Systems of Differential Equations — Question 2

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Question 2

A scalar measurement of a three-state system is X′=AX,A=(010001−6−11−6),y=X1+2X2.X'=AX,\qquad A=\begin{pmatrix}0&1&0\\0&0&1\\-6&-11&-6\end{pmatrix}, \qquad y=X_1+2X_2. The measured initial derivatives are y(0)=1y(0)=1, y′(0)=0y'(0)=0, y″(0)=−12y''(0)=-12. All coefficients are constant and t∈ℝt\in\mathbb R.

Tasks

  1. Form the matrix OO such that (y,y′,y″)T=OX(y,y',y'')^T=OX. Determine whether the three measured derivatives uniquely determine the state.

  2. Derive a scalar third-order equation for yy and explicit reconstruction formulas for all three state components in terms of y,y′,y″y,y',y''.

  3. Recover X(0)X(0) and find the measured response y(t)y(t) explicitly.

  4. Prove that every solution of your scalar equation reconstructs a solution of the original system. Verify the recovered trajectory and explain why differentiating the measurement has lost no state information.

Original worksheet page 1: question and worked solution for 7-6-002
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Question 2 – Solution

Strategy. Invert the map from state coordinates to the measurement’s derivative coordinates.

Step 1: Test the measurement map. With c=(1,2,0)c=(1,2,0), the rows of OO are c,cA,cA2c,cA,cA^2. Hence O=(120012−12−22−11),det⁡O=−15≠0.O=\begin{pmatrix}1&2&0\\0&1&2\\-12&-22&-11\end{pmatrix},\qquad \det O=-15\ne 0. The derivative triple determines the state uniquely.

Step 2: Convert and reconstruct. The identity A3+6A2+11A+6I=0A^3+6A^2+11A+6I=0 gives y‴+6y″+11y′+6y=0.\boxed{y'''+6y''+11y'+6y=0.} Solving OX=(y,y′,y″)TOX=(y,y',y'')^T gives X1=(−33y−22y′−4y″)/15,X2=(24y+11y′+2y″)/15,X3=(−12y+2y′−y″)/15.\boxed{\begin{aligned} X_1&=(-33y-22y'-4y'')/15,\\ X_2&=(24y+11y'+2y'')/15,\\ X_3&=(-12y+2y'-y'')/15. \end{aligned}}

Step 3: Solve the recovered IVP. The measured data give X(0)=(1,0,0)TX(0)=(1,0,0)^T. The scalar roots are −1,−2,−3-1,-2,-3; imposing the measured derivative triple yields y=−3e−t+9e−2t−5e−3t.\boxed{y=-3e^{-t}+9e^{-2t}-5e^{-3t}.} The state is X=(f,f′,f″)TX=(f,f',f'')^T, where f=3e−t−3e−2t+e−3tf=3e^{-t}-3e^{-2t}+e^{-3t}. In particular, f+2f′=yf+2f'=y and (f,f′,f″)(0)=(1,0,0)(f,f',f'')(0)=(1,0,0).

Step 4: Prove full equivalence. If Z=(y,y′,y″)TZ=(y,y',y'')^T, then Z′=BZZ'=BZ with last row of BB equal to (−6,−11,−6)(-6,-11,-6). Direct multiplication gives OA=BOOA=BO, so for any scalar solution, X=O−1ZX=O^{-1}Z satisfies X′=O−1BZ=AXX'=O^{-1}BZ=AX. Its measurement is yy by the first row of OO. Conversely every state solution produces this scalar equation. The recovered ff satisfies f‴+6f″+11f′+6f=0f'''+6f''+11f'+6f=0, checking the original last row directly. Invertibility of OO proves that no hidden state was discarded.

Original worksheet page 2: question and worked solution for 7-6-002

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