Differential-Equations Β· Unit 9 Β· Video 4 Β· Interactive Practice

Equal Roots and the Missing Solution: Reduction of Order Finds t eβˆ’att\,e^{-at}

IKey Formulas

FormulaNameWhere it comes from
(r+a)2=r2+2ar+a2=0(r + a)^2 = r^2 + 2ar + a^2 = 0Double root r=βˆ’ar = -a, a>0a > 0yβ€²β€²+2a yβ€²+a2y=0y'' + 2a\,y' + a^2 y = 0: A=2aA = 2a, B=a2B = a^2, so A=2BA = 2\sqrt{B}
y=y1 uy = y_1\,uReduction of orderOne known solution y1y_1 of yβ€²β€²+p yβ€²+q y=0y'' + p\,y' + q\,y = 0; pp, qq may depend on tt
eβˆ’atuβ€²β€²=0β€…β€Šβ‡’β€…β€Šu=c1t+c2e^{-at}u'' = 0 \;\Rightarrow\; u = c_1 t + c_2Condition on uuSubstitute y=eβˆ’atuy = e^{-at}u; the uu and uβ€²u' columns cancel
y=(c1+c2t) eβˆ’aty = (c_1 + c_2 t)\,e^{-at}Critically damped general solutiony1=eβˆ’aty_1 = e^{-at}, y2=t eβˆ’aty_2 = t\,e^{-at}, independent since y2/y1=ty_2/y_1 = t

Key Insight: A double root gives the exponential trial only one function, eβˆ’ate^{-at}. Writing y=eβˆ’atuy = e^{-at}u turns the equation into uβ€²β€²=0u'' = 0, and the simplest non-constant choice u=tu = t supplies the factor of tt no exponential could produce.

IIVisualization 1 β€” The Case Between Over- and Underdamping

For yβ€²β€²+Ayβ€²+y=0y'' + Ay' + y = 0, so B=1B = 1, only A=2B=2A = 2\sqrt{B} = 2 merges the two roots into a double root.

IIIVisualization 2 β€” Which uu Makes eβˆ’atue^{-at}u a Solution?

Substituting y=eβˆ’atuy = e^{-at}u leaves only eβˆ’atuβ€²β€²e^{-at}u'', so uu works exactly when uβ€²β€²=0u'' = 0.

multiply byuu columnuβ€²u' columnuβ€²β€²u'' column
a2a^2y=y =eβˆ’atue^{-at}u
2a2ayβ€²=y' =βˆ’a eβˆ’atu-a\,e^{-at}u+ eβˆ’atuβ€²+\,e^{-at}u'
11yβ€²β€²=y'' =a2eβˆ’atua^2 e^{-at}uβˆ’2a eβˆ’atuβ€²-2a\,e^{-at}u'+ eβˆ’atuβ€²β€²+\,e^{-at}u''
sumyβ€²β€²+2a yβ€²+a2y=y'' + 2a\,y' + a^2 y =(a2βˆ’2a2+a2) eβˆ’atu=0(a^2 - 2a^2 + a^2)\,e^{-at}u = 0(2aβˆ’2a) eβˆ’atuβ€²=0(2a - 2a)\,e^{-at}u' = 0eβˆ’atuβ€²β€²e^{-at}u''

IVVisualization 3 β€” Two Constants Match Any Start

For yβ€²β€²+2yβ€²+y=0y'' + 2y' + y = 0, one constant times eβˆ’te^{-t} fixes yβ€²(0)=βˆ’y(0)y'(0) = -y(0); adding t eβˆ’tt\,e^{-t} frees the slope.

VQuiz Questions

Problem 1 Β· The Critical Damping Value

Given: yβ€²β€²+Ayβ€²+16y=0y'' + Ay' + 16y = 0 with A>0A > 0. Find the value of AA that makes the system critically damped, and the resulting double root.

What is A?

What is the double root?

βœ… Correct! A=216=8A = 2\sqrt{16} = 8, and r2+8r+16=(r+4)2r^2 + 8r + 16 = (r + 4)^2 has the double root r=βˆ’4r = -4, so a=4a = 4.
❌ That is B\sqrt{B}, which is aa. The damping coefficient is A=2a=2BA = 2a = 2\sqrt{B}.
❌ That is 2B2B. Matching (r+a)2=r2+2ar+a2(r + a)^2 = r^2 + 2ar + a^2 gives B=a2B = a^2, so a=Ba = \sqrt{B}, not BB.
❌ That is A2A^2, not AA. A double root needs A2βˆ’4B=0A^2 - 4B = 0, so A2=64A^2 = 64 and A=8A = 8.
❌ Check AA. A double root means the discriminant A2βˆ’4BA^2 - 4B is zero.
❌ Check the sign. (r+4)2=0(r + 4)^2 = 0 at r=βˆ’4r = -4; with damping present the root is negative.
❌ That is βˆ’A-A. The double root of r2+Ar+Br^2 + Ar + B is βˆ’A/2-A/2.
❌ Check the root. Factor r2+8r+16r^2 + 8r + 16 as a perfect square.
Show solution

