Table Of Laplace Transforms — Question 6

Section 23-10 · Calculus pages 4251–4252

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Question 6

Use causal one-sided Laplace transforms. Write Ha(t)=0H_a(t)=0 for t<at<a and 11 for t≥at\ge a. Ordinary functions are zero for t<0t<0. Justify the table entries and operational rules you use; give exact expressions.

Let pp be the continuous periodic triangular signal of period 22 with p(t)={t,0≤t≤1,2−t,1≤t<2,p(t+2)=p(t).p(t)=\begin{cases}t,&0\le t\le 1,\\2-t,&1\le t<2,\end{cases} \qquad p(t+2)=p(t). A standard table lists delayed ramps but does not list this periodic function.

Tasks

  1. Derive the periodic-transform formula by splitting the half-line into cycles. Apply it to this signal.

  2. Write a locally finite series of delayed ramps for pp and use it to obtain the same transform independently.

  3. Find the exact real transform domain. Compute lim⁡s→0+sP(s)\lim_{s\to 0^+}sP(s) and interpret it using the mean over one period.

  4. Explain why the cycle mean is not a pointwise final value, and determine the first two leading terms of P(s)P(s) as s→0+s\to 0^+.

Question 6 – Solution

Strategy. A one-cycle transform and a geometric series supply the periodic row; delayed ramps independently encode its slope changes.

Step 1: Sum the cycles. For s>0s>0, boundedness gives absolute convergence. Splitting into intervals [2n,2n+2][2n,2n+2] and translating yields P(s)=∫02e−stp(t)dt1−e−2s=(1−e−s)2s2(1−e−2s)=1−e−ss2(1+e−s).P(s)=\frac{\int_0^2e^{-st}p(t)\,dt}{1-e^{-2s}} =\boxed{\frac{(1-e^{-s})^2}{s^2(1-e^{-2s})} =\frac{1-e^{-s}}{s^2(1+e^{-s})}.} The one-cycle integral is (1−e−s)2/s2(1-e^{-s})^2/s^2, obtained by integration by parts on [0,1][0,1] and [1,2][1,2].

Step 2: Recover the slope changes. Write Ra=(t−a)Ha(t)R_a=(t-a)H_a(t). The series p(t)=∑n=0∞[R2n−2R2n+1+R2n+2]p(t)=\sum_{n=0}^\infty[R_{2n}-2R_{2n+1}+R_{2n+2}] is locally finite; each bracket is a unit triangular pulse on [2n,2n+2][2n,2n+2]. Its transform is e−2ns(1−2e−s+e−2s)/s2e^{-2ns}(1-2e^{-s}+e^{-2s})/s^2. Summing for s>0s>0 gives the same PP. These brackets, rather than the individual growing ramps across all cycles, also make absolute convergence clear.

Step 3: Check convergence and the mean. The signal is bounded, nonnegative and has area 11 per period. Thus the exact real domain is s>0s>0: at s=0s=0 the areas sum to infinity, and for s<0s<0 the weighted cycle contributions grow. Using (1−e−s)/(1+e−s)=tanh⁡(s/2)(1-e^{-s})/(1+e^{-s})=\tanh(s/2), lim⁡s→0+sP(s)=1/2\lim_{s\to 0^+}sP(s)=\boxed{1/2}, the cycle mean 1/21/2.

Step 4: Distinguish the limit notions. The samples p(2n)=0p(2n)=0 and p(2n+1)=1p(2n+1)=1 rule out a pointwise final value. Taylor expansion of the last quotient gives P(s)=12s−s24+O(s3).\boxed{P(s)=\frac 1{2s}-\frac{s}{24}+O(s^3).} The leading pole records the mean, while the constant term vanishes. The figure displays continuous corners and equal successive cycles.

Diagram shown in the original SVG worksheet.