynomial times e−te^{-t} tends to zero. The same trajectory admits both decompositions above, so neither piece is unique without a chosen particular solution.

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