Differential-Equations Β· Unit 7 Β· Video 1 Β· Interactive Practice

Steady-State and Transient Solutions of y' + ky = q(t)

IKey Formulas

FormulaNameWhat it says
yβ€²+ky=q(t)y' + ky = q(t), often yβ€²+ky=k qe(t)y' + ky = k\,q_e(t)Constant-coefficient linear equationTemperature Tβ€²+kT=kTe(t)T' + kT = kT_e(t), concentration and mixing take the second form; the RC circuit and radioactive decay do not
y=eβˆ’kt∫q(t) ekt dt+c eβˆ’kty = e^{-kt}\displaystyle\int q(t)\,e^{kt}\,dt + c\,e^{-kt}General solutionIntegrating factor ekte^{kt}; for q=1q = 1 the exponentials cancel and leave 1k+c eβˆ’kt\tfrac{1}{k} + c\,e^{-kt}
y=eβˆ’kt∫0tq(u) eku du⏟steadyΒ state+y0 eβˆ’kt⏟transienty = \underbrace{e^{-kt}\displaystyle\int_0^t q(u)\,e^{ku}\,du}_{\text{steady state}} + \underbrace{y_0\,e^{-kt}}_{\text{transient}}Initial-value solutionFor k>0k > 0 the transient carries y0y_0 and tends to 00; the steady state does not involve y0y_0
y1βˆ’y2=(c1βˆ’c2) eβˆ’ktβ†’0y_1 - y_2 = (c_1 - c_2)\,e^{-kt} \to 0Any two solutions (k>0k > 0)Every solution approaches every other, so the steady-state solution is not unique

Key Insight: Any solution could serve as the steady state. The one called the steady-state solution is the simplest, usually the one from integrating with no arbitrary constant, and the terminology only makes sense when k>0k > 0.

IISteady State Plus Transient

For k>0k > 0, every solution is the steady state S(t)S(t) plus a transient c eβˆ’ktc\,e^{-kt} that decays to zero.

IIIAny Solution Can Be the Steady State

In the bath equation yβ€²+0.5y=10y' + 0.5y = 10, every solution is approached by all the others.

IVWhy kk Must Be Positive

Steady state and transient are meaningful only when eβˆ’kte^{-kt} decays, that is, when k>0k > 0.

VQuiz Questions

Problem 1 Β· Split a Solution

Given: yβ€²+3y=6y' + 3y = 6 with y(0)=5y(0) = 5 β€” find the simplest steady-state solution and the transient that goes with it.

What is the steady-state solution?

What is the transient?

βœ… Correct! y=2+3eβˆ’3ty = 2 + 3e^{-3t}: the constant 2=6/32 = 6/3 ignores y0y_0, and 3eβˆ’3t3e^{-3t} carries the initial offset 5βˆ’25 - 2 and dies away.
❌ Close, but… 66 is qq, not the solution. A constant right-hand side qq produces the constant q/kq/k.
❌ Not quite. 55 is the initial value, and the steady state is exactly the part that does not involve y0y_0.
❌ Check the steady state. Try a constant y=Ay = A: then 3A=63A = 6.
❌ Close, but… 5eβˆ’3t5e^{-3t} is the transient that pairs with the definite-integral steady state 2(1βˆ’eβˆ’3t)2(1 - e^{-3t}), not with 22.
❌ Check the transient. It has the form c eβˆ’3tc\,e^{-3t}, and cc is fixed by y(0)=2+c=5y(0) = 2 + c = 5.
Show solution

With the integrating factor e3te^{3t} and no arbitrary constant in the integral:

y=eβˆ’3t∫6e3t dt+c eβˆ’3t=eβˆ’3tβ‹…2e3t+c eβˆ’3t=2+c eβˆ’3t.y = e^{-3t}\int 6e^{3t}\,dt + c\,e^{-3t} = e^{-3t}\cdot 2e^{3t} + c\,e^{-3t} = 2 + c\,e^{-3t}.

The condition y(0)=5y(0) = 5 gives 2+c=52 + c = 5, so c=3c = 3 and

y=2⏟steadyΒ state+3eβˆ’3t⏟transient.y = \underbrace{2}_{\text{steady state}} + \underbrace{3e^{-3t}}_{\text{transient}}.

Check: yβ€²+3y=βˆ’9eβˆ’3t+6+9eβˆ’3t=6y' + 3y = -9e^{-3t} + 6 + 9e^{-3t} = 6. The definite form splits the same function differently, 2(1βˆ’eβˆ’3t)+5eβˆ’3t2(1 - e^{-3t}) + 5e^{-3t}; the constant 22 is the simpler steady state.

Problem 2 Β· Which Steady State?

Given: the bath equation yβ€²+ky=20ky' + ky = 20k with k>0k > 0. The definite integral from 00 to tt gives 20(1βˆ’eβˆ’kt)20(1 - e^{-kt}), and the indefinite integral with no constant gives 2020 β€” which of these are steady-state solutions?

