Laplace Transforms — Question 8

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Question 8

A stable third-order filter receives identical unit impulses at times T,2T,3T,…T,2T,3T,\ldots, where T>0T>0: (D+1)3y=∑n=1∞δ(t−nT).(D+1)^3y=\sum_{n=1}^\infty\delta(t-nT). Assume zero prehistory and zero initial state. Interpret the equation in the sense of distributions; there is no impulse at t=0t=0.

Tasks

  1. Find Y(s)Y(s), stating a convergence half-plane. Give the exact finite-sum response at any finite time.

  2. For t=NT+xt=NT+x with 0≤x<T0\leq x<T, find the limiting periodic profile as N→∞N\to\infty. Sum it explicitly using q=e−Tq=e^{-T}.

  3. Determine the continuity and derivative jumps across each impulse, including the join in the limiting profile. Compute the mean of the limiting profile over a period.

  4. Decide whether y(t)y(t) has a pointwise limit as t→∞t\to\infty. Explain the failure or validity of a final-value argument, and sketch the transient and limiting profile for T=2T=2.

Original worksheet page 1: question and worked solution for 7-5-008
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Question 8 – Solution

Strategy. Sum delayed impulse kernels and distinguish a periodic limiting profile from a constant final value.

Step 1: Sum the transformed impulses. For Re⁡s>0\operatorname{Re}s>0, Y=e−sT(1−e−sT)(s+1)3,y(t)=∑1≤n≤⌊t/T⌋h(t−nT),h(v)=12v2e−v.Y=\frac{e^{-sT}}{(1-e^{-sT})(s+1)^3},\qquad y(t)=\sum_{1\leq n\leq\lfloor t/T\rfloor}h(t-nT),\quad h(v)=\tfrac 12v^2e^{-v}. The sum is empty before TT; including the current impulse adds h(0)=0h(0)=0.

Step 2: Sum the limiting profile. At t=NT+xt=NT+x the sum is ∑k=0N−1h(x+kT)\sum_{k=0}^{N-1}h(x+kT). Geometric-series identities give p(x)=e−x2[x21−q+2xTq(1−q)2+T2q(1+q)(1−q)3],q=e−T.\boxed{p(x)=\frac{e^{-x}}2\left[\frac{x^2}{1-q} +\frac{2xTq}{(1-q)^2}+\frac{T^2q(1+q)}{(1-q)^3}\right],\quad q=e^{-T}.} The omitted tail is uniformly O(N2qN)O(N^2q^N) for 0≤x≤T0\leq x\leq T and fixed TT, so y(NT+x)→p(x)y(NT+x)\to p(x) uniformly on a period.

Step 3: Check joins and mean. Since (h,h′,h″)(0)=(0,0,1)(h,h',h'')(0)=(0,0,1), y,y′y,y' are continuous and y″y'' jumps upward by one. Reindexing the convergent profile series gives the same periodic joins: p(0)=p(T−)p(0)=p(T-), p′(0)=p′(T−)p'(0)=p'(T-), p″(0)−p″(T−)=1p''(0)-p''(T-)=1. Also ∫0Tp(x)dx=∫0∞h(v)dv=1\int_0^T p(x)\,dx=\int_0^\infty h(v)\,dv=1, so its mean is 1/T1/T.

Step 4: Reject a constant final value. The profile is nonconstant: on each open gap (D+1)3p=0(D+1)^3p=0, so a constant profile would be zero, contradicting its integral. Distinct phases therefore have distinct subsequential limits. Poles at s=2πik/Ts=2\pi i k/T, k≠0k\ne 0, remain in sYsY; the formal limit lim⁡s→0sY=1/T\lim_{s\to 0}sY=1/T is a mean, not a final value.

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