Schrodinger Equation for Constrained Particle

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Discussion Overview

The discussion revolves around the derivation and understanding of a specific form of the Schrödinger equation for a particle constrained to move along a line. Participants are exploring the mathematical background and reasoning behind the equation, particularly focusing on the term involving \(8\pi^2\) and its derivation. The context includes elements of quantum mechanics relevant to physical chemistry.

Discussion Character

  • Exploratory
  • Technical explanation
  • Homework-related
  • Mathematical reasoning

Main Points Raised

  • Chris expresses confusion about the derivation of the term \( \frac{8\pi^2 mE}{\hbar^2} \) in the Schrödinger equation.
  • Some participants suggest looking at external resources, such as a link to a chemistry wiki, to clarify the derivation process.
  • Chris indicates that the explanation in the linked resource does not resolve their confusion, specifically regarding the derivation of the \(8\pi^2\) value.
  • Another participant points out that the term can be derived by comparing the rearranged Schrödinger equation with the form presented in the resource.
  • Chris acknowledges a misunderstanding related to the reasoning of separation of variables in the context of the time-independent Schrödinger equation (TISE) and its relation to energy levels.
  • There is a side discussion about trigonometric identities and their application, with Chris seeking clarification on solving for an angle in a trigonometric context.
  • Some participants speculate about potential typos in the trigonometric equations presented, suggesting that they might be misinterpreted or incorrectly stated in the textbook.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the derivation of the \(8\pi^2\) term, as confusion persists. There are also differing views on the correctness of the trigonometric relationships discussed, with some participants questioning the accuracy of the presented equations.

Contextual Notes

Limitations include the potential for misunderstandings regarding the derivation steps and the assumptions made in the mathematical expressions. The discussion also highlights the dependence on definitions and the context of quantum mechanics in physical chemistry.

Who May Find This Useful

Students studying quantum mechanics, particularly in the context of physical chemistry, as well as those interested in the mathematical foundations of the Schrödinger equation and its applications.

chrisa88
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Hi, I am confused about how we obtain a part of the Schrödinger equation for a particle of mass m that is constrained to move freely along a line between 0 and a.

Equation:
\frac{d^{2}ψ}{dx^{2}}+(\frac{8∏^{2}mE}{h^{2}})ψ(x)=0


Where does the value in the parenthesis come from and what is this value for? How do we arrive at this part of this equation??

I'd really appreciate some help with this I have a quiz in the morning for physical chemistry and I really need to do well.

Thank you,

Chris
 
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Does this help?

http://chemwiki.ucdavis.edu/Physical_Chemistry/Quantum_Mechanics/Quantum_Theory/Trapped_Particles/Particle_in_a_1-dimensional_box
 
Last edited by a moderator:
Actually, I've looked at that and am still confused... I don't get where that comes from..
 
Can you be more specific where you get confused in http://chemwiki.ucdavis.edu/Physical_Chemistry/Quantum_Mechanics/Quantum_Theory/Trapped_Particles/Particle_in_a_1-dimensional_box ?
 
Last edited by a moderator:
Yes, under Step 3 where it says "If we then solve for k by comparing with the Schrödinger equation above, we find: k=" what I said in parenthesis. The 8pi^2 value. Where does this come from? I'm not sure how this is derived.
 
chrisa88 said:
Yes, under Step 3 where it says "If we then solve for k by comparing with the Schrödinger equation above, we find: k=" what I said in parenthesis. The 8pi^2 value. Where does this come from? I'm not sure how this is derived.

2 equations bfore Step 3 we have:

##-\dfrac{\hbar^2}{2m} \dfrac{d^2\psi(x)}{dx^2} = E\psi(x)##,

which can be rearranged to

## \dfrac{d^2\psi(x)}{dx^2} = -\dfrac{2mE}{\hbar^2}\psi(x)##,

which you can compare with the equation in step 3 to get the result (remembering that ##\hbar = \frac{h}{2\pi}##)
 
Wow.. I can't believe I missed that. So is this being done by the reasoning of separation of variables? Correct me if I'm wrong, but we have to separate them because E varies differently than ψ(x)? Thank you very much for pointing out my silly mistake!

