Systems of Differential Equations — Question 6

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Question 6

Let D=d/dtD=d/dt. Ordered differential factors act from right to left in (D+1)(D−t)(D−1)y=0,(y,y′,y″)(0)=(0,0,1).(D+1)(D-t)(D-1)y=0,\qquad (y,y',y'')(0)=(0,0,1). Here (D−t)f=f′−tf(D-t)f=f'-tf. Multiplication by tt does not commute with differentiation.

Tasks

  1. Define q1=yq_1=y, q2=(D−1)yq_2=(D-1)y, q3=(D−t)q2q_3=(D-t)q_2. Derive the first-order system for qq and its initial vector.

  2. Expand the scalar third-order equation and show that the change between (y,y′,y″)(y,y',y'') and qq is invertible for every real tt.

  3. Solve the triangular system by successive integrating factors. Give an explicit nested-integral formula for yy and verify the initial data and equation through the state relations.

  4. Compare the given operator with (D−t)(D+1)(D−1)(D-t)(D+1)(D-1). Compute their difference, and exhibit a function that solves the reordered equation but not the original one.

Original worksheet page 1: question and worked solution for 7-6-006
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Question 6 – Solution

Strategy. Keep the factors in their stated order and regard intermediate derivatives as state coordinates.

Step 1: Form the ordered cascade. The definitions give q1′=q1+q2,q2′=tq2+q3,q3′=−q3,q(0)=(0,0,1)T.\boxed{q_1'=q_1+q_2,\qquad q_2'=tq_2+q_3,\qquad q_3'=-q_3,\qquad q(0)=(0,0,1)^T.} In particular, q3=y″−(t+1)y′+tyq_3=y''-(t+1)y'+ty; using only y″y'' as this coordinate would lose the variable-coefficient terms.

Step 2: Expand and invert the coordinate map. Differentiating the expression for q3q_3 and adding q3q_3 yields y‴−ty″−2y′+(t+1)y=0.\boxed{y'''-t y''-2y'+(t+1)y=0.} The coordinate matrix is q=(100−110t−(t+1)1)(yy′y″),det⁡=1.q=\begin{pmatrix}1&0&0\\-1&1&0\\t&-(t+1)&1\end{pmatrix} \begin{pmatrix}y\\y'\\y''\end{pmatrix},\qquad \det=1. Its inverse relations are y=q1y=q_1, y′=q1+q2y'=q_1+q_2 and y″=q1+(t+1)q2+q3y''=q_1+(t+1)q_2+q_3, so the conversion is globally reversible.

Step 3: Integrate in triangular order. Successive integrating factors give q3=e−t,q2=et2/2∫0te−v−v2/2dv,q_3=e^{-t},\qquad q_2=e^{t^2/2}\int_0^t e^{-v-v^2/2}\,dv, y(t)=et∫0te−u+u2/2(∫0ue−v−v2/2dv)du.\boxed{y(t)=e^t\int_0^t e^{-u+u^2/2} \left(\int_0^u e^{-v-v^2/2}\,dv\right)du.} These oriented integrals apply to every real tt. Their derivatives give the three cascade equations. At zero the state is (0,0,1)(0,0,1), and the inverse relations give (y,y′,y″)=(0,0,1)(y,y',y'')=(0,0,1). Finally q3′+q3=0q_3'+q_3=0 verifies the original ordered product directly.

Step 4: Quantify the order error. The commutator (D+1)(D−t)−(D−t)(D+1)(D+1)(D-t)-(D-t)(D+1) is multiplication by −1-1. Thus the original operator minus the reordered one equals −(D−1)-(D-1). The reordered operator is D3−tD2−D+tD^3-tD^2-D+t, whereas the original has the extra −D+1-D+1. For y=e−ty=e^{-t} the reordered product vanishes, but the original gives 2e−t≠02e^{-t}\ne 0. Reordering these factors changes the solution space.

Original worksheet page 2: question and worked solution for 7-6-006

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