Explaining Hydrogen Atom's Line Spectra: The Rutherford Atomic Model

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Discussion Overview

The discussion centers on the limitations of the Rutherford atomic model in explaining the line spectra of the hydrogen atom. Participants explore the implications of classical physics on atomic stability and radiation emission, contrasting it with quantum mechanical perspectives.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants argue that the Rutherford model cannot explain the line spectra because it predicts a continuous spectrum due to the instability of electrons spiraling into the nucleus.
  • Others suggest that if the atom is unstable, it would emit a continuous spectrum, similar to bremsstrahlung radiation.
  • A participant proposes that the continuous radiation would imply a single wavelength, which another participant challenges as contradictory to the concept of discrete spectra.
  • There is a discussion about the nature of electron orbits in the Rutherford model, with some asserting that electrons cannot occupy arbitrary energy levels, as the model is classical and does not account for quantization.
  • One participant mentions that in a certain approximation, the Rutherford model can describe a quasi-continuous spectrum if the electron starts from a distant point, but this is limited by quantum mechanics.
  • Another participant emphasizes that electron capture is a quantum mechanical phenomenon and does not relate to the classical idea of electrons spiraling towards the nucleus.

Areas of Agreement / Disagreement

