IVP’s With Step Functions — Question 8

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Question 8

Let Ha(t)=0H_a(t)=0 for t<at<a and Ha(t)=1H_a(t)=1 for t≥at\ge a. Use one-sided Laplace transforms. Solutions are continuous (and have continuous first derivative for second-order equations); satisfy the equation away from switches and use one-sided derivatives there. Isolated input values do not change the solution.

An initially unexcited system is driven by one unknown positive step: y′+2y=AHa(t),y(0)=0,A>0,a>0.y'+2y=A H_a(t),\qquad y(0)=0,\qquad A>0,\quad a>0. Exact measurements give y(1)=0y(1)=0, y(2)=1y(2)=1, and y(3)=2y(3)=2. A fourth proposed measurement is y(4)=3y(4)=3.

Tasks

  1. Derive the transformed and time-domain response for arbitrary A,aA,a.

  2. Use positivity and the measurements to locate the switch interval, then determine AA and aa exactly.

  3. Verify that the recovered parameters satisfy all three original measurements and are unique in this one-step family.

  4. Test the fourth measurement and find the limiting response. Explain the scope of the identification.

Original worksheet page 1: question and worked solution for 4-7-008
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Question 8 – Solution

Strategy. The zero measurement locates the delay. Once the input is on, equally spaced samples obey a simple exponential approach to the same level.

Step 1: Solve the parameterized IVP. For s>0s>0, Y=Ae−ass(s+2),y(t)=A2Ha(t)(1−e−2(t−a)).Y=\frac{Ae^{-as}}{s(s+2)},\qquad \boxed{y(t)=\frac A2H_a(t)(1-e^{-2(t-a)}).} The response is zero through aa, positive for t>at>a, and continuous at aa. Its derivative jumps by AA, as the equation requires.

Step 2: Locate and recover the switch. Since A>0A>0, the first two measurements imply 1≤a<21\le a<2. Put r=e−2r=e^{-2} and C=A/2C=A/2. On each full unit interval after activation, y(t+1)=ry(t)+C(1−r).y(t+1)=r\,y(t)+C(1-r). Thus 2=r+C(1−r)2=r+C(1-r), and A=2(2−r)1−r.\boxed{A=\frac{2(2-r)}{1-r}}. Using y(2)=1y(2)=1 gives e−2(2−a)=1−1/C=1/(2−r)e^{-2(2-a)}=1-1/C=1/(2-r), hence a=2−12ln⁡(2−e−2).\boxed{a=2-\tfrac 12\ln(2-e^{-2}).}

Step 3: Verify admissibility and uniqueness. Because 1<2−r<2<e21<2-r<2<e^2, one has 0<ln⁡(2−r)<20<\ln(2-r)<2, so 1<a<21<a<2. Also C=(2−r)/(1−r)>0C=(2-r)/(1-r)>0. The recovered values give y(1)=0y(1)=0 and y(2)=C(1−12−r)=1,y(3)=r+C(1−r)=2.y(2)=C\left(1-\frac 1{2-r}\right)=1,\qquad y(3)=r+C(1-r)=2. The sample recurrence fixes CC uniquely. Then the exponential expression for y(2)y(2) is strictly monotone in aa, fixing the delay uniquely. Direct substitution into the response verifies the IVP on both sides of the switch.

Step 4: Test the extra datum and interpret. The same recurrence predicts y(4)=2r+C(1−r)=2+e−2<3.\boxed{y(4)=2r+C(1-r)=2+e^{-2}<3.} The fourth datum is inconsistent with the stated model. The limiting level is C=(2−e−2)/(1−e−2)\boxed{C=(2-e^{-2})/(1-e^{-2})}, approached from below after activation. Its positive constant tail gives exact real transform domain s>0s>0. Uniqueness here concerns the specified single positive step with known system coefficient; finitely many samples do not identify an arbitrary forcing history.

Original worksheet page 2: question and worked solution for 4-7-008

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