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

In summary, De-Broglie's explanation on Bohr's second postulate is that the concept of standing waves should be understood in order to understand it. The 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 byCircumference = nλ/2 2∏r = nλ/2.
  • #1
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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  • #2
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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  • #3
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.
 
  • #4
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!
 
  • #5
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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1. What is De-Broglie's explanation on Bohr's Angular Momentum quantization?

De-Broglie's explanation on Bohr's Angular Momentum quantization is a theory that states that particles, such as electrons, have both wave-like and particle-like properties. This means that they possess a certain amount of energy and momentum, but also exhibit wave-like behavior, such as diffraction and interference. In the context of Bohr's model of the atom, De-Broglie's theory explains the quantization of angular momentum, which refers to the specific, discrete values that an electron can have as it orbits the nucleus of an atom.

2. How does De-Broglie's theory relate to Bohr's model of the atom?

De-Broglie's theory is used to explain the quantization of angular momentum in Bohr's model of the atom. This is because the theory states that electrons, which orbit the nucleus in Bohr's model, have both particle-like and wave-like properties. This means that the electrons can only possess certain, discrete values of angular momentum, as observed in Bohr's model.

3. What is the significance of De-Broglie's theory in quantum mechanics?

De-Broglie's theory is significant in quantum mechanics because it provides a way to understand the behavior of particles at the atomic level. It explains how particles, such as electrons, can have both wave-like and particle-like properties, and how this relates to their energy and momentum. This theory helped to pave the way for the development of quantum mechanics and our understanding of the subatomic world.

4. Can De-Broglie's theory be applied to other particles besides electrons?

Yes, De-Broglie's theory can be applied to other particles besides electrons. The theory applies to all particles that have mass and momentum, including protons, neutrons, and even larger particles like atoms and molecules. This theory is a fundamental concept in quantum mechanics and is used to describe the behavior of particles at the atomic and subatomic level.

5. How does De-Broglie's theory impact our understanding of the dual nature of matter?

De-Broglie's theory is a key factor in our understanding of the dual nature of matter. It helps to explain how particles, which were previously thought of as only having particle-like properties, also exhibit wave-like behavior. This theory has changed our understanding of matter and has led to the development of quantum mechanics, which is crucial in explaining the behavior of particles at the atomic level.

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