Modeling with First Order DE’s — Question 5

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Question 5

A series resistor-capacitor circuit has resistance R=1000ΩR=1000\ \Omega and capacitance C=0.001C=0.001 F. Its capacitor voltage is U(t)U(t), charge is q=CUq=CU, and current is I=q′I=q'. The source voltage E(t)E(t) obeys the loop relation E=RI+UE=RI+U. Initially the capacitor is uncharged. Time is in seconds.

A designer wants the exact voltage trajectory Ud(t)=6(1−e−t/2) V,t≥0,U_d(t)=6(1-e^{-t/2})\text{ V},\qquad t\ge 0, but the available source must satisfy 0≤E(t)≤50\le E(t)\le 5 V. Ideal circuit laws are assumed; capacitor energy is W=12CU2W=\tfrac 12 CU^2.

Tasks

  1. Derive a first-order IVP for the capacitor voltage and identify the time constant, with units.

  2. Find the unique source voltage and the current required to produce the desired trajectory exactly.

  3. Determine the longest interval starting at 00 on which this trajectory respects the source bound. Find the capacitor voltage at the limiting time.

  4. Calculate the stored energy at that time. Explain why simply fixing the source at 55 V afterward cannot continue the same prescribed trajectory.

Original worksheet page 1: question and worked solution for 2-7-005
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Question 5 – Solution

Strategy. Use the circuit balance backward: a specified capacitor trajectory determines its current and therefore the required source.

Step 1: Derive the voltage model. Since I=CU′I=CU', the loop equation gives RCU′+U=E(t),U(0)=0.RC\,U'+U=E(t),\qquad U(0)=0. Here RC=(1000)(0.001)=1RC=(1000)(0.001)=1 s is the time constant. With time numerically measured in seconds, the model is U′+U=EU'+U=E; the derivative coefficient carries the one-second time constant.

Step 2: Find the required input and current. The desired derivative is Ud′=3e−t/2U_d'=3e^{-t/2} V/s, so E(t)=6−3e−t/2 V,I(t)=0.003e−t/2 A.\boxed{E(t)=6-3e^{-t/2}\text{ V}},\qquad \boxed{I(t)=0.003e^{-t/2}\text{ A}}. Substitution gives RCUd′+Ud=ERC\,U_d'+U_d=E and Ud(0)=0U_d(0)=0. The prescribed UdU_d fixes its derivative, so the loop relation leaves no other possible source trajectory. In particular, the initial current is 33 mA and the required initial source is 33 V.

Step 3: Apply the source constraint. The required source increases strictly from 33 V toward 66 V. It first reaches 55 V when e−t/2=1/3e^{-t/2}=1/3. Therefore the full feasible initial interval is 0≤t≤t*=2ln⁡3≈2.197 s,Ud(t*)=4 V.\boxed{0\le t\le t_*=2\ln 3\approx 2.197\text{ s}},\qquad \boxed{U_d(t_*)=4\text{ V}}. Equality at the limiting time is allowed by the given source bound. Beyond it the unique required source exceeds 55 V.

Step 4: Compute energy and interpret saturation. At the limiting time, W=12(0.001)(4)2=0.008 J.\boxed{W=\tfrac 12(0.001)(4)^2=0.008\text{ J}}. A source fixed at 55 V afterward would instead produce U=5−e−(t−t*)U=5-e^{-(t-t_*)} V, starting from 44 V. It tends to 55 V, whereas the desired trajectory tends to 66 V. Thus the circuit can continue operating, but it cannot continue this exact target under the source constraint. The feasible interval is a hardware limitation, not a singularity of the ideal differential equation.

Original worksheet page 2: question and worked solution for 2-7-005

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