Free Electron passing over Potential Well

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Homework Help Overview

The discussion revolves around a free electron interacting with a potential well, specifically focusing on the conditions required for the electron to pass over the well and the relationship between the electron's energy and the potential well's characteristics.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore the conditions for the electron to pass over the potential well and question how the wave parameters relate to the electron's energy and the well's depth. There are attempts to derive relationships between energy, momentum, and wavelength, as well as discussions on the implications of energy conservation.

Discussion Status

Participants are actively engaging with the problem, offering various approaches to understanding the Schrödinger equation and its implications for the electron's behavior. Some guidance has been provided regarding the interpretation of energy levels and wave functions, but there remains a lack of consensus on certain aspects of the problem.

Contextual Notes

There are discussions about the specific energy values of the electron in relation to the potential well, with some participants questioning the assumptions regarding energy conservation and the definitions of energy levels in this context.

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Homework Statement



See figure attached.

Homework Equations





The Attempt at a Solution



What condition must be satisfied in order for the electron to pass over the well?

Thanks again!
 

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The solutions of the time dependent Schrödinger equation are waves both in free space and over the potential well. How are the parameters of the wave related to the energy of the electron and the depth of the well?

ehild
 
ehild said:
The solutions of the time dependent Schrödinger equation are waves both in free space and over the potential well. How are the parameters of the wave related to the energy of the electron and the depth of the well?

ehild

When E < Ub, because it is a matter wave, the electron has a finite probability of tunneling through the barrier and materializing on the other side, moving rightward with energy E as though nothing had happened in the region of 0 ≤ x ≤ L.

But I'm still lost on how to solve this one or what equation(s) I should be looking at.

EDIT: [tex]\frac{d^{2}\psi}{dx^{2}} + \frac{8\pi^{2}m}{h^{2}}[E-U(x)]\psi = 0[/tex]

This relates the mechanical energy of the particle to the potential of the well.
 
Giving this another shot.

[tex]K = \frac{1}{2}mv^{2}[/tex]

[tex]p = mv[/tex]

So,

[tex]E = \frac{p^{2}}{2m}[/tex]

but,

[tex]p=\frac{h}{\lambda}[/tex]

So,

[tex]E = \frac{h^{2}}{2m \lambda^{2}}[/tex]

then,

[tex]\lambda = \frac{h}{\sqrt{2mE}} = 430pm[/tex]
 
That is all right, but E in your equation is E-Ub=8 eV really, is not it?

You could have approached the problem also by solving the Schrödinger equation.
The electron is free as it has positive energy. Its wave function is of the form A exp(ikx). Substituting into the Schrödinger equation,

k=sqrt(2m(E-Ub))/(h/(2pi)).

But you know that k=2pi/lambda.

ehild
 
ehild said:
That is all right, but E in your equation is E-Ub=8 eV really, is not it?

You could have approached the problem also by solving the Schrödinger equation.
The electron is free as it has positive energy. Its wave function is of the form A exp(ikx). Substituting into the Schrödinger equation,

k=sqrt(2m(E-Ub))/(h/(2pi)).

But you know that k=2pi/lambda.

ehild

Well it states the electron is passing over the well so it's energy would be (5+3)eV=8eV
 
No, energy is conserved, so it would still be 3 eV. 8 eV is the energy above the bottom of the well, which is the quantity you want in this case.
 

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