Solutions to Systems — Question 1

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Question 1

For X′=AXX'=AX, with A=(1101)A=\begin{pmatrix}1&1\\0&1\end{pmatrix}, consider U(t)=et(1,0)T,V(t)=et(t,1)T,W(t)=et(1,t)T.U(t)=e^t(1,0)^T,\quad V(t)=e^t(t,1)^T,\quad W(t)=e^t(1,t)^T. A vector solution must satisfy both rows at every time in its interval. A fundamental matrix has solution columns that form a basis at each time.

Tasks

  1. Compute the residual F′−AFF\prime-AF for each candidate F=U,V,WF=U,V,W. Decide which are solutions on a nonempty open interval.

  2. Use the valid candidates to form a fundamental matrix. Prove that every solution is their constant linear combination, rather than merely checking that combinations work.

  3. Solve the IVP X(0)=(2,−1)TX(0)=(2,-1)^T and verify both the equations and initial data.

  4. For this IVP, find the first zero of its first component for t≥0t\ge 0. Determine the full state and derivative there, and explain why a zero component does not mean a zero solution.

Original worksheet page 1: question and worked solution for 5-5-001
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Question 1 – Solution

Strategy. Check vector residuals first; then solve the triangular equations to establish completeness.

Step 1: Test all candidates. Direct differentiation gives U′−AU=0U'-AU=0 and V′−AV=0V'-AV=0. For the third candidate, W′=et(1,t+1)T,AW=et(1+t,t)T,W′−AW=et(−t,1)T.W'=e^t(1,t+1)^T,\quad AW=e^t(1+t,t)^T, \quad\boxed{W'-AW=e^t(-t,1)^T.} Its second residual component never vanishes, so WW is not a solution on any nonempty open interval.

Step 2: Prove that the valid family is complete. The matrix Φ=(UV)=et(1t01)\Phi=(U\ V)=e^t\begin{pmatrix}1&t\\0&1\end{pmatrix} has determinant e2t>0e^{2t}>0. More explicitly, the second equation gives y=c2ety=c_2e^t. Then (e−tx)′=c2(e^{-t}x)'=c_2, so X=et(c1+c2t,c2)T=c1U+c2V.\boxed{X=e^t(c_1+c_2t,c_2)^T=c_1U+c_2V.} This derivation reaches every solution and introduces exactly two arbitrary constants. The family is valid on the whole real axis.

Step 3: Select and verify the initial-value solution. At 00, the constants are c1=2c_1=2, c2=−1c_2=-1, hence X=et(2−t,−1)T\boxed{X=e^t(2-t,-1)^T}. Its derivative is et(1−t,−1)Te^t(1-t,-1)^T, exactly AXAX, and its initial state is (2,−1)T(2,-1)^T as required.

Step 4: Interpret a component zero. Since et≠0e^t\ne 0, the first component first vanishes at t=2t=2. There X(2)=(0,−e2)TX(2)=(0,-e^2)^T and X′(2)=(−e2,−e2)TX'(2)=(-e^2,-e^2)^T. The state is nonzero and continues moving; the first component crosses zero with negative slope. For a homogeneous linear system with continuous coefficients, only a full zero state at a time would force the identically zero solution by uniqueness. The plot displays both components.

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