How to Convert the TISE for SHM into Dimensionless Form?

  • Thread starter Thread starter Exulus
  • Start date Start date
  • Tags Tags
    Shm
Click For Summary
SUMMARY

The discussion focuses on converting the Time-Independent Schrödinger Equation (TISE) for Simple Harmonic Motion (SHM) into its dimensionless form. The transformation involves substituting variables where \( E = \epsilon\hbar\omega \) and \( x = y\sqrt{\frac{\hbar}{m\omega}} \). The key steps include calculating the second derivatives correctly and substituting them into the equation to achieve the dimensionless form: \( \frac{d^2}{dy^2}u(y) + (2\epsilon - y^2)u(y) = 0 \). Participants emphasize the importance of understanding the derivatives and the constant factor derived from the variable transformation.

PREREQUISITES
  • Understanding of the Time-Independent Schrödinger Equation (TISE)
  • Familiarity with dimensional analysis in physics
  • Knowledge of variable substitution techniques in differential equations
  • Basic calculus, particularly differentiation and second derivatives
NEXT STEPS
  • Study the derivation of dimensionless forms in quantum mechanics
  • Learn about variable transformations in differential equations
  • Explore the implications of dimensionless parameters in physical systems
  • Investigate the role of constants in quantum mechanical equations
USEFUL FOR

Students and professionals in physics, particularly those focusing on quantum mechanics and mathematical methods in physics, will benefit from this discussion. It is also valuable for anyone looking to deepen their understanding of the Schrödinger Equation and its applications in SHM.

Exulus
Messages
50
Reaction score
0
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!
 
Physics news on Phys.org
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
 
Last edited:
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
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
1
Views
2K
  • · Replies 0 ·
Replies
0
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K