βœ… Correct! Any two solutions differ by a transient, so every solution has the property that all others approach it; 2020 is the simplest choice.
❌ Not quite. The lower limit 00 is a choice, not a law. Any solution that all others approach qualifies, and 20βˆ’20(1βˆ’eβˆ’kt)=20eβˆ’ktβ†’020 - 20(1 - e^{-kt}) = 20e^{-kt} \to 0.
❌ Not quite. Steady states need not be constant; in general they follow q(t)q(t). Here 20(1βˆ’eβˆ’kt)20(1 - e^{-kt}) also qualifies, since the two differ by a decaying 20eβˆ’kt20e^{-kt}.
❌ Roles reversed. The transient carries y0y_0; the steady state does not involve the initial value at all.
Show solution

Definite integral from 00 to tt:

eβˆ’kt∫0t20k eku du=eβˆ’ktβ‹…20(ektβˆ’1)=20(1βˆ’eβˆ’kt).e^{-kt}\int_0^t 20k\,e^{ku}\,du = e^{-kt}\cdot 20\left(e^{kt} - 1\right) = 20\left(1 - e^{-kt}\right).

Indefinite integral with no arbitrary constant:

eβˆ’kt∫20k ekt dt=eβˆ’ktβ‹…20ekt=20.e^{-kt}\int 20k\,e^{kt}\,dt = e^{-kt}\cdot 20e^{kt} = 20.

Both satisfy yβ€²+ky=20ky' + ky = 20k, and their difference is

20βˆ’20(1βˆ’eβˆ’kt)=20eβˆ’ktβ†’0(k>0),20 - 20\left(1 - e^{-kt}\right) = 20e^{-kt} \to 0 \quad (k > 0),

a transient. Every solution approaches both, so both are steady-state solutions; the one usually meant is the simplest, y=20y = 20.

Problem 3 Β· Starting at 127

Given: yβ€²+0.5y=10y' + 0.5y = 10 (a bath held at 2020, k=0.5k = 0.5). One solution starts at y(0)=127y(0) = 127, another at y(0)=20y(0) = 20 β€” when are they exactly 11 apart?

βœ… Correct! The gap is the transient difference 107eβˆ’0.5t107e^{-0.5t}, and it falls to 11 at t=2ln⁑107t = 2\ln 107.
❌ Close, but… The gap between the two solutions is (127βˆ’20)eβˆ’0.5t(127 - 20)e^{-0.5t}: the shared steady state 2020 cancels.
❌ Check the last step. From 0.5t=ln⁑1070.5t = \ln 107 you divide by 0.50.5, which doubles ln⁑107\ln 107.
❌ Not quite. The exponent is βˆ’0.5t-0.5t, not βˆ’t-t; the factor k=0.5k = 0.5 cannot be dropped.
Show solution

Every solution is y=20+c eβˆ’0.5ty = 20 + c\,e^{-0.5t} with c=y(0)βˆ’20c = y(0) - 20:

y1=20+107eβˆ’0.5t,y2=20.y_1 = 20 + 107e^{-0.5t}, \qquad y_2 = 20.

Their difference is a transient: y1βˆ’y2=107eβˆ’0.5ty_1 - y_2 = 107e^{-0.5t}. Setting it equal to 11:

eβˆ’0.5t=1107β€…β€Šβ‡’β€…β€Š0.5t=ln⁑107β€…β€Šβ‡’β€…β€Št=2ln⁑107β‰ˆ9.35.e^{-0.5t} = \frac{1}{107} \;\Rightarrow\; 0.5t = \ln 107 \;\Rightarrow\; t = 2\ln 107 \approx 9.35.

The solution that starts at 127127 comes down and stays above 2020, closing in on it as tβ†’βˆžt \to \infty.

Problem 4 Β· When k Is Negative

Given: yβ€²βˆ’0.2y=3sin⁑ty' - 0.2y = 3\sin t. Two solutions start 11 apart at t=0t = 0 β€” how far apart are they at t=10t = 10, and does a steady state make sense?

βœ… Correct! Here k=βˆ’0.2k = -0.2, so the difference (c1βˆ’c2)e0.2t(c_1 - c_2)e^{0.2t} grows: e2e^{2} at t=10t = 10.
❌ Watch the sign of kk. Matching yβ€²+kyy' + ky with yβ€²βˆ’0.2yy' - 0.2y gives k=βˆ’0.2k = -0.2, so eβˆ’kt=e0.2te^{-kt} = e^{0.2t} grows.
❌ Not quite. The difference is (c1βˆ’c2)eβˆ’kt(c_1 - c_2)e^{-kt}, which stays constant only when k=0k = 0.
❌ Check the exponent. e0.2e^{0.2} is the factor at t=1t = 1; at t=10t = 10 the exponent is 0.2β‹…10=20.2 \cdot 10 = 2.
Show solution

In the form yβ€²+ky=q(t)y' + ky = q(t) this equation has k=βˆ’0.2k = -0.2 and q(t)=3sin⁑tq(t) = 3\sin t. Any two solutions share the first term and differ only in their constants:

y1βˆ’y2=(c1βˆ’c2) eβˆ’kt=(c1βˆ’c2) e0.2t.y_1 - y_2 = (c_1 - c_2)\,e^{-kt} = (c_1 - c_2)\,e^{0.2t}.

At t=0t = 0 the difference is c1βˆ’c2=1c_1 - c_2 = 1, so at t=10t = 10 it is

e0.2β‹…10=e2β‰ˆ7.39.e^{0.2 \cdot 10} = e^{2} \approx 7.39.

The term carrying the initial value grows instead of dying away, the solutions fan apart, and the words steady state and transient are inappropriate.

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