Laplace Transforms — Question 10

PDF ↗

Question 10

For real ss, write ℒ{f}(s)=F(s)=∫0∞e−stf(t)dt\mathcal L\{f\}(s)=F(s)=\int_0^\infty e^{-st}f(t)\,dt where the integral converges.

Let ff be twice continuously differentiable, with f,f′,f″f,f',f'' of exponential order. Work at sufficiently large real ss so that all transforms below converge and all exponential boundary terms vanish. You may use ℒ{f′}=sF−f(0),ℒ{tf}=−F′,ℒ{f″}=s2F−sf(0)−f′(0).\mathcal L\{f'\}=sF-f(0),\qquad \mathcal L\{tf\}=-F',\qquad \mathcal L\{f''\}=s^2F-sf(0)-f'(0).

Tasks

  1. Compute ℒ{(tf)′}\mathcal L\{(tf)'\} and ℒ{tf′}\mathcal L\{tf'\} separately. Explain their difference using the product rule in time.

  2. Verify both results explicitly for f(t)=e−tf(t)=e^{-t}.

  3. Derive ℒ{t2f″}\mathcal L\{t^2f''\}, carefully differentiating every ss-dependent factor.

  4. A student keeps only s2F″s^2F'' in the last result. Identify the missing terms and verify the correct formula for f=e−tf=e^{-t} by transforming t2e−tt^2e^{-t} directly.

Original worksheet page 1: question and worked solution for 4-2-010
Show solutionHide solution

Question 10 – Solution

Strategy. Multiplication by time and differentiation in time correspond to operations in ss that must be applied in the correct order.

Step 1: Compare the two orders. Since (tf)(0)=0(tf)(0)=0, applying the time-derivative rule after time multiplication gives ℒ{(tf)′}=−sF′(s).\boxed{\mathcal L\{(tf)'\}=-sF'(s).} In the opposite order, parameter differentiation applies to the entire transform of f′f': ℒ{tf′}=−dds[sF(s)−f(0)]=−F(s)−sF′(s).\boxed{\mathcal L\{tf'\}=-\frac d{ds}[sF(s)-f(0)]=-F(s)-sF'(s).} Their difference is F(s)F(s), exactly as required by (tf)′−tf′=f(tf)'-tf'=f. The initial value f(0)f(0) is constant in ss and differentiates to zero.

Step 2: Check a concrete example. For f=e−tf=e^{-t}, F=1/(s+1)F=1/(s+1) and F′=−1/(s+1)2F'=-1/(s+1)^2. The formulas predict ℒ{(1−t)e−t}=s(s+1)2,ℒ{−te−t}=−1(s+1)2.\mathcal L\{(1-t)e^{-t}\}=\frac{s}{(s+1)^2},\qquad \mathcal L\{-te^{-t}\}=-\frac 1{(s+1)^2}. Direct use of the exponential and te−tte^{-t} integrals verifies both, for s>−1s>-1. Their difference is 1/(s+1)=F1/(s+1)=F.

Step 3: Differentiate the complete expression twice. Multiplication by t2t^2 corresponds to two parameter derivatives with positive sign. Thus ℒ{t2f″}=d2ds2[s2F−sf(0)−f′(0)]=2F+4sF′+s2F″.\mathcal L\{t^2f''\}=\frac{d^2}{ds^2}[s^2F-sf(0)-f'(0)] =\boxed{2F+4sF'+s^2F''.} The first derivative of s2Fs^2F is 2sF+s2F′2sF+s^2F'; differentiating again produces both product-rule contributions. The initial terms are at most linear in ss, so their second derivatives vanish.

Step 4: Diagnose and verify. The proposed s2F″s^2F'' omits 2F+4sF′2F+4sF'. For f=e−tf=e^{-t}, the correct result simplifies to 2s+1−4s(s+1)2+2s2(s+1)3=2(s+1)3.\frac 2{s+1}-\frac{4s}{(s+1)^2}+\frac{2s^2}{(s+1)^3} =\boxed{\frac 2{(s+1)^3}}. Since f″=e−tf''=e^{-t}, direct integration of t2e−(s+1)tt^2e^{-(s+1)t} gives this same value for s>−1s>-1. Differentiating only FF while treating its prefactors as constants is the source of the error.

Original worksheet page 2: question and worked solution for 4-2-010

Original worksheet layout. Use Enlarge or open the PDF for a closer view.