Systems of Differential Equations — Question 7

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Question 7

For a real constant κ\kappa, consider the implicit derivative equations x′+y′=−x,x′+κy′=y.x'+y'=-x,\qquad x'+\kappa y'=y. A classical solution is a continuously differentiable pair satisfying both relations throughout an interval. An algebraically consistent derivative at one state is not necessarily part of a solution through that state.

Tasks

  1. Write MκX′=BXM_\kappa X\prime=BX and determine exactly when it can be solved for a unique derivative at every state. Find the explicit system in that case.

  2. At κ=1\kappa=1, determine the states at which the two equations are algebraically consistent for a derivative. Describe the possible derivatives at such a state.

  3. Still at κ=1\kappa=1, find every classical solution on an interval of positive length. Explain why most instantaneously consistent states cannot be used as initial data.

  4. For κ≠1\kappa\ne 1 and initial state (x,y)=(1,−1)(x,y)=(1,-1), compute the initial derivative and the derivative of x+yx+y. Does a finite, parameter-independent initial velocity imply that a solution exists through the same state at κ=1\kappa=1?

Original worksheet page 1: question and worked solution for 5-4-007
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Question 7 – Solution

Strategy. Separate invertibility of the derivative matrix from the extra consistency conditions imposed when its rank drops.

Step 1: Solve when the derivative matrix is invertible. Here Mκ=(111κ),B=(−1001),det⁡Mκ=κ−1.M_\kappa=\begin{pmatrix}1&1\\1&\kappa\end{pmatrix},\quad B=\begin{pmatrix}-1&0\\0&1\end{pmatrix},\quad \det M_\kappa=\kappa-1. For κ≠1\kappa\ne 1, inversion yields X′=1κ−1(−κ−111)X.\boxed{X'=\frac 1{\kappa-1} \begin{pmatrix}-\kappa&-1\\1&1\end{pmatrix}X.} This constant linear system has a unique solution for every initial state.

Step 2: Test instantaneous algebraic consistency. At κ=1\kappa=1, the left sides coincide, so the right sides must satisfy y=−xy=-x. At a state (a,−a)(a,-a), the derivative pairs (p,q)(p,q) satisfy p+q=−ap+q=-a, an entire line of possibilities. Outside y=−xy=-x, no derivative can satisfy both equations even at that instant.

Step 3: Enforce the constraint along a solution. A classical solution must have y(t)=−x(t)y(t)=-x(t) at every time. Differentiating this identity gives x′+y′=0x'+y'=0. The first equation then forces x=0x=0, and the constraint forces y=0y=0. Therefore X(t)≡(0,0)T is the only classical solution at κ=1.\boxed{X(t)\equiv(0,0)^T\text{ is the only classical solution at }\kappa=1.} It indeed satisfies both equations. Nonzero points on the consistency line admit instantaneous derivatives but no solution interval through them. Even at the origin, most algebraic derivative choices cannot persist.

Step 4: Check the limiting initial velocity. Substituting (1,−1)(1,-1) into the explicit system gives x′=(−κ+1)/(κ−1)=−1x'=(-\kappa+1)/(\kappa-1)=-1 and y′=0y'=0 for every κ≠1\kappa\ne 1. Thus (x+y)′=−1(x+y)'=-1, although initially x+y=0x+y=0. This velocity does not keep the state on the constraint line required at κ=1\kappa=1. Its finiteness does not imply a limiting solution through (1,−1)(1,-1); Step 3 proves that no such solution exists at that parameter.

Original worksheet page 2: question and worked solution for 5-4-007

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