A function of x; the system is solvable when W(x0β)ξ =0
Wβ‘0 or W(x)ξ =0 for every x
Abel's theorem
For two solutions of yβ²β²+pyβ²+qy=0 with p,q continuous
W(er1βx,er2βx)=(r2ββr1β)e(r1β+r2β)x
Distinct real roots
Never zero when r1βξ =r2β
Key Insight: For independent solutions the Wronskian is never zero, so c1βy1β+c2βy2β can match any value and slope at any point.
IIVisualization 1 β Fit a Value and a Slope
For yβ²β²β3yβ²+2y=0 with y1β=ex, y2β=e2x, every value A and slope B at x0β is reached by exactly one c1β,c2β.
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.
π‘ For x and x2, the standard form yβ²β²βx2βyβ²+x22βy=0 has p and q discontinuous at x=0 β exactly where W=x2 vanishes. Abel's theorem needs continuous coefficients.
IVQuiz Questions
Problem 1 Β· A Wronskian of Exponentials
Given:y1β=e2x and y2β=eβ3x β findW(y1β,y2β)=y1βy2β²ββy2βy1β²β.
β Correct!(r2ββr1β)e(r1β+r2β)x=(β3β2)eβx, never zero.
β Check the order.W=y1βy2β²ββy2βy1β²β, which gives the factor r2ββr1β=β5; you computed y2βy1β²ββy1βy2β²β.
β Not quite. The derivatives bring down the exponents: y2β²β=β3eβ3x and y1β²β=2e2x, so the factor is β3β2=β5.
This matches W(er1βx,er2βx)=(r2ββr1β)e(r1β+r2β)x with r1β=2, r2β=β3. Since eβx>0, W is never zero.
Problem 2 Β· One Zero of the Wronskian
Given:y1β, y2β solve yβ²β²+p(x)yβ²+q(x)y=0 with p,q continuous for all x, and W(y1β,y2β)(1)=0 β what follows?
β Correct! Abel's theorem rules out a single zero, so W is identically zero; by the converse quoted in the video, the pair is dependent.
β Not quite. Abel's theorem makes the Wronskian of two solutions zero everywhere once it is zero somewhere, so the system fails at every x0β.
β Not quite. For two solutions with continuous p,q an isolated zero is impossible β that is exactly what Abel's theorem says.
β Not quite. A sign change would mean W is zero at one point and nonzero nearby, which Abel's theorem forbids.
Show solution
Abel's theorem: for two solutions of yβ²β²+pyβ²+qy=0 with p,q continuous, either Wβ‘0 or W(x)ξ =0 for every x. Since W(1)=0, the second case is impossible, so Wβ‘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:yβ²β²β4y=0 with y1β=e2x, y2β=eβ2x, and y(0)=3, yβ²(0)=2 β findW(0) and the constants.
What is W(y1β,y2β)(0)?
What are c1β and c2β?
β Correct!W(0)=β4ξ =0, and y=2e2x+eβ2x has y(0)=3, yβ²(0)=4β2=2.
β Check the Wronskian. At 0: y1β=y2β=1, y1β²β=2, y2β²β=β2, so W=1β (β2)β1β 2.
β Check the constants. The system is c1β+c2β=3 and 2c1ββ2c2β=2; the initial values are not the constants themselves.
Show solution
At x0β=0: y1β(0)=1, y2β(0)=1, y1β²β(0)=2, y2β²β(0)=β2, so
W(0)=β12β1β2ββ=β2β2=β4ξ =0.
The system c1β+c2β=3, 2c1ββ2c2β=2 gives c1ββc2β=1; adding, 2c1β=4, so c1β=2 and c2β=1:
y=2e2x+eβ2x.
Problem 4 Β· A Wronskian That Vanishes Once
Given:y1β=x and y2β=x2 solve x2yβ²β²β2xyβ²+2y=0, and W(x,x2)=x2 is zero at x=0 only β why does this not contradict Abel's theorem?
β Correct! Abel's theorem assumes p and q continuous; dividing by x2 breaks that at x=0, the one place W vanishes.
β Not quite.x2/x=x is not constant, so the pair is independent β and a dependent pair would have Wβ‘0.
β Not quite. The theorem covers variable coefficients, as long as p(x) and q(x) are continuous.
β Not quite.W=xβ 2xβx2β 1=x2, which is 0 at x=0.
Show solution
W(x,x2)=xβ 2xβx2β 1=x2: zero at x=0, nonzero elsewhere. Abel's theorem would forbid this for an equation yβ²β²+pyβ²+qy=0 with continuous coefficients.
Dividing by x2 gives the standard form yβ²β²βx2βyβ²+x22βy=0, with p=β2/x and q=2/x2 undefined at x=0. The hypothesis fails exactly there, so there is no contradiction. On x>0 (or x<0) the coefficients are continuous and W is never zero, as the theorem says.