The Definition — Question 3

Section 23-1 · Calculus pages 4065–4066

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Question 3

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 f(t)=sin⁡3tf(t)=\sin 3t for t≥0t\ge 0. Its truncated transform is FR(s)=∫0Re−stsin⁡3tdtF_R(s)=\int_0^R e^{-st}\sin 3t\,dt.

Tasks

  1. Evaluate FR(s)F_R(s) for real ss, retaining its upper-endpoint contribution.

  2. Find the exact real convergence interval for F(s)F(s) and determine whether convergence there is absolute.

  3. At s=0s=0, exhibit two sequences of upper endpoints giving different values of FR(0)F_R(0).

  4. Compare lim⁡s→0+F(s)\lim_{s\to 0^+}F(s) with the existence of F(0)F(0). Why does a finite parameter limit not justify interchanging the two limits R→∞R\to\infty and s→0+s\to 0^+?

Question 3 – Solution

Strategy. Damping by e−ste^{-st} can create convergence that disappears at the boundary parameter.

Step 1: Keep the endpoint term. Two integrations by parts, or differentiation of the resulting antiderivative, give FR(s)=3−e−sR[ssin⁡3R+3cos⁡3R]s2+9.\boxed{F_R(s)=\frac{3-e^{-sR}[s\sin 3R+3\cos 3R]}{s^2+9}.} There is no real zero of the denominator, but that alone says nothing about the limit as R→∞R\to\infty.

Step 2: Classify convergence. If s>0s>0, the endpoint term vanishes and F(s)=3s2+9,s>0.\boxed{F(s)=\frac 3{s^2+9},\qquad s>0.} Absolute convergence follows from |e−stsin⁡3t|≤e−st|e^{-st}\sin 3t|\le e^{-st}. If s<0s<0, take Rn=2nπ/3R_n=2n\pi/3. Then FRn(s)=3(1−e|s|Rn)/(s2+9)→−∞F_{R_n}(s)=3(1-e^{|s|R_n})/(s^2+9)\to-\infty, so the improper integral cannot converge.

Step 3: Test the boundary directly. At s=0s=0, FR(0)=(1−cos⁡3R)/3F_R(0)=(1-\cos 3R)/3. For Rn=2nπ/3,FRn(0)=0;Qn=(2n+1)π/3,FQn(0)=2/3.R_n=2n\pi/3,\quad F_{R_n}(0)=0;\qquad Q_n=(2n+1)\pi/3,\quad F_{Q_n}(0)=2/3. The two sequences tend to infinity but have different integral values. Thus F(0)F(0) does not exist, and the full real convergence interval is (0,∞)(0,\infty).

Step 4: Separate the two limiting procedures. The damped transforms satisfy lim⁡s→0+F(s)=1/3\lim_{s\to 0^+}F(s)=1/3. In contrast, setting s=0s=0 first produces an oscillating truncated integral with no limit. For fixed RR, the limit in ss exists, but convergence in RR is not uniform as damping disappears. The value 1/31/3 is a limit of damped integrals, not the value of the undamped improper integral. The graph compares accumulated integrals, not the original sine signal.

Diagram shown in the original SVG worksheet.