Bohr-Sommerfeld model question "Old" Quantum Theory

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Homework Help Overview

The problem involves applying the Bohr-Sommerfeld model to develop a quantum theory of Earth satellites, focusing on calculating the orbit radius and energy in terms of the quantum number and other parameters. The context is set around a satellite with a specified mass and orbit radius, prompting questions about the relationship between quantum numbers and physical quantities.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of the Bohr-Sommerfeld model, with some attempting to derive expressions for the radius and energy based on angular momentum and gravitational forces. Questions arise about the treatment of the quantum number as a continuous variable and the implications of differentiating it.

Discussion Status

The discussion is active, with participants providing insights and clarifications on the equations involved. Some express uncertainty about specific terms and the integration process, while others confirm the validity of certain approaches and calculations. There is a collaborative effort to cross-check results and understand the underlying principles.

Contextual Notes

Participants note that the given radius is a fixed parameter, while the quantum number and energy are treated as unknowns to be determined. The discussion also touches on the legitimacy of differentiating the quantum number despite it being an integer, with references to Taylor series to justify this approach.

RJLiberator
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Homework Statement


In analogy to the Bohr theory of the hydrogen atom, develop a quantum theory of Earth satellites, obtaining expressions for the orbit radius, r_n, and the energy, E_n in terms of the quantum number n and other relevant parameters. Use the "Old" Quantum Theory. A satellite of mass 1000kg is in a circular orbit of radius 7000 km. To what value of n does this correspond? What is the satellite energy? Determine the differences in the radius, Δr_n, and in the energy ΔE_n, for successive orbits at this radius. (Hint: Differentiate with respect to n and set Δn = 1. Why is this legitimate since n is not a continuous variable?)

Homework Equations



V_{Sat} = \sqrt{\frac{GM_e}{r}}

L=angular momentum of satelite:
L_{sat} = rm_{sat}v_{sat}

T = period
T = 2*\pi\sqrt{\frac{r^3}{GM_e}}

Bohr–Sommerfeld model,

\int_0^T p_rdq_r\ =nh
h = Planck's constant = 6.626*10^(-34) J*s

The Attempt at a Solution

So, based on the above equations and m = 1000kg, r = 7000km, I can find V_s = 7548.6 m/s and the period, T = 5826.6 s.

If I have angular momentum correctly, then that is equal to 5.284*10^(13) kg*m^2/s .

I can easily set up the bounds of integration from 0 to the period, T.
But I've never used the Bohr-Sommerfeld model. I don't know what is meant by the wiki's description of "where p_r is the radial momentum canonically conjugate to the coordinate q which is the radial position and T is one full orbital period."

Once I am able to calculate the integral, it will be easy to solve for n, and thus should be easy to find the Energy.

I believe that we are allowed to treat n like a continuous variable due to how minute it will be compared to the other numbers. n will likely be so small, that it will act like a continuous variable, thus we can differentiate it.

Any help on how to get started with the Bohr-Sommerfeld model in relation to this problem? What is "dq" ?
 
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A simpler form of the Bohr model might be helpful: The results are the same: ## \\ ## 1) ## L=mvr=n \frac{h}{2 \pi} ## (Angular momentum is an integer number times ## h/(2 \pi) ##). ## \\ ## 2) ## \frac{mv^2}{r}=\frac{GMm}{r^2} ## (centripetal force=gravitational force) ## \\ ## 3) ## E_n=\frac{1}{2}mv^2-\frac{GMm}{r} ## (Energy is the sum of the kinetic energy plus the potential energy). ## \\ ## These are 3 equations, and 3 unknowns (##v ##, ##r ##, and ## E_n ##). ## \\ ## You can solve for the unknowns and then compute the required quantities. ## \\ ## Note: The integral ## \int\limits_{0}^{T} p \, dq=mv(2 \pi r)=n h ##, which is the same as ## mvr=n \frac{h}{2 \pi} ##. And you also have ## v=2 \pi r/T ##, but I don't think you need to solve for ## T ##.
 
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Hi Charles, thank you kindly for helping me.

I have some follow up questions.

1. Are you sure r is an unknown? The question states that radius = 7000km. I am finding "n", E_n, and v as my unknowns.

2. So, the bohr-sommerfeld statement (that integral) comes down to be simply nh = mv(2*pi*r)?

3. How do you type latex in the middle of the sentence on PhysicsForums like you did? :)

Thank you.
 
1) ## r ## will be a function of ## n ## and the other constants. They then give you ## r ## so that will tell you what ## n ## is. In these 3 equations, you might not need ## v ##, but you need to solve for ## r ## and ##E_n ## (I could have called it ## r_n ##, and the ## v ## I could have called ## v_n ##). ## \\ ## 2) The answer is yes. ## \\ ## 3) just type ## on both sides of the Latex expression.
 
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Ah, I see. That makes sense, so using the first equation:

mvr = n\frac{h}{2*\pi}
We get a function r of n, namely ##r(n)=\frac{n}{mv}\frac{h}{2*\pi}##.

Couldn't I use r = 7,000,000 m to find what v is in the second equation? ##v=\sqrt{\frac{GM}{r}}## and we have r, G (grav. constant), M (mass of earth). This nets us a v of 7548.6 m/s.

With that v and using an r value again of 7,000,000 m, we can find what n is in the first equation which comes out to be a huge 5.0106*10^(47).
 
RJLiberator said:
Ah, I see. That makes sense, so using the first equation:

mvr = n\frac{h}{2*\pi}
We get a function r of n, namely ##r(n)=\frac{n}{mv}\frac{h}{2*\pi}##.

Couldn't I use r = 7,000,000 m to find what v is in the second equation? ##v=\sqrt{\frac{GM}{r}}## and we have r, G (grav. constant), M (mass of earth). This nets us a v of 7548.6 m/s.

With that v and using an r value again of 7,000,000 m, we can find what n is in the first equation which comes out to be a huge 5.0106*10^(47).
The second equation gives you ## v=\sqrt{\frac{GM}{r}} ##, so for this case, yes, you can take that shortcut to the answer. ## \\ ## Meanwhile the huge ## n ## does not surprise me. I might try to compute it, and see if I concur.
 
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Yes, my thoughts when first reading this problem was that n would be very extreme and the changes from the change in n should result in very minute differences. This is what explains why we can differentiate r(n) without n being a continuous variable.
 
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RJLiberator said:
Yes, my thoughts when first reading this problem was that n would be very extreme and the changes from the change in n should result in very minute differences. This is what explains why we can differentiate r(n) without n being a continuous variable.
The arithmetic checked out=I agree with your answers. ## \\ ## Meanwhile ## r_n ## can be written as a Taylor series: ## r(n)=r(n_o)+r'(n_o)(n-n_o)+\frac{1}{2}r''(n_o)(n-n_o)^2+...##. The derivatives get successively smaller. Your explanation is ok too, but I think justifying it with the Taylor series is more mathematical. (Even though ## n ## is integer, you can assume it to be a continuous variable in the formula for ## r(n) ##, and when you put in integers ## n ## and ## n_o ##, the Taylor Series would get you the exact answer for ## r(n) ## if you included all of the terms in the series. In this case you find ## \Delta r=r(n)-r(n_o) ## with just the first derivative term).
 
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Charles, thank you for helping me with my problem and even cross-checking your solution with mine.

:biggrin::bow::bow::partytime:
 

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