Systems of Differential Equations — Question 5

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Question 5

Two coupled displacements satisfy x″+2x−z=0,z″+2z−x=0,x''+2x-z=0,\qquad z''+2z-x=0, with (x,x′,z,z′)(0)=(1,0,0,0)(x,x',z,z')(0)=(1,0,0,0). Time is measured in units that make the coefficients dimensionless.

Tasks

  1. Write a four-state first-order system using the order (x,x′,z,z′)(x,x',z,z'). Eliminate zz to obtain a fourth-order scalar equation for xx and translate all four initial values.

  2. Introduce u=x+zu=x+z, v=x−zv=x-z. Solve the resulting independent equations and recover x,zx,z.

  3. Prove that every solution of the scalar fourth-order equation reconstructs a unique solution of the coupled equations. Verify the prescribed solution and its initial data.

  4. Derive a positive conserved energy, express it in u,vu,v, and use it to prove boundedness. Sketch both displacements for 0≤t≤120\leq t\leq 12 and explain how two different frequencies appear.

Original worksheet page 1: question and worked solution for 7-6-005
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Question 5 – Solution

Strategy. Compare the derivative-state, scalar-elimination and normal-mode descriptions of the same four-dimensional motion.

Step 1: Convert and transfer the initial state. For X=(x,x′,z,z′)TX=(x,x',z,z')^T, X′=(0100−2010000110−20)X.X'=\begin{pmatrix}0&1&0&0\\-2&0&1&0\\0&0&0&1\\1&0&-2&0\end{pmatrix}X. Since z=x″+2xz=x''+2x, substitution into the second equation gives x(4)+4x″+3x=0,(x,x′,x″,x‴)(0)=(1,0,−2,0).\boxed{x^{(4)}+4x''+3x=0,\qquad(x,x',x'',x''')(0)=(1,0,-2,0).}

Step 2: Solve the normal modes. Adding and subtracting give u″+u=0u''+u=0, v″+3v=0v''+3v=0, with initial displacements one and velocities zero. Thus x=12(cos⁡t+cos⁡(3t)),z=12(cos⁡t−cos⁡(3t)).\boxed{x=\tfrac 12(\cos t+\cos(\sqrt 3t)),\qquad z=\tfrac 12(\cos t-\cos(\sqrt 3t)).}

Step 3: Prove reversibility. For any scalar solution, define z=x″+2xz=x''+2x. The first coupled equation is then an identity, and the second has residual x(4)+4x″+3x=0x^{(4)}+4x''+3x=0. This formula also proves uniqueness of zz. The displayed cosines satisfy the scalar factors (D2+1)(D2+3)(D^2+1)(D^2+3) and give z(0)=z′(0)=0z(0)=z'(0)=0 as required.

Step 4: Check energy and boundedness. Multiplying the equations by x′,z′x',z' and adding proves conservation of E=12(x′2+z′2)+x2+z2−xz=14(u′2+u2+v′2+3v2)=1.E=\tfrac 12(x'^2+z'^2)+x^2+z^2-xz =\tfrac 14(u'^2+u^2+v'^2+3v^2)=1. Since x2+z2−xz≥(x2+z2)/2x^2+z^2-xz\geq(x^2+z^2)/2, both displacements are bounded; the explicit formulas sharpen this to |x|,|z|≤1|x|,|z|\leq 1. Each displacement mixes the frequencies 11 and 3\sqrt 3.

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Original worksheet page 2: question and worked solution for 7-6-005

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