Differential-Equations Β· Unit 11 Β· Video 2 Β· Interactive Practice

The Wronskian and Abel's Theorem: Fitting Any Initial Values

IKey Formulas

FormulaNameWhat it says
c1y1(x0)+c2y2(x0)=A,c1y1β€²(x0)+c2y2β€²(x0)=Bc_1y_1(x_0) + c_2y_2(x_0) = A,\quad c_1y_1'(x_0) + c_2y_2'(x_0) = BInitial value systemTwo linear equations in the unknowns c1,c2c_1, c_2
W(y1,y2)=∣y1y2y1β€²y2β€²βˆ£=y1y2β€²βˆ’y2y1β€²W(y_1, y_2) = \begin{vmatrix} y_1 & y_2 \\ y_1' & y_2' \end{vmatrix} = y_1y_2' - y_2y_1'WronskianA function of xx; the system is solvable when W(x0)β‰ 0W(x_0) \neq 0
W≑0W \equiv 0 or W(x)β‰ 0W(x) \neq 0 for every xxAbel's theoremFor two solutions of yβ€²β€²+p yβ€²+q y=0y'' + p\,y' + q\,y = 0 with p,qp, q continuous
W(er1x,er2x)=(r2βˆ’r1) e(r1+r2)xW(e^{r_1x}, e^{r_2x}) = (r_2 - r_1)\,e^{(r_1 + r_2)x}Distinct real rootsNever zero when r1β‰ r2r_1 \neq r_2

Key Insight: For independent solutions the Wronskian is never zero, so c1y1+c2y2c_1y_1 + c_2y_2 can match any value and slope at any point.

IIVisualization 1 β€” Fit a Value and a Slope

For yβ€²β€²βˆ’3yβ€²+2y=0y'' - 3y' + 2y = 0 with y1=exy_1 = e^x, y2=e2xy_2 = e^{2x}, every value AA and slope BB at x0x_0 is reached by exactly one c1,c2c_1, c_2.

IIIVisualization 2 β€” Identically Zero or Never Zero

Abel's theorem leaves the Wronskian of two solutions only two options: zero everywhere, or zero nowhere.

πŸ’‘ For xx and x2x^2, the standard form yβ€²β€²βˆ’2xyβ€²+2x2y=0y'' - \frac{2}{x}y' + \frac{2}{x^2}y = 0 has pp and qq discontinuous at x=0x = 0 β€” exactly where W=x2W = x^2 vanishes. Abel's theorem needs continuous coefficients.

IVQuiz Questions

Problem 1 Β· A Wronskian of Exponentials

Given: y1=e2xy_1 = e^{2x} and y2=eβˆ’3xy_2 = e^{-3x} β€” find W(y1,y2)=y1y2β€²βˆ’y2y1β€²W(y_1, y_2) = y_1y_2' - y_2y_1'.

βœ… Correct! (r2βˆ’r1) e(r1+r2)x=(βˆ’3βˆ’2) eβˆ’x(r_2 - r_1)\,e^{(r_1 + r_2)x} = (-3 - 2)\,e^{-x}, never zero.
❌ Check the order. W=y1y2β€²βˆ’y2y1β€²W = y_1y_2' - y_2y_1', which gives the factor r2βˆ’r1=βˆ’5r_2 - r_1 = -5; you computed y2y1β€²βˆ’y1y2β€²y_2y_1' - y_1y_2'.
❌ Not quite. The derivatives bring down the exponents: y2β€²=βˆ’3eβˆ’3xy_2' = -3e^{-3x} and y1β€²=2e2xy_1' = 2e^{2x}, so the factor is βˆ’3βˆ’2=βˆ’5-3 - 2 = -5.
❌ Check the exponent. e2xeβˆ’3x=e(2βˆ’3)x=eβˆ’xe^{2x}e^{-3x} = e^{(2 - 3)x} = e^{-x}.
Show solution
W=e2xβ‹…(βˆ’3eβˆ’3x)βˆ’eβˆ’3xβ‹…2e2x=βˆ’3eβˆ’xβˆ’2eβˆ’x=βˆ’5eβˆ’x.W = e^{2x}\cdot(-3e^{-3x}) - e^{-3x}\cdot 2e^{2x} = -3e^{-x} - 2e^{-x} = -5e^{-x}.

This matches W(er1x,er2x)=(r2βˆ’r1) e(r1+r2)xW(e^{r_1x}, e^{r_2x}) = (r_2 - r_1)\,e^{(r_1 + r_2)x} with r1=2r_1 = 2, r2=βˆ’3r_2 = -3. Since eβˆ’x>0e^{-x} > 0, WW is never zero.

Problem 2 Β· One Zero of the Wronskian

Given: y1y_1, y2y_2 solve yβ€²β€²+p(x) yβ€²+q(x) y=0y'' + p(x)\,y' + q(x)\,y = 0 with p,qp, q continuous for all xx, and W(y1,y2)(1)=0W(y_1, y_2)(1) = 0 β€” what follows?

βœ… Correct! Abel's theorem rules out a single zero, so WW is identically zero; by the converse quoted in the video, the pair is dependent.
❌ Not quite. Abel's theorem makes the Wronskian of two solutions zero everywhere once it is zero somewhere, so the system fails at every x0x_0.
❌ Not quite. For two solutions with continuous p,qp, q an isolated zero is impossible β€” that is exactly what Abel's theorem says.
❌ Not quite. A sign change would mean WW is zero at one point and nonzero nearby, which Abel's theorem forbids.
Show solution

Abel's theorem: for two solutions of yβ€²β€²+p yβ€²+q y=0y'' + p\,y' + q\,y = 0 with p,qp, q continuous, either W≑0W \equiv 0 or W(x)β‰ 0W(x) \neq 0 for every xx. Since W(1)=0W(1) = 0, the second case is impossible, so W≑0W \equiv 0.

The converse quoted in the video says an identically zero Wronskian of two solutions means they are dependent. Such a pair cannot fit most initial values at any point.

Problem 3 Β· Solve the Initial Value Problem

Given: yβ€²β€²βˆ’4y=0y'' - 4y = 0 with y1=e2xy_1 = e^{2x}, y2=eβˆ’2xy_2 = e^{-2x}, and y(0)=3y(0) = 3, yβ€²(0)=2y'(0) = 2 β€” find W(0)W(0) and the constants.

What is W(y1,y2)(0)W(y_1, y_2)(0)?

What are c1c_1 and c2c_2?

βœ… Correct! W(0)=βˆ’4β‰ 0W(0) = -4 \neq 0, and y=2e2x+eβˆ’2xy = 2e^{2x} + e^{-2x} has y(0)=3y(0) = 3, yβ€²(0)=4βˆ’2=2y'(0) = 4 - 2 = 2.
❌ Check the Wronskian. At 00: y1=y2=1y_1 = y_2 = 1, y1β€²=2y_1' = 2, y2β€²=βˆ’2y_2' = -2, so W=1β‹…(βˆ’2)βˆ’1β‹…2W = 1\cdot(-2) - 1\cdot 2.
❌ Check the constants. The system is c1+c2=3c_1 + c_2 = 3 and 2c1βˆ’2c2=22c_1 - 2c_2 = 2; the initial values are not the constants themselves.
Show solution

At x0=0x_0 = 0: y1(0)=1y_1(0) = 1, y2(0)=1y_2(0) = 1, y1β€²(0)=2y_1'(0) = 2, y2β€²(0)=βˆ’2y_2'(0) = -2, so

W(0)=∣112βˆ’2∣=βˆ’2βˆ’2=βˆ’4β‰ 0.W(0) = \begin{vmatrix} 1 & 1 \\ 2 & -2 \end{vmatrix} = -2 - 2 = -4 \neq 0.

The system c1+c2=3c_1 + c_2 = 3, 2c1βˆ’2c2=22c_1 - 2c_2 = 2 gives c1βˆ’c2=1c_1 - c_2 = 1; adding, 2c1=42c_1 = 4, so c1=2c_1 = 2 and c2=1c_2 = 1:

y=2e2x+eβˆ’2x.y = 2e^{2x} + e^{-2x}.

Problem 4 Β· A Wronskian That Vanishes Once

Given: y1=xy_1 = x and y2=x2y_2 = x^2 solve x2yβ€²β€²βˆ’2xyβ€²+2y=0x^2y'' - 2xy' + 2y = 0, and W(x,x2)=x2W(x, x^2) = x^2 is zero at x=0x = 0 only β€” why does this not contradict Abel's theorem?

βœ… Correct! Abel's theorem assumes pp and qq continuous; dividing by x2x^2 breaks that at x=0x = 0, the one place WW vanishes.
❌ Not quite. x2/x=xx^2/x = x is not constant, so the pair is independent β€” and a dependent pair would have W≑0W \equiv 0.
❌ Not quite. The theorem covers variable coefficients, as long as p(x)p(x) and q(x)q(x) are continuous.
❌ Not quite. W=xβ‹…2xβˆ’x2β‹…1=x2W = x\cdot 2x - x^2\cdot 1 = x^2, which is 00 at x=0x = 0.
Show solution

W(x,x2)=xβ‹…2xβˆ’x2β‹…1=x2W(x, x^2) = x\cdot 2x - x^2\cdot 1 = x^2: zero at x=0x = 0, nonzero elsewhere. Abel's theorem would forbid this for an equation yβ€²β€²+p yβ€²+q y=0y'' + p\,y' + q\,y = 0 with continuous coefficients.

Dividing by x2x^2 gives the standard form yβ€²β€²βˆ’2xyβ€²+2x2y=0y'' - \frac{2}{x}y' + \frac{2}{x^2}y = 0, with p=βˆ’2/xp = -2/x and q=2/x2q = 2/x^2 undefined at x=0x = 0. The hypothesis fails exactly there, so there is no contradiction. On x>0x > 0 (or x<0x < 0) the coefficients are continuous and WW is never zero, as the theorem says.

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