Differential-Equations Β· Unit 12 Β· Video 2 Β· Interactive Practice

Particular Plus Complementary: The Form of Every Solution

IKey Formulas

FormulaNameWhat it says
y=yp+yc=yp+c1y1+c2y2y = y_p + y_c = y_p + c_1y_1 + c_2y_2General solution of L y=fL\,y = fypy_p is any one solution of the full equation; ycy_c solves L y=0L\,y = 0
L(yp+c1y1+c2y2)=L(yp)+L(c1y1+c2y2)=f+0L(y_p + c_1y_1 + c_2y_2) = L(y_p) + L(c_1y_1 + c_2y_2) = f + 0Claim 1 (linearity)Every member of the family is a solution
L(uβˆ’yp)=L(u)βˆ’L(yp)=fβˆ’f=0L(u - y_p) = L(u) - L(y_p) = f - f = 0Claim 2 (linearity)Any solution uu differs from ypy_p by a solution of L y=0L\,y = 0
y=eβˆ’kt∫0tf(t~) ekt~ dt~+c eβˆ’kty = e^{-kt}\displaystyle\int_0^t f(\tilde t)\,e^{k\tilde t}\,d\tilde t + c\,e^{-kt}First-order case yβ€²+ky=f(t)y' + ky = f(t)ypy_p plus yc=c eβˆ’kty_c = c\,e^{-kt}; for k>0k > 0, steady state plus transient

Key Insight: "Particular" means any one. Two different particular solutions differ by a solution of the homogeneous equation, so either one, plus ycy_c, gives the same family.

IIVisualization 1 β€” Every Member of the Family Solves the Equation

For yβ€²β€²+y=3sin⁑2xy'' + y = 3\sin 2x, each choice of particular solution and constants still has yβ€²β€²+y=3sin⁑2xy'' + y = 3\sin 2x.

IIIVisualization 2 β€” Any Solution Minus ypy_p

Any solution uu of yβ€²β€²+y=3sin⁑2xy'' + y = 3\sin 2x minus yp=βˆ’sin⁑2xy_p = -\sin 2x is a solution of yβ€²β€²+y=0y'' + y = 0.

IVVisualization 3 β€” Steady State and Transient in First Order

For yβ€²+ky=1y' + ky = 1, the starting value fades when k>0k > 0 and takes over when k<0k < 0.

VQuiz Questions

Problem 1 Β· Assembling the General Solution

Given: yp=βˆ’2y_p = -2 is a particular solution of yβ€²β€²βˆ’4y=8y'' - 4y = 8 β€” find the general solution.

βœ… Correct! ycy_c solves yβ€²β€²βˆ’4y=0y'' - 4y = 0 (roots Β±2\pm 2), and adding the one particular solution βˆ’2-2 gives every solution.
❌ Not quite. That is only ycy_c; it solves yβ€²β€²βˆ’4y=0y'' - 4y = 0, not =8= 8. Add the particular solution.
❌ Check the roots. r2βˆ’4=0r^2 - 4 = 0 gives r=Β±2r = \pm 2 (real), so ycy_c uses eΒ±2xe^{\pm 2x}, not sines and cosines.
❌ Check by plugging in. For the constant 22: 0βˆ’4β‹…2=βˆ’8β‰ 80 - 4 \cdot 2 = -8 \neq 8. The given yp=βˆ’2y_p = -2 is the one that works.
Show solution

Step 1, ycy_c: the reduced equation yβ€²β€²βˆ’4y=0y'' - 4y = 0 has r2βˆ’4=0r^2 - 4 = 0, r=Β±2r = \pm 2, so yc=c1e2x+c2eβˆ’2xy_c = c_1e^{2x} + c_2e^{-2x}.

Step 2, ypy_p: check βˆ’2-2: (βˆ’2)β€²β€²βˆ’4(βˆ’2)=8(-2)'' - 4(-2) = 8. βœ“

y=βˆ’2+c1e2x+c2eβˆ’2x.y = -2 + c_1e^{2x} + c_2e^{-2x}.

Problem 2 Β· Two Solutions of the Same Equation

Given: uu and vv both solve L y=f(x)L\,y = f(x), where LL is linear and fβ‰ 0f \neq 0 β€” which function must solve the homogeneous equation L y=0L\,y = 0?