Also, this doesn't really apply to this same question, but you seem very knowledgeable, so do you know how this trig occurs:
knowing: A=(c^{2}_{1}+c^{2}_{2})^{1/2} and c_{2}= Acos(\phi)
solve for \phi
which yields: \phi=sin^{-1}\frac{c_{2}}{(c^{2}_{1}+c^{2}_{2})^{1/2}}=tan^{-1}\frac{c_{2}}{c_{1}}
I'm not sure how we use the inverse sin to find the phi in the cos function.
 
chrisa88 said:
Wow.. I can't believe I missed that. So is this being done by the reasoning of separation of variables? Correct me if I'm wrong, but we have to separate them because E varies differently than ψ(x)? Thank you very much for pointing out my silly mistake!

In http://chemwiki.ucdavis.edu/Physical_Chemistry/Quantum_Mechanics/Quantum_Theory/Trapped_Particles/Particle_in_a_1-dimensional_box the starting equation was the time-independent Schroedinger equation or TISE, in which E is a constant for each energy level.

However, the TISE is usually derived en route to solving the time-dependent Schroedinger equation (TDSE), which is the more general equation. To solve the TDSE, we usually start by assuming separation of variables, which splits the TDSE into two equations, one of which is TISE.

The TISE has many solutions called the energy eigenfunctions, each of which corresponds to a different E.

The solutions of the TDSE can be constructed from the solutions of the TISE.

chrisa88 said:
Also, this doesn't really apply to this same question, but you seem very knowledgeable, so do you know how this trig occurs:
knowing: A=(c^{2}_{1}+c^{2}_{2})^{1/2} and c_{2}= Acos(\phi)
solve for \phi
which yields: \phi=sin^{-1}\frac{c_{2}}{(c^{2}_{1}+c^{2}_{2})^{1/2}}=tan^{-1}\frac{c_{2}}{c_{1}}
I'm not sure how we use the inverse sin to find the phi in the cos function.

I'm terrible at trig, maybe someone else can help, or ask it in the math forums below?
 
Last edited by a moderator:
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Thank you very much. I did make a post in the math forum.
 
  • #10
I hope my explanation wasn't too confusing. At any rate, there's usually plenty of people here who can help.
 
  • #11
Good deal, two buddies and I are studying for our physical chemistry, the quantum mechanics portion, quiz that is tomorrow. It's as if our textbook expects us to know a bunch of things without it telling us.
 
  • #12
chrisa88 said:
Also, this doesn't really apply to this same question, but you seem very knowledgeable, so do you know how this trig occurs:
knowing: A=(c^{2}_{1}+c^{2}_{2})^{1/2} and c_{2}= Acos(\phi)
solve for \phi
which yields: \phi=sin^{-1}\frac{c_{2}}{(c^{2}_{1}+c^{2}_{2})^{1/2}}=tan^{-1}\frac{c_{2}}{c_{1}}
I'm not sure how we use the inverse sin to find the phi in the cos function.

Is it a typo? I think it could make sense if c_{1}= Acos(\phi).

By squaring A=(c^{2}_{1}+c^{2}_{2})^{1/2} and recognizing Pythagoras's theorem, it could mean that c_{1} and c_{2} are the sides of a right angle triangle, and A is the hypotenuse.

c_{1}= Acos(\phi) means that c_{1}/A=cos(\phi), so c_{1} is the side adjacent to \phi since A is the hypotenuse.

So sin(\phi) would be opposite/hypotenuse which would be \frac{c_{2}}{A}, and tan(\phi) would be opposite/adjacent which would be \frac{c_{2}}{c_{1}}
 
  • #13
Yeah, I'm assuming this is just a typo unless one of the math genius gets back to me and says otherwise. It's very disturbing though because I spent probably 30-45 minutes earlier today digging through trig stuff to figure out where I was going wrong, since it was printed like this in the solutions manual to our textbook and our teacher's handwritten solutions he posts online has the same, supposed, error.
 

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