Table Of Laplace Transforms — Question 3

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Question 3

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.

A short table gives only ℒ{sin⁡(at)}=a/(s2+a2)\mathcal L\{\sin(at)\}=a/(s^2+a^2), where a>0a>0. You need inverses of Aa(s)=s(s2+a2)2,Ba(s)=1(s2+a2)2.A_a(s)=\frac{s}{(s^2+a^2)^2},\qquad B_a(s)=\frac 1{(s^2+a^2)^2}.

Tasks

  1. Derive the inverse of AaA_a by differentiating a transform with respect to ss.

  2. Derive the inverse of BaB_a by differentiating the given sine entry with respect to aa. Explain why the parameter differentiation is justified for real s>0s>0.

  3. Check the first nonzero Taylor term at t=0t=0 against the leading large-ss term of each transform.

  4. Find both pointwise limits as a→0+a\to 0^+ and explain why substituting a=0a=0 into an unsimplified inverse formula is invalid.

Original worksheet page 1: question and worked solution for 4-10-003
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Question 3 – Solution

Strategy. Generate missing table rows through operations whose normalization can be checked independently.

Step 1: Differentiate with respect to ss. Since −dds[a/(s2+a2)]=2as/(s2+a2)2-\frac{d}{ds}[a/(s^2+a^2)]=2as/(s^2+a^2)^2, ℒ−1{Aa}=tsin⁡(at)2a.\boxed{\mathcal L^{-1}\{A_a\}=\frac{t\sin(at)}{2a}.} The factor 2a2a must be divided out.

Step 2: Differentiate with respect to aa. The parameter derivative gives ℒ{tcos⁡(at)}=(s2−a2)/(s2+a2)2\mathcal L\{t\cos(at)\}=(s^2-a^2)/(s^2+a^2)^2. For fixed s>0s>0, te−stt e^{-st} dominates the differentiated integrand uniformly in aa, justifying differentiation under the integral. Subtracting this row from ℒ{sin⁡(at)/a}\mathcal L\{\sin(at)/a\} yields 1s2+a2−s2−a2(s2+a2)2=2a2(s2+a2)2.\frac 1{s^2+a^2}-\frac{s^2-a^2}{(s^2+a^2)^2} =\frac{2a^2}{(s^2+a^2)^2}. Thus ℒ−1{Ba}=sin⁡(at)−atcos⁡(at)2a3.\boxed{\mathcal L^{-1}\{B_a\}= \frac{\sin(at)-at\cos(at)}{2a^3}.}

Step 3: Check the onset powers. The inverses start as t2/2+O(t4)t^2/2+O(t^4) and t3/6+O(t5)t^3/6+O(t^5). Their leading transforms are respectively 1/s31/s^3 and 1/s41/s^4, matching AaA_a and BaB_a. This checks both factorials and the cancellation of the linear term in the second numerator.

Step 4: Remove the apparent parameter singularities. At each fixed tt, the Taylor expansions give limits t2/2t^2/2 and t3/6t^3/6. Their transforms are 1/s31/s^3 and 1/s41/s^4, agreeing with the limits of the rational functions for s>0s>0. Directly inserting a=0a=0 into the inverse quotients produces 0/00/0; the limits require cancellation first. The figure uses a=1a=1 and shows that the repeated denominator can produce oscillations with increasing size, unlike a single sine entry.

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