How to Convert the TISE for SHM into Dimensionless Form?

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Homework Help Overview

The discussion revolves around transforming the Time-Independent Schrödinger Equation (TISE) for Simple Harmonic Motion (SHM) into its dimensionless form. The original poster presents the equation and the necessary substitutions for energy and position variables.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to manipulate the TISE using given substitutions but expresses uncertainty about the next steps. Some participants suggest focusing on the transformation of derivatives and calculating the constant from the relationship between the variables. Others question the need for specific forms of the function and express confusion about differentiation.

Discussion Status

Participants are actively engaging with the problem, providing hints and guidance on how to proceed with the transformation. There is a recognition of the need to correctly handle derivatives, and some participants express their struggles with the concepts involved. While there is no explicit consensus, the discussion is moving towards clarifying the derivative transformations needed for the solution.

Contextual Notes

Some participants mention their previous notes and relationships related to the function, indicating varying levels of familiarity with the topic. There is a sense of uncertainty regarding the assumptions and transformations required to proceed with the problem.

Exulus
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Hi guys, hoping someone can help with this manipulation. I need to transform this:
\frac{-\hbar^2}{2m}\frac{d^2}{dx^2}u(x) + \frac{1}{2}m\omega^2 x^2 u(x) = Eu(x)
Into its dimensionless form:
\frac{d^2}{dy^2}u(y) + (2\epsilon - y^2)u(y) = 0
I have the following info:
E = \epsilon\hbar\omega
x = y\sqrt{\frac{\hbar}{m\omega}}
Heres what I've done so far:
\frac{-\hbar^2}{2m}\frac{d^2}{dx^2}u(x) + \frac{1}{2}m\omega^2 y^2 \frac{\hbar}{m\omega} u(x) = \epsilon\hbar\omega u(x)
\frac{-\hbar}{m}\frac{d^2}{dx^2}u(x) + \omega^2 y^2 u(x) = 2\epsilon\omega u(x)
\frac{\hbar}{m}\frac{d^2}{dx^2}u(x) + 2\epsilon\omega u(x) - \omega^2 y^2 u(x) = 0
\frac{\hbar}{m}\frac{d^2}{dx^2}u(x) + (2\epsilon - y^2)\omega u(x) = 0
But i can't see where to go next..i know i must be close to the end though..surely!
 
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at first sight, there is one thing that remains to be done : the transformation of the derivatives.

you know that u(x) = u(y)
Hint : \frac {du(x)}{dx}= \frac{du(y)}{dx} = \frac {du(y)}{dy} \cdot \frac{dy}{dx} . More specifically, can you calculate \frac {dy}{dx} = constant ? What is that constant ? Then, do the same to get the second derivatives.

marlon

ps i did not check the calculations you have done so far but let us first look at the derivatives
 
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hmm, the only relationships i have in my notes are:

u(x) = Ce^{-\gamma x}

So \frac{d^2}{dx^2}u(x) = \gamma^2 u(x)

Where \gamma^2 = \frac{2m}{\hbar^2}(V_0 - E)

edit - just saw your hint..will inspect further!


edit again - would i be correct to assume that u(y) = Ce^{-\gamma y \sqrt{\frac{\hbar}{m\omega}}} ?
 
Last edited:
Exulus said:
hmm, the only relationships i have in my notes are:
u(x) = Ce^{-\gamma x}
So \frac{d^2}{dx^2}u(x) = \gamma^2 u(x)
Where \gamma^2 = \frac{2m}{\hbar^2}(V_0 - E)
edit - just saw your hint..will inspect further!

This is all true but you do not need this right now. The problem is quite simple, trust me. Once you get the second derivatives right, the problem is very elementary. just try it, i will keep an eye on it. :approve:

marlon
 
meanwhile, your calculations are ok. Once you get my hint (ie the constant), you are done !

marlon
 
hmm..no I am totally lost...sorry :cry:

I don't see how you can differentiate the function when you say i don't need to know what it is. I can make a wild guess that dy/dx = 2m/hbar^2..but that would just be guessing and not actually understanding.

Could you give me a further hint? To be honest functions have always confused me slightly.
 
Exulus said:
hmm..no I am totally lost...sorry :cry:
I don't see how you can differentiate the function when you say i don't need to know what it is. I can make a wild guess that dy/dx = 2m/hbar^2..but that would just be guessing and not actually understanding.
Could you give me a further hint? To be honest functions have always confused me slightly.
:-p your guess is wrong.

Well it is very easy. if you know that x = y \sqrt {\frac{\hbar}{m\omega}} then dx = dy \sqrt{\frac{\hbar}{m \omega}} and you know the constant.

But, we need to have second derivatives, this is also easy :
\frac {d^2u(x)}{dx^2}= \frac{d^2u(y)}{dx^2} = \frac {d^2u(y)}{dy^2} \cdot ( \frac{dy}{dx} )^2

So you need to replace the second derivative of u to x by \frac {d^2u(y)}{dy^2} \frac {m \omega}{\hbar}

Just substitute this into your last equation and all is done
marlon
 
Last edited:
:bugeye:

I cannot believe i didnt see that. Whoops! Simple things like that...pretty easy to overlook i guess. Thanks for the help..gonna try it out now! :)
 
no, problem, this happens to all of us

marlon
 

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