Laplace Transforms — Question 3

Section 24-11 · Calculus pages 4465–4466

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Question 3

A delayed input drives the zero-state system x′=−x+H(t−2),y′=x−2y,x(0)=y(0)=0,t≥0.x'=-x+H(t-2),\qquad y'=x-2y,\qquad x(0)=y(0)=0,\quad t\ge 0. Here H(t−a)H(t-a) is zero for t<at<a and one for t>at>a; its value at the switch does not affect the continuous state. Interpret derivatives there one-sidedly.

Tasks

  1. Find the transforms of both components and identify the factor that encodes the input delay.

  2. Invert them to obtain a piecewise solution. Explain why multiplying an undelayed response by e−2te^{-2t} does not implement a delay.

  3. Determine continuity of x,y,x′,y′x,y,x',y' at t=2t=2, and find the one-sided values of y″y'' there.

  4. Prove both components increase after the switch and approach their limits without overshoot. Sketch their time responses, marking the switch and limiting levels.

Question 3 – Solution

Strategy. First invert the undelayed rational factors, then translate the entire response using the second shifting theorem.

Step 1: Transform both equations. With F=ℒ{x}F=\mathcal L\{x\} and G=ℒ{y}G=\mathcal L\{y\}, (s+1)F=e−2s/s(s+1)F=e^{-2s}/s and (s+2)G=F(s+2)G=F. Hence F=e−2ss(s+1),G=e−2ss(s+1)(s+2),Re⁡s>0.F=\frac{e^{-2s}}{s(s+1)},\qquad G=\frac{e^{-2s}}{s(s+1)(s+2)},\qquad \operatorname{Re}s>0. It is e−2se^{-2s}, rather than an exponential in time, that encodes the delay.

Step 2: Shift the inverse transforms. The undelayed inverses are 1−e−t1-e^{-t} and 12−e−t+12e−2t=12(1−e−t)2\tfrac 12-e^{-t}+\tfrac 12e^{-2t}=\tfrac 12(1-e^{-t})^2. Writing τ=t−2\tau=t-2, the solution is zero for t<2t<2, and for t≥2t\ge 2, x=1−e−τ,y=12(1−e−τ)2.\boxed{x=1-e^{-\tau},\qquad y=\tfrac 12(1-e^{-\tau})^2.} These formulas give zero at the joining point. Multiplication by e−2te^{-2t} would change decay rates while generally leaving a nonzero response before t=2t=2; it is a different transform operation.

Step 3: Check the switch regularity. Both states are continuous. Before the switch their derivatives vanish; after it x′=e−τx'=e^{-\tau} and y′=e−τ−e−2τy'=e^{-\tau}-e^{-2\tau}. Thus x′(2−)=0x'(2^-)=0, x′(2+)=1x'(2^+)=1, whereas y′(2−)=y′(2+)=0y'(2^-)=y'(2^+)=0. Afterward y″=−e−τ+2e−2τy''=-e^{-\tau}+2e^{-2\tau}, so y″(2−)=0,y″(2+)=1\boxed{y''(2^-)=0,\ y''(2^+)=1}. In particular yy is continuously differentiable at the switch but is not twice differentiable there.

Step 4: Establish shape and limits. For τ>0\tau>0, x′>0x'>0 and y′=e−τ(1−e−τ)>0y'=e^{-\tau}(1-e^{-\tau})>0. Also 0<x<10<x<1 and 0<y<1/20<y<1/2, with limits 11 and 1/21/2. These inequalities prove the absence of overshoot for all later times. The dotted horizontal guides in the sketch are limits; the solid and dashed curves are the components. Both remain zero throughout the waiting interval.

Diagram shown in the original SVG worksheet.