Systems of Differential Equations — Question 5

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Question 5

Let X′=AX,A=(01−10),X(0)=(0,1)T,X'=AX,\quad A=\begin{pmatrix}0&1\\-1&0\end{pmatrix},\qquad X(0)=(0,1)^T, and introduce a time-dependent coordinate system X=P(t)ZX=P(t)Z, where P(t)=(1t01).P(t)=\begin{pmatrix}1&t\\0&1\end{pmatrix}. The physical state XX and its coordinate column ZZ describe the same vector using different bases at different times.

Tasks

  1. Derive the differential equation for ZZ by differentiating X=PZX=PZ. Explain why the constant-basis formula P−1APP^{-1}AP is insufficient.

  2. Compute the coefficient matrix and initial state for ZZ. Classify the transformed system as linear, homogeneous, and autonomous or nonautonomous.

  3. Verify the supplied physical trajectory X(t)=(sin⁡t,cos⁡t)TX(t)=(\sin t,\cos t)^T. Obtain Z(t)Z(t) and check both transformed equations directly.

  4. Compare X′(0)X\prime(0) with Z′(0)Z\prime(0). Explain how a zero instantaneous coordinate derivative can coexist with a changing physical vector.

Original worksheet page 1: question and worked solution for 5-4-005
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Question 5 – Solution

Strategy. A moving basis contributes its own derivative; keep that contribution before multiplying by the inverse.

Step 1: Differentiate the whole change of coordinates. Since X′=P′Z+PZ′=APZX'=P'Z+PZ'=APZ, invertibility of PP gives Z′=P−1(AP−P′)Z.\boxed{Z'=P^{-1}(AP-P')Z.} Dropping P′P' would treat a moving basis as fixed and generally produce incorrect coordinate derivatives. Here det⁡P=1\det P=1 for all real tt.

Step 2: Compute the transformed system. The matrices are P−1=(1−t01),AP−P′=(00−1−t).P^{-1}=\begin{pmatrix}1&-t\\0&1\end{pmatrix},\qquad AP-P'=\begin{pmatrix}0&0\\-1&-t\end{pmatrix}. Consequently Z′=(tt2−1−t)Z,Z(0)=(0,1)T.\boxed{Z'=\begin{pmatrix}t&t^2\\-1&-t\end{pmatrix}Z, \qquad Z(0)=(0,1)^T.} This system is linear and homogeneous, but nonautonomous. Explicit time dependence can arise entirely from a time-dependent choice of coordinates.

Step 3: Check the supplied trajectory in both descriptions. For X=(sin⁡t,cos⁡t)TX=(\sin t,\cos t)^T, X′=(cos⁡t,−sin⁡t)T=AXX'=(\cos t,-\sin t)^T=AX, with the stated data. Multiplication by P−1P^{-1} gives Z=(sin⁡t−tcos⁡t,cos⁡t)T.\boxed{Z=(\sin t-t\cos t,\,\cos t)^T.} Its derivative is (tsin⁡t,−sin⁡t)T(t\sin t,-\sin t)^T. The transformed right-hand side is also (t(sin⁡t−tcos⁡t)+t2cos⁡t,−(sin⁡t−tcos⁡t)−tcos⁡t)T(t(\sin t-t\cos t)+t^2\cos t,-(\sin t-t\cos t)-t\cos t)^T, which simplifies to the same vector.

Step 4: Interpret the instantaneous difference. At 00, X′=(1,0)TX'=(1,0)^T but Z′=(0,0)TZ'=(0,0)^T. The identity X′=P′Z+PZ′X'=P'Z+PZ' explains this: P′(0)Z(0)=(1,0)TP'(0)Z(0)=(1,0)^T. The basis motion accounts for the entire instantaneous change. The figure compares the first components; the coordinate curve starts with a horizontal tangent while the physical component has slope 11.

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Original worksheet page 2: question and worked solution for 5-4-005

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