De-Broglie's explanation on Bohr's Angluar Momentum quantization?

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SUMMARY

The discussion centers on De-Broglie's explanation of Bohr's angular momentum quantization, specifically addressing the conditions for standing waves in circular strings. The correct condition for standing waves is established as 2πr = nλ, where r is the radius of the ring and n is an integer. The conversation highlights the distinction between standing waves on linear strings and those on circular strings, emphasizing the necessity for whole wavelengths to avoid discontinuities. Corrections to De-Broglie's theory by Sommerfeld and Wilson are also noted, particularly the integral condition ∫pdx = nh for closed curves.

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  • Understanding of quantum mechanics principles, particularly wave-particle duality.
  • Familiarity with the concept of standing waves and their mathematical representation.
  • Knowledge of angular momentum quantization in atomic physics.
  • Basic calculus, particularly integration, to comprehend the integral conditions discussed.
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  • Study the implications of Sommerfeld and Wilson's corrections to De-Broglie's theory.
  • Learn about the mathematical derivation of standing waves in circular geometries.
  • Explore the relationship between wave functions and particle behavior in quantum mechanics.
  • Investigate the historical context and evolution of quantum theory from Bohr to modern interpretations.
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Students of quantum mechanics, physicists interested in wave-particle duality, and educators teaching advanced concepts in atomic physics will benefit from this discussion.

easwar2641993
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In order to understand about De-Broglie's explanation on Bohr's second postulate,concept of standing waves should be understood.
But condition of λ for a given value of length(string) L is given by L=nλ/s where n =1,2,3 etc.
But for a string whose ends are connected together and its shape is like a ring and let the radius of ring be r. Then standing waves condition is given by
Circumference = nλ/2
2∏r = nλ/2.

But this isn't right.
it should be 2∏r=nλ

I am missing something.Please correct me.
 
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A standing wave can exist if there is one half wavelength around the circumference - in the same way that it can exist in a half wavelength string. It's the equivalent of two waves traveling in opposite directions around the circumference. Only one node is necessary.
 
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If there were a rope around the circumference, we'd need a whole number of wavelengths in order for the wave pattern to join up properly, without discontinuities. An odd number of half wavelengths won't do - try drawing it.

Note that this 'rope picture' is nothing like the 'proper' wave function picture, at least not for small values of the principal quantum number, n. Interestingly, for large n, and ell = m = n-1 it gives a remarkably good picture.
 
Philip Wood said:
If there were a rope around the circumference, we'd need a whole number of wavelengths in order for the wave pattern to join up properly, without discontinuities. An odd number of half wavelengths won't do - try drawing it.

Note that this 'rope picture' is nothing like the 'proper' wave function picture, at least not for small values of the principal quantum number, n. Interestingly, for large n, and ell = m = n-1 it gives a remarkably good picture.
I thought this through a bit better and I think you must be right. I was assuming that the nodes at each fixed end were the equivalent to joining them together on a circular string but the phases would be wrong unless you have a full wavelength path around the circle. Cheers!
 
Yes in fact it should be 2Πr=nλ for circular circumference.
Sommerfeld and Wilson have made a correction to De-Broglie's theory that it should be:
∫pdx = nh for a closed curve, for the general case.
For our specific case assuming p is constant and not a function and λ=h/p:
∫dx=nλ
De-Broglie assumed a standing wave on a non-curved string, which works perfectly as the two waves go back and forth between two ends, but for a curved string this isn't the case, as the wave can continue, and thus destroy itself. Should a particle be a wave it must not destroy itself, as is evident by the fact matter exists for a long enough time, so the solution is to have one wave, that will interfere with itself such that the circumference is exactly an integer multiple of the wavelength, and thus not destroy itself but construct itself, and still be a standing wave.
 
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