Dirac Delta Function — Question 8

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Question 8

Interpret the equation through ordinary motion away from the impulse and its jump conditions. For this question only, the initial-time transform convention is specified below; write [v]0=v(0+)−v(0−)[v]_0=v(0^+)-v(0^-) for a jump.

Use a full-mass initial impulse convention: the transform starts at 0−0^-, ℒ{δ(t)}=1\mathcal L\{\delta(t)\}=1, and ℒ{y′}=sY−y(0−),ℒ{y″}=s2Y−sy(0−)−y′(0−).\mathcal L\{y'\}=sY-y(0^-),\qquad \mathcal L\{y''\}=s^2Y-sy(0^-)-y'(0^-). Consider 2y″+4y′+2y=Jδ(t),y(0−)=1,y′(0−)=2.2y''+4y'+2y=J\delta(t),\qquad y(0^-)=1,\quad y'(0^-)=2. These are pre-impact data, not post-impact data.

Tasks

  1. Find y(0+)y(0^+) and y′(0+)y'(0^+) by the impulse jump conditions.

  2. Use the stated 0−0^- convention to find Y(s)Y(s) and the response for t≥0t\ge 0.

  3. Reproduce the same response by solving a regular homogeneous IVP from 0+0^+. Explain why keeping the impulse again would double-count it.

  4. Classify every JJ for which the post-impact response is nonnegative and nonincreasing for all t≥0t\ge 0. Describe the boundary cases.

Original worksheet page 1: question and worked solution for 4-8-008
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Question 8 – Solution

Strategy. An impulse at the initial time requires a declared convention. Either transform pre-impact data with the impulse or restart after the jump.

Step 1: Compute the post-impact data. There is no displacement jump under an ordinary force impulse. Integrating the equation across the origin gives 2[y′]0=J2[y']_0=J; the damping contribution is 4[y]0=04[y]_0=0. Thus y(0+)=1,y′(0+)=2+J2.\boxed{y(0^+)=1,\qquad y'(0^+)=2+\frac J2.} The factor 22 is the mass and must not be omitted.

Step 2: Transform the pre-impact formulation. The stipulated derivative rules give 2(s2Y−s−2)+4(sY−1)+2Y=J,2(s^2Y-s-2)+4(sY-1)+2Y=J, so Y=2s+8+J2(s+1)2=1s+1+3+J/2(s+1)2.Y=\frac{2s+8+J}{2(s+1)^2} =\frac 1{s+1}+\frac{3+J/2}{(s+1)^2}. Writing c=3+J/2c=3+J/2, the inverse is y(t)=e−t(1+ct),t≥0\boxed{y(t)=e^{-t}(1+ct),\quad t\ge 0}. It has y(0+)=1y(0^+)=1 and y′(0+)=c−1=2+J/2y'(0^+)=c-1=2+J/2, exactly as the jump calculation.

Step 3: Check the equivalent restart. For t>0t>0 the equation is y″+2y′+y=0y''+2y'+y=0. Using the post-impact data 1,2+J/21,2+J/2 gives the critical solution e−t[1+(3+J/2)t]e^{-t}[1+(3+J/2)t] again. This restart has no remaining initial impulse: its effect is already encoded in the velocity. Inserting Jδ(t)J\delta(t) again with those data would add a second velocity change J/2J/2.

Step 4: Classify positivity and monotonicity. Since the exponential is positive, nonnegativity for every t≥0t\ge 0 requires and is ensured by c≥0c\ge 0. Also y′=e−t(c−1−ct).y'=e^{-t}(c-1-ct). For c≥0c\ge 0, this is nonpositive for all t≥0t\ge 0 exactly when c≤1c\le 1. Therefore 0≤c≤1⇔−6≤J≤−4.\boxed{0\le c\le 1\quad\Longleftrightarrow\quad -6\le J\le-4.} At J=−6J=-6, y=e−ty=e^{-t}; at J=−4J=-4, y=(1+t)e−ty=(1+t)e^{-t} starts horizontal and then decreases strictly. For J<−6J<-6 the response eventually becomes negative, and for J>−4J>-4 it initially increases. All these nonzero polynomial-exponential responses have exact real transform domain s>−1s>-1.

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