Associated Legendre Function with Angles

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The discussion centers on the validity of using the substitution x = cos(θ) in the context of associated Legendre functions. It highlights that while the left-hand side of the equation is always positive, the right-hand side can be both positive and negative depending on the angle θ. The importance of managing the range of θ is emphasized, particularly noting that in spherical coordinates, θ is typically constrained between 0 and π, ensuring that sin(θ) remains non-negative. This range allows for the effective application of the substitution in mathematical contexts. Overall, the substitution is justified within the specified domain of the associated Legendre functions.
bryanso
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Homework Statement
In Associated Legendre Function with Angles ... why is the following argument used?
Relevant Equations
## \sqrt{1 - x^2} = sin\,\theta ##
In Wikipedia https://en.m.wikipedia.org/wiki/Associated_Legendre_polynomials, Section Reparameterization in terms of angles, I see this argument:

Let ## x = cos\,\theta ##

## \sqrt{1 - x^2} = sin\,\theta ##

This is also in Griffiths' Introduction to Quantum Mechanics.

Why is this a valid argument?

The LHS is always positive. The RHS is sometimes positive and sometimes negative. ##\theta = -1## makes it wrong.
 
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Yes, one has to manage the range of the angels. For ##\theta > \pi## we need the negative root. I assume that most applications have angels from ##[0,\pi]## and in the other case: switch to the opposite orientation of the coordinate system. The problem only occurs if angels occur in both ranges.
 
Thanks!
 
bryanso said:
Homework Statement:: In Associated Legendre Function with Angles ... why is the following argument used?
Relevant Equations:: ## \sqrt{(1 - x)^2} = sin\,\theta ##

In Wikipedia https://en.m.wikipedia.org/wiki/Associated_Legendre_polynomials, Section Reparameterization in terms of angles, I see this argument:

Let ## x = cos\,\theta ##

## \sqrt{(1 - x)^2} = sin\,\theta ##
No, that's not what it says. Instead, it's ##\sqrt{1 - x^2}##. This is a standard substitution used in trig substitution in integrals.

You also have the same incorrect equation in your Relevant Equations.
bryanso said:
This is also in Griffiths' Introduction to Quantum Mechanics.

Why is this a valid argument?

The LHS is always positive. The RHS is sometimes positive and sometimes negative. ##\theta = -1## makes it wrong.
 
fresh_42 said:
Yes, one has to manage the range of the angels.
It's better to manage the range of the angles. I don't think we'd have much luck trying to manage angels.
 
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Yes I had a typo. I will try to edit it. The question remains.
 
Mark44 said:
No, that's not what it says. Instead, it's ##\sqrt{1 - x^2}##. This is a standard substitution used in trig substitution in integrals.

You also have the same incorrect equation in your Relevant Equations.

Thanks. I have edited the equations.
 
The range of ##\theta## in spherical coordinates (which is where the associated Legendre functions are used) is 0 to ##\pi##. Therefore ##\sin(\theta)## is always positive.
 
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Orodruin said:
The range of ##\theta## in spherical coordinates (which is where the associated Legendre functions are used) is 0 to ##\pi##. Therefore ##\sin(\theta)## is always positive.
Put differently, the domain of the associated Legendre functions (just as that of the Legendre polynomials) is [-1,1]. This is why ##x = \cos\theta## works so well with ##\theta \in [0,\pi]## (and, consequently, ##\sin\theta \geq 0##).
 
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