Extended version of associated Legendre eq. Can I use the Frobenius method?

In summary, we have a differential equation that involves functions of \mu and x, with a limiting case of n \rightarrow \infty resulting in an associated Legendre equation. The solutions can be found using the Frobenius method and have a similar behavior to those obtained from the associated Legendre's equation. Additionally, the differential relation between x and \mu can be integrated to give a form of the solutions.
  • #1
omyojj
37
0
Hello,

Let us assume we have a differential equation

[tex] ( \frac{d^2}{dx^2}+ \frac{2}{1+1/n}\Theta_n^{n-1} - \nu^2 ) y = 0[/tex]

where

[tex]\Theta_n = (1-\mu^2)^{1/(n+1)}[/tex]

is a function of [tex]\mu[/tex] which is a function of [tex]x[/tex] :

[tex] \frac{d\mu}{dx} = \Theta_n^n = (1-\mu^2)^{n/(n+1)} [/tex]

In terms of [tex]\mu[/tex] and [tex]\frac{d}{dx} = \frac{d\mu}{dx}\frac{d}{d\mu}[/tex], the above equation becomes

[tex]\left( \Theta_n^n\frac{d}{d\mu}\Theta_n^n\frac{d}{d\mu} + \frac{2}{1+1/n}\Theta_n^{n-1} - \nu^2 \right)y = 0[/tex]

In the limit of [tex]n \rightarrow \infty [/tex], we have

[tex]\lim_{n\rightarrow \infty} \Theta_n^n = 1- \mu^2 [/tex]

[tex]\left( (1-\mu^2)\frac{d}{d\mu}(1-\mu^2)\frac{d}{d\mu} + 2(1-\mu^2) - \nu^2 \right) y = 0 [/tex]

and this is just associated Legendre equation.

[tex]y^{\prime\prime} - \frac{2\mu}{1-\mu^2}y^{\prime} + \left[ \frac{a(a+1)}{1-\mu^2}-\frac{\nu^2}{(1-x^2)^2}\right]y = 0[/tex]

with a=1.

(The solutions go like this

[tex] P_{1}^{\pm\nu} \propto ( 1+ \mu )^{\pm \nu/2} \cdot ( 1 - \mu )^{\mp \nu/2} \cdot (\nu - \mu) [/tex]

)

I think that solutions should show qualitatively similar behavior to that obtained from the associated Legendre's equation, But coudn't make any progress

Can I solve this equation utilizing a commonly-used technique like the Frobenius method for any rational number n > 0?

Can't I just have the form that the solutions might have? (like power series)

Thank you..

p.s. I should further note that the differential relation b/w x and mu can be directly integrated to give (x = 0 when mu = 0)

[tex] x = \mu {}_2 F_1 (1/2,\,\, n/(n+1);\,\,3/2;\,\,\mu^2) [/tex]
In the limiting case (n -> ∞ )

[tex] x = \mu {}_2 F_1 (1/2,\,\,1;\,\,3/2;\,\,\mu^2) = \tanh^{-1}\mu[/tex]
 
Last edited:
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  • #2
So the differential equation can be rewritten in terms of x ( (1-\tanh^2x)\frac{d^2}{dx^2} + \frac{2}{1+1/n}\tanh x\,\Theta_n^{n-1} - \nu^2 )y = 0
 

1. What is the significance of the extended version of associated Legendre equation?

The extended version of associated Legendre equation is used to solve problems involving spherical harmonics, which are important in many areas of physics and mathematics. It allows for the expansion of a function in terms of Legendre polynomials, which can then be used to describe the behavior of physical systems.

2. How does the Frobenius method apply to the extended version of associated Legendre equation?

The Frobenius method is a technique for finding solutions to differential equations with singular points. In the case of the extended version of associated Legendre equation, the singular point is at the poles of the spherical coordinate system. The Frobenius method is used to find a series solution to the equation.

3. Can the extended version of associated Legendre equation be used for all types of physical systems?

Yes, the extended version of associated Legendre equation is a generalization of the traditional Legendre equation and can be used for a wide range of physical systems. It is commonly used in problems involving spherical symmetry, such as the behavior of particles in a spherical potential well.

4. What is the advantage of using the extended version of associated Legendre equation?

The extended version of associated Legendre equation allows for the expansion of functions in terms of Legendre polynomials with complex arguments. This makes it useful for solving problems involving spherical harmonics in quantum mechanics and electromagnetism, where complex arguments are often encountered.

5. Are there any limitations to using the extended version of associated Legendre equation?

One limitation of the extended version of associated Legendre equation is that it is only applicable to problems with spherical symmetry. It also requires the use of the Frobenius method, which can be time-consuming and difficult to apply in some cases. Additionally, the solutions obtained using this method may not always be physically meaningful, so caution must be taken when interpreting the results.

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