Laplace Transforms — Question 3

PDF ↗

Question 3

Let u(t−a)u(t-a) denote the unit step at aa. Solve the delayed-ramp problem (D+2)3y=u(t−1)(t−1),(y,y′,y″)(0)=(0,0,0),t≥0.(D+2)^3y=u(t-1)(t-1),\qquad (y,y',y'')(0)=(0,0,0),\qquad t\geq 0. The value assigned to u(0)u(0) does not affect an ordinary Laplace transform.

Tasks

  1. Transform the initial-value problem, taking care to shift the entire ramp.

  2. Obtain a closed form for the response on each side of t=1t=1. Display a partial-fraction decomposition for the unshifted transform.

  3. Check the equation on the two open time intervals and determine exactly which derivative first jumps at t=1t=1. State the global smoothness of yy.

  4. Prove the response is positive after switching, find its large-time linear asymptote, and sketch it together with that asymptote on t≥1t\geq 1.

Original worksheet page 1: question and worked solution for 7-5-003
Show solutionHide solution

Question 3 – Solution

Strategy. Solve a zero-state ramp response, then translate time and check the switching jet.

Step 1: Transform the shifted input. All initial terms vanish. The second shifting theorem gives Y(s)=e−ss2(s+2)3,Re⁡s>0.Y(s)=\frac{e^{-s}}{s^2(s+2)^3},\qquad \operatorname{Re}s>0.

Step 2: Invert before translating. The unshifted fraction decomposes as 1s2(s+2)3=−316s+18s2+316(s+2)+14(s+2)2+14(s+2)3.\frac 1{s^2(s+2)^3}=-\frac 3{16s}+\frac 1{8s^2} +\frac 3{16(s+2)}+\frac 1{4(s+2)^2}+\frac 1{4(s+2)^3}. Thus, with r=t−1r=t-1, g(r)=r8−316+e−2r(316+r4+r28),y(t)={0,0≤t≤1,g(t−1),t>1.g(r)=\frac r8-\frac 3{16}+e^{-2r}\left(\frac 3{16}+\frac r4+\frac{r^2}{8}\right), \qquad \boxed{y(t)=\begin{cases}0,&0\leq t\leq 1,\\g(t-1),&t>1.\end{cases}}

Step 3: Verify forcing and regularity. The exponential term is annihilated by (D+2)3(D+2)^3; applying it to r/8−3/16r/8-3/16 gives rr. Also g(r)=r4/24+O(r5)g(r)=r^4/24+O(r^5) as r↓0r\downarrow 0. Consequently y,y′,y″,y‴y,y',y'',y''' match zero at switching, while y(4)(1+)−y(4)(1−)=1y^{(4)}(1+)-y^{(4)}(1-)=1. The solution is C3C^3 but not C4C^4; the original equation also holds at t=1t=1.

Step 4: Establish shape and asymptote. Convolution gives g(r)=∫0r(r−v)v2e−2v/2dv>0g(r)=\int_0^r (r-v)v^2e^{-2v}/2\,dv>0 for r>0r>0. The exponential correction tends to zero, so the asymptote is y=(t−1)/8−3/16y=(t-1)/8-3/16, approached from above. It is drawn only for t≥1t\geq 1.

See the diagram in the original worksheet below.

Original worksheet page 2: question and worked solution for 7-5-003

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