βœ… Correct! L(uβˆ’v)=L(u)βˆ’L(v)=fβˆ’f=0L(u - v) = L(u) - L(v) = f - f = 0 β€” the key step of Claim 2.
❌ Not quite. L(u+v)=f+f=2fL(u + v) = f + f = 2f, which is not 00 when fβ‰ 0f \neq 0.
❌ Not quite. Linearity says nothing about products: L(uv)L(uv) is not L(u) L(v)L(u)\,L(v) in general.
❌ Not quite. L(2uβˆ’v)=2fβˆ’f=fL(2u - v) = 2f - f = f: this is another solution of the full equation, not of the homogeneous one.
Show solution

By linearity, L(au+bv)=a L(u)+b L(v)=(a+b) fL(au + bv) = a\,L(u) + b\,L(v) = (a + b)\,f. This is 00 exactly when a+b=0a + b = 0, i.e. for multiples of uβˆ’vu - v:

L(uβˆ’v)=fβˆ’f=0.L(u - v) = f - f = 0.

So any two particular solutions differ by a member of ycy_c.

Problem 3 Β· Fitting the Initial Values

Given: yβ€²β€²+y=xy'' + y = x has the particular solution yp=xy_p = x β€” find the solution with y(0)=1y(0) = 1, yβ€²(0)=0y'(0) = 0.

βœ… Correct! y(0)=1y(0) = 1 and yβ€²(0)=1βˆ’0βˆ’1=0y'(0) = 1 - 0 - 1 = 0, and it solves the full equation.
❌ Check the slope. yp=xy_p = x contributes slope 11 at 00, so yβ€²(0)=1y'(0) = 1 here. The constants must be fitted to the whole yp+ycy_p + y_c, not to ycy_c alone.
❌ Not quite. cos⁑x\cos x solves yβ€²β€²+y=0y'' + y = 0, not =x= x. The particular solution has to be included before fitting.
❌ Check the slope. Its derivative at 00 is 1+0+1=21 + 0 + 1 = 2, not 00.
Show solution

General solution: y=x+c1cos⁑x+c2sin⁑xy = x + c_1\cos x + c_2\sin x, so yβ€²=1βˆ’c1sin⁑x+c2cos⁑xy' = 1 - c_1\sin x + c_2\cos x.

y(0)=c1=1,yβ€²(0)=1+c2=0Β β‡’Β c2=βˆ’1.y(0) = c_1 = 1,\qquad y'(0) = 1 + c_2 = 0 \ \Rightarrow\ c_2 = -1.

Hence y=x+cos⁑xβˆ’sin⁑xy = x + \cos x - \sin x.

Problem 4 Β· When the Split Means Nothing

Given: yβ€²βˆ’3y=6y' - 3y = 6 β€” which statement describes its solutions as tβ†’βˆžt \to \infty?

βœ… Correct! Here k=βˆ’3<0k = -3 < 0: y=βˆ’2+c e3ty = -2 + c\,e^{3t}, and c e3tc\,e^{3t} grows whenever cβ‰ 0c \neq 0.
❌ That is the k>0k > 0 picture. In yβ€²+ky=6y' + ky = 6 form, k=βˆ’3k = -3, so yc=c e3ty_c = c\,e^{3t} grows instead of dying away.
❌ Not quite. The constant solution satisfies 0βˆ’3y=60 - 3y = 6, so it is y=βˆ’2y = -2; and the other solutions do not approach it.
❌ Not quite. y=0y = 0 is not even a solution (0βˆ’0β‰ 60 - 0 \neq 6), and c e3tc\,e^{3t} grows for cβ‰ 0c \neq 0.
Show solution

Write it as yβ€²+ky=6y' + ky = 6 with k=βˆ’3k = -3. A constant ypy_p satisfies βˆ’3yp=6-3y_p = 6, so yp=βˆ’2y_p = -2; and yc=c eβˆ’kt=c e3ty_c = c\,e^{-kt} = c\,e^{3t}.

y=βˆ’2+c e3t.y = -2 + c\,e^{3t}.

For cβ‰ 0c \neq 0 the exponential runs off to ±∞\pm\infty and dominates; the initial condition never stops mattering, so there is no steady state.

Solved: 0 / 4