The characteristic equation is r2+Ar+16=0r^2 + Ar + 16 = 0. It has a double root when the discriminant vanishes:

A2βˆ’4β‹…16=0β€…β€Šβ‡’β€…β€ŠA2=64β€…β€Šβ‡’β€…β€ŠA=8(A>0).A^2 - 4 \cdot 16 = 0 \;\Rightarrow\; A^2 = 64 \;\Rightarrow\; A = 8 \quad (A > 0).

Equivalently, A=2B=216=8A = 2\sqrt{B} = 2\sqrt{16} = 8. Then

r2+8r+16=(r+4)2=0β€…β€Šβ‡’β€…β€Šr=βˆ’4Β (double),r^2 + 8r + 16 = (r + 4)^2 = 0 \;\Rightarrow\; r = -4 \text{ (double)},

so a=4a = 4 and the general solution is y=(c1+c2t) eβˆ’4ty = (c_1 + c_2 t)\,e^{-4t}.

Problem 2 Β· The Same Exponential Twice

Given: yβ€²β€²+4yβ€²+4y=0y'' + 4y' + 4y = 0 with y(0)=1y(0) = 1, yβ€²(0)=0y'(0) = 0. A student tries y=c1eβˆ’2t+c2eβˆ’2ty = c_1 e^{-2t} + c_2 e^{-2t}. Which statement is true?

βœ… Correct! y=(c1+c2)eβˆ’2ty = (c_1 + c_2)e^{-2t} has one effective constant; y(0)=1y(0) = 1 forces yβ€²(0)=βˆ’2(c1+c2)=βˆ’2β‰ 0y'(0) = -2(c_1 + c_2) = -2 \neq 0.
❌ That pair gets y(0)=1y(0) = 1 but not the slope. Any pair with c1+c2=1c_1 + c_2 = 1 gives y=eβˆ’2ty = e^{-2t}, whose slope at 00 is βˆ’2-2, not 00.
❌ c1+c2=1c_1 + c_2 = 1 handles only y(0)y(0). All those pairs give the same function eβˆ’2te^{-2t}, and its slope at 00 is βˆ’2-2, so yβ€²(0)=0y'(0) = 0 still fails.
❌ Not quite. Factor out eβˆ’2te^{-2t} and count the free constants.
Show solution

The characteristic equation r2+4r+4=(r+2)2=0r^2 + 4r + 4 = (r + 2)^2 = 0 has the double root r=βˆ’2r = -2. The student's combination collapses:

y=c1eβˆ’2t+c2eβˆ’2t=(c1+c2) eβˆ’2t=Ceβˆ’2t.y = c_1 e^{-2t} + c_2 e^{-2t} = (c_1 + c_2)\,e^{-2t} = C e^{-2t}.

Then y(0)=C=1y(0) = C = 1, and yβ€²(t)=βˆ’2Ceβˆ’2ty'(t) = -2C e^{-2t} gives yβ€²(0)=βˆ’2C=βˆ’2β‰ 0y'(0) = -2C = -2 \neq 0.

One free constant cannot meet two conditions. The fix is the second solution t eβˆ’2tt\,e^{-2t}: y=(1+2t) eβˆ’2ty = (1 + 2t)\,e^{-2t} has y(0)=1y(0) = 1 and yβ€²(0)=2βˆ’2=0y'(0) = 2 - 2 = 0.

Problem 3 Β· Solving a Critically Damped Initial Value Problem

Given: yβ€²β€²+6yβ€²+9y=0y'' + 6y' + 9y = 0, y(0)=2y(0) = 2, yβ€²(0)=βˆ’1y'(0) = -1. Find y(t)y(t).

βœ… Correct! c1=y(0)=2c_1 = y(0) = 2 and yβ€²(0)=c2βˆ’3c1=βˆ’1y'(0) = c_2 - 3c_1 = -1 give c2=5c_2 = 5.
❌ c2c_2 is not yβ€²(0)y'(0). Differentiating (c1+c2t)eβˆ’3t(c_1 + c_2 t)e^{-3t} also hits the exponential: yβ€²(0)=c2βˆ’3c1y'(0) = c_2 - 3c_1.
❌ The constants are in the wrong slots. At t=0t = 0 the factor is c1+c2β‹…0c_1 + c_2 \cdot 0, so c1=y(0)=2c_1 = y(0) = 2.
❌ Check the sign of the exponential's derivative. ddteβˆ’3t=βˆ’3eβˆ’3t\frac{d}{dt}e^{-3t} = -3e^{-3t}, so yβ€²(0)=c2βˆ’3c1y'(0) = c_2 - 3c_1, not c2+3c1c_2 + 3c_1.
❌ Not quite. Use y(0)y(0) for c1c_1, then the product rule for yβ€²(0)y'(0).
Show solution

r2+6r+9=(r+3)2=0r^2 + 6r + 9 = (r + 3)^2 = 0 gives the double root r=βˆ’3r = -3, so

y=(c1+c2t) eβˆ’3t,yβ€²=c2eβˆ’3tβˆ’3(c1+c2t) eβˆ’3t.y = (c_1 + c_2 t)\,e^{-3t}, \qquad y' = c_2 e^{-3t} - 3(c_1 + c_2 t)\,e^{-3t}.

At t=0t = 0:

y(0)=c1=2,yβ€²(0)=c2βˆ’3c1=c2βˆ’6=βˆ’1β€…β€Šβ‡’β€…β€Šc2=5.y(0) = c_1 = 2, \qquad y'(0) = c_2 - 3c_1 = c_2 - 6 = -1 \;\Rightarrow\; c_2 = 5. y=(2+5t) eβˆ’3t.y = (2 + 5t)\,e^{-3t}.

Check: yβ€²(0)=5βˆ’3β‹…2=βˆ’1y'(0) = 5 - 3 \cdot 2 = -1 βœ“.

Problem 4 Β· Reduction of Order with Variable Coefficients

Given: For t>0t > 0, y1=t2y_1 = t^2 solves t2yβ€²β€²βˆ’3t yβ€²+4y=0t^2 y'' - 3t\,y' + 4y = 0. Substitute y=t2uy = t^2 u. Find the condition on uu and a second solution y2y_2.

What equation must u satisfy?

Which is a second solution?

βœ… Correct! The uu column cancels, leaving t4uβ€²β€²+t3uβ€²=0t^4u'' + t^3u' = 0, so (t uβ€²)β€²=0(t\,u')' = 0, u=c1ln⁑t+c2u = c_1 \ln t + c_2, and y2=t2ln⁑ty_2 = t^2\ln t.
❌ That was the constant-coefficient case. Here the uβ€²u' column does not cancel: it leaves 4t3uβ€²βˆ’3t3uβ€²=t3uβ€²4t^3u' - 3t^3u' = t^3u'.
❌ Check the condition on uu. Write yy, yβ€²y', yβ€²β€²y'' in uu, uβ€²u', uβ€²β€²u'' columns, multiply by 44, βˆ’3t-3t, t2t^2, and add each column.
❌ Multiplying by tt was special to eβˆ’ate^{-at}. Test it: t2(6t)βˆ’3t(3t2)+4t3=t3β‰ 0t^2(6t) - 3t(3t^2) + 4t^3 = t^3 \neq 0.
❌ That is uu, not yy. The second solution is y2=y1u=t2ln⁑ty_2 = y_1 u = t^2\ln t.
❌ Check y2y_2. Solve the equation for uu, then multiply by y1=t2y_1 = t^2.
Show solution

With y=t2uy = t^2 u, arrange the derivatives in columns and multiply each row by its coefficient:

4β€…β€Š]y=t2uβˆ’3tβ€…β€Š]yβ€²=2t u+t2uβ€²t2β€…β€Š]yβ€²β€²=2u+4t uβ€²+t2uβ€²β€²\begin{aligned} 4 \;]\quad y &= t^2 u \\ -3t \;]\quad y' &= 2t\,u + t^2 u' \\ t^2 \;]\quad y'' &= 2u + 4t\,u' + t^2 u'' \end{aligned}

Column sums: uu: 4t2βˆ’6t2+2t2=04t^2 - 6t^2 + 2t^2 = 0; uβ€²u': βˆ’3t3+4t3=t3-3t^3 + 4t^3 = t^3; uβ€²β€²u'': t4t^4. So

t4uβ€²β€²+t3uβ€²=0β€…β€Šβ‡’β€…β€Št uβ€²β€²+uβ€²=0β€…β€Šβ‡’β€…β€Š(t uβ€²)β€²=0.t^4 u'' + t^3 u' = 0 \;\Rightarrow\; t\,u'' + u' = 0 \;\Rightarrow\; (t\,u')' = 0.

Hence t uβ€²=c1t\,u' = c_1, uβ€²=c1/tu' = c_1/t, and u=c1ln⁑t+c2u = c_1 \ln t + c_2. The simplest non-constant choice u=ln⁑tu = \ln t gives

y2=t2ln⁑t,y2y1=ln⁑t (not constant).y_2 = t^2 \ln t, \qquad \frac{y_2}{y_1} = \ln t \text{ (not constant)}.

As the video promised, reduction of order works even when the coefficients depend on tt.

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