What does l represent in the radial Schrodinger equation?

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Homework Help Overview

The discussion revolves around the radial Schrödinger equation in quantum mechanics, specifically focusing on the implications of the angular momentum quantum number, l, in the context of a potential well defined by V(r). The original poster is attempting to find the minimum value of Vo for which a bound state exists, considering the case where energy E is less than zero.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster questions the meaning of l in the radial Schrödinger equation, suggesting it may relate to angular momentum. They explore the case of l=0 and derive expressions for the wave function in different regions. Participants discuss the implications of taking the limit as E approaches zero, particularly in relation to the parameters β and k.

Discussion Status

Participants are actively engaging with the mathematical aspects of the problem, particularly the behavior of the parameters as E approaches zero. There is a focus on understanding the limit of β/k and its implications for the boundary conditions. Some guidance has been provided regarding the signs and values of β, but no consensus has been reached on the final interpretation or next steps.

Contextual Notes

The discussion involves the application of boundary conditions and the behavior of the wave function at the limits of the potential well. There are ongoing questions about how to properly apply the limit E→0 in the context of the derived equations.

Dassinia
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Hi,

Homework Statement



A particle of mass m has a potential
V(r)= -Vo r<a
0 r>a

Find the minimum value of Vo for which there's a bound state of energy and angular momentum are zero by solving shrodinger equation for E<0 and taking the limit E-> 0

Homework Equations


The Attempt at a Solution


I want to know what does l represent in the radial shrodinger equation ? Is it the angular momentum ?
For now, I considered l=0 and solved Shrodinger equation
I got
r<a
u(r)=C*sin(βr) with β=sqrt(2m(Vo+E)/h²)
r>a
u(r)=Bexp(-kr) with k= sqrt(-2mE/h²)

With boundary conditions we have
-β/k=tan(βa)

Where am I supposed to use E->0 ..?
Is it just in β=sqrt(2m(Vo+E)/h²)
so that Vo=β²h²/2m ?
 
Last edited:
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You need to let E → 0 in both β and k.
 
So we have that k=0 and then ? I don't Know what i have to do then
 
Dassinia said:
So we have that k=0 and then ? I don't Know what i have to do then

What is the limit of β/k as E → 0? What does that tell you about the quantity βa in tan(βa)?
 
We have tan(aβ)= -β/k=-sqrt(-1-Vo/E)
so when E-> 0-
tan(aβ)=-infinity
so βa=-pi/2 ?
 
Last edited:
Dassinia said:
We have tan(aβ)= -β/k=-sqrt(-1-Vo/E)
so when E-> 0-
tan(aβ)=-infinity
so βa=-pi/2 ?

Yes, except for the sign. β is a positive quantity.
 
OK Thank you !
 

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