The Definition — Question 9

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Question 9

For real ss, use F(s)=∫0∞e−stf(t)dtF(s)=\int_0^\infty e^{-st}f(t)\,dt whenever this ordinary improper integral converges.

Let ff have period two, with f(t)=1f(t)=1 for 0≤t<10\le t<1 and f(t)=0f(t)=0 for 1≤t<21\le t<2, repeated for all t≥0t\ge 0. Use the definition rather than a precomputed periodic-transform formula.

Tasks

  1. Split the integral into complete periods, sum the resulting series, and determine the exact real convergence set.

  2. Simplify the transform on its convergence interval.

  3. Compute lim⁡s→0+sF(s)\lim_{s\to 0^+}sF(s) and lim⁡s→∞sF(s)\lim_{s\to\infty}sF(s). Relate these to the period average and to the signal just after zero.

  4. If the defining integral is truncated after NN complete periods, find its exact relative error for s>0s>0. At s=0.2s=0.2, find the smallest integer NN making that error at most 10−310^{-3}.

Original worksheet page 1: question and worked solution for 4-1-009
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Question 9 – Solution

Strategy. A time translation by one period multiplies the weighted area by a fixed factor, producing a geometric series.

Step 1: Build the series and its domain. For s>0s>0, the nnth nonzero interval contributes ∫2n2n+1e−stdt=e−2ns1−e−ss.\int_{2n}^{2n+1}e^{-st}\,dt=e^{-2ns}\frac{1-e^{-s}}s. The ratio e−2se^{-2s} lies in (0,1)(0,1), so the sum converges. At s=0s=0, each interval contributes one and the sum diverges. For s<0s<0, e−st≥1e^{-st}\ge 1 on each such interval, so it also diverges. The real convergence set is exactly (0,∞)(0,\infty), with absolute convergence since f≥0f\ge 0.

Step 2: Simplify the geometric sum. Summing gives F(s)=1−e−ss(1−e−2s)=1s(1+e−s),s>0.F(s)=\frac{1-e^{-s}}{s(1-e^{-2s})} =\boxed{\frac 1{s(1+e^{-s})},\qquad s>0.} The integral over only one period is the first term of this sum, not the transform of the endlessly repeated signal.

Step 3: Interpret the two normalized limits. The formula gives lims→0+sF(s)=12,lims→∞sF(s)=1.\boxed{\lim_{s\to 0^+}sF(s)=\tfrac 12,\qquad \lim_{s\to\infty}sF(s)=1.} The first value is the period average (1/2)∫02f(t)dt=1/2(1/2)\int_0^2f(t)\,dt=1/2. The second agrees with f(0+)=1f(0^+)=1: large ss weights short times most strongly. These normalized limits do not assert that F(0)F(0) exists; it does not.

Step 4: Quantify finite-window error. Writing FN=∫02Ne−stf(t)dtF_N=\int_0^{2N}e^{-st}f(t)\,dt, the finite geometric sum gives FN=F(s)(1−e−2Ns),F(s)−FNF(s)=e−2Ns.F_N=F(s)(1-e^{-2Ns}),\qquad \boxed{\frac{F(s)-F_N}{F(s)}=e^{-2Ns}.} At s=0.2s=0.2, the requirement is e−0.4N≤10−3e^{-0.4N}\le 10^{-3}, so N≥ln⁡(1000)/0.4≈17.27N\ge\ln(1000)/0.4\approx 17.27. The least integer is N=18\boxed{N=18}, corresponding to a cutoff time of 3636. Endpoint assignments do not affect the integrals; the graph uses the values specified in the question.

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Original worksheet page 2: question and worked solution for 4-1-009

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