Table Of Laplace Transforms — Question 4

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Question 4

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.

An unknown function has transform F(s)=As+Bs2+4,s>0,F(s)=\frac{As+B}{s^2+4},\qquad s>0, where A,BA,B are real. Measurements give f(0)=1f(0)=1 and f′(0)=−2f'(0)=-2.

Tasks

  1. Invert the general transform by matching numerators to table entries, then recover A,BA,B from the data.

  2. For the recovered function, find its amplitude, all positive zeros, and the conserved quantity f′(t)2+4f(t)2f'(t)^2+4f(t)^2.

  3. Classify all real pairs (A,B)(A,B) for which the inverse is nonnegative for every t≥0t\ge 0. Prove the classification.

  4. A student argues that lim⁡s→0+sF(s)=0\lim_{s\to 0^+}sF(s)=0 proves lim⁡t→∞f(t)=0\lim_{t\to\infty}f(t)=0. Refute the conclusion with two sequences of times and identify the missing hypothesis in that use of the final-value theorem.

Original worksheet page 1: question and worked solution for 4-10-004
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Question 4 – Solution

Strategy. Matching a denominator is insufficient: the numerator determines the phase, initial state and sign changes.

Step 1: Match and use the data. The table gives f=Acos⁡2t+(B/2)sin⁡2tf=A\cos 2t+(B/2)\sin 2t, so f(0)=Af(0)=A and f′(0)=Bf'(0)=B. Therefore A=1A=1, B=−2B=-2 and f(t)=cos⁡2t−sin⁡2t=2cos⁡(2t+π/4).\boxed{f(t)=\cos 2t-\sin 2t=\sqrt 2\cos(2t+\pi/4).}

Step 2: Determine the motion. The amplitude is 2\sqrt 2. The positive zeros are t=π/8+kπ/2t=\pi/8+k\pi/2, k=0,1,2,…k=0,1,2,\ldots. Direct differentiation gives f″+4f=0f''+4f=0, so (f′2+4f2)′=2f′(f″+4f)=0(f'^2+4f^2)'=2f'(f''+4f)=0. Its initial value is (−2)2+4(1)2=8(-2)^2+4(1)^2=\boxed{8}.

Step 3: Prove the positivity classification. If (A,B)≠(0,0)(A,B)\ne(0,0), the amplitude A2+B2/4\sqrt{A^2+B^2/4} is positive. The sinusoid attains both that amplitude and its negative at arbitrarily large nonnegative times. It cannot be nonnegative on the whole half-line. Only A=B=0\boxed{A=B=0} works. An alternative proof uses zero integral over one period: a continuous nonnegative function with zero integral must vanish.

Step 4: Check the claimed final value. Although sF(s)→0sF(s)\to 0 as s→0+s\to 0^+, the selected solution obeys f(nπ)=1f(n\pi)=1 and f(nπ+π/2)=−1f(n\pi+\pi/2)=-1. Hence it has no time limit. The usual rational final-value theorem requires the poles of sF(s)sF(s) to lie strictly in the left half-plane after cancellation. Here the uncanceled poles are s=±2is=\pm 2i, supporting persistent oscillations. An algebraic limit of the transform does not by itself establish a limit of the function.

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