Step Functions — Question 3

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Question 3

For a≥0a\ge 0, let ua(t)=0u_a(t)=0 for t<at<a and ua(t)=1u_a(t)=1 for t≥at\ge a. Use ordinary one-sided Laplace integrals for real ss; a value at one isolated point does not change an integral.

An oscillator is observed only during the window f(t)=sin⁡t[uπ/2(t)−u3π/2(t)].f(t)=\sin t\,[u_{\pi/2}(t)-u_{3\pi/2}(t)]. Use ℒ{cos⁡t}=s/(s2+1)\mathcal L\{\cos t\}=s/(s^2+1) for s>0s>0.

Tasks

  1. Write the exact piecewise function, including its values at both window endpoints.

  2. Express each switched sine using its local clock and derive F(s)F(s) for s>0s>0.

  3. Determine the full real convergence set, F(0)F(0) and F′(0)F'(0). Verify them by direct finite-interval integration.

  4. Explain why F(s)>0F(s)>0 for s>0s>0 even though the signal has both signs and zero unweighted integral. Use the window symmetry to justify the sign.

Original worksheet page 1: question and worked solution for 4-4-003
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Question 3 – Solution

Strategy. Re-express the phase at each switch separately. The second switch occurs at a different oscillator phase.

Step 1: Identify the window and endpoint values. The function equals sin⁡t\sin t on [π/2,3π/2)[\pi/2,3\pi/2) and zero elsewhere. In particular f(π/2)=1f(\pi/2)=1, while f(3π/2)=0f(3\pi/2)=0. At the latter time the left limit is −1-1; the graph distinguishes it from the assigned value.

Step 2: Shift the two phases correctly. With a=π/2a=\pi/2 and b=3π/2b=3\pi/2, we have sin⁡(v+a)=cos⁡v\sin(v+a)=\cos v and sin⁡(v+b)=−cos⁡v\sin(v+b)=-\cos v. Therefore f=ua(t)cos⁡(t−a)+ub(t)cos⁡(t−b),f=u_a(t)\cos(t-a)+u_b(t)\cos(t-b), F(s)=s(e−πs/2+e−3πs/2)s2+1.\boxed{F(s)=\frac{s(e^{-\pi s/2}+e^{-3\pi s/2})}{s^2+1}.} The plus sign in the transform reflects the phase reversal at shutoff. After bb, the two shifted cosine terms cancel exactly, as the original window requires.

Step 3: Use finite support to evaluate zero. The defining integral has finite support, so it converges for every real ss; finite-interval integration gives the displayed expression on the whole real line. Directly, F(0)=∫absin⁡tdt=0,F(0)=\int_a^b\sin t\,dt=0, F′(0)=−∫abtsin⁡tdt=−[−tcos⁡t+sin⁡t]ab=2.F'(0)=-\int_a^b t\sin t\,dt =-[-t\cos t+\sin t]_a^b=\boxed 2. The formula also gives F(0)=0F(0)=0 and expands as 2s+O(s2)2s+O(s^2), verifying the derivative.

Step 4: Pair the equal and opposite lobes. Write t=π+xt=\pi+x with −π/2≤x≤π/2-\pi/2\le x\le\pi/2. Pair xx with −x-x. For 0<x<π/20<x<\pi/2, the earlier value is sin⁡x>0\sin x>0 and the later value is −sin⁡x-\sin x. Their weighted contribution is e−πssin⁡x[esx−e−sx]>0(s>0).e^{-\pi s}\sin x\,[e^{sx}-e^{-sx}]>0\qquad(s>0). Integrating these pairs proves strict positivity, despite cancellation at s=0s=0. This also agrees with the positive numerator and denominator of the formula for s>0s>0.

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Original worksheet page 2: question and worked solution for 4-4-003

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