Undergrad Solving an ODE with Legendre Polynomials

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The discussion focuses on solving a specific ordinary differential equation (ODE) derived from Griffiths' "Electromagnetism" textbook, which is expressed in terms of Legendre Polynomials. The ODE is manipulated by dividing through by sin(θ) and changing variables to x = -cos(θ), leading to a form that aligns with Legendre's differential equation. This transformation demonstrates how the solution Θ can be represented as a Legendre Polynomial, P_l(cos(θ)). Participants express curiosity about the generalization of this solution and seek additional examples of ODEs that can be transformed into a similar form. The conversation emphasizes the relationship between the ODE and Legendre Polynomials, providing insight into their applications in solving physical problems.
CrosisBH
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From Griffiths E&M 4th edition. He went over solving a PDE using separation of variables. It got to this ODE
\frac{d}{d\theta}\left(\sin\theta\frac{d\Theta}{d\theta}\right)= -l(l+1)\sin \theta \Theta
Griffths states that this ODE has the solution
\Theta = P_l(\cos\theta)
Where $$P_l = \frac{1}{2^l !} \frac{d^l}{dx^l} (x^2 - 1)^l $$ is a Legendre Polynomial. I was curious to see how this generalizes. I found the definition of the Legendre's Polynomials is
[source]

I have trouble seeing how this is the form of the ODE above. I've tried playing with it but I can't get it into the form where it makes sense that the Legendre Polynomials are the solution. I'm also curious of more examples of ODEs that can be manipulated into this form. Thank you!
 
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Begin by deviding both side of
$$\frac{d}{d\theta}\bigg(\sin\theta\frac{d\Theta}{d\theta}\bigg) = - l(l+1)\sin\theta\,\Theta$$
by ##\sin\theta## to get
$$\frac{1}{\sin\theta}\frac{d}{d\theta}\bigg(\sin\theta\frac{d\Theta}{d\theta}\bigg) + l(l+1)\Theta = 0.$$
Now, introduce the new variable ##x=-\cos\theta## and thus
$$\frac{d}{d\theta} = \sin\theta\frac{d}{dx}.$$
Therefore
$$\frac{d}{dx}\bigg(\sin^2\theta\frac{d\Theta}{dx}\bigg) + l(l+1)\Theta = 0.$$
Lastly, notice that ##x^2 = \cos^2\theta## together with the trigonometric identity ##\sin^2\theta = 1-\cos^2\theta##. Thus,
$$\frac{d}{dx}\bigg((1-x^2)\frac{d\Theta}{dx}\bigg) + l(l+1)\Theta = 0$$
which exactly is Legendre's differential equation.
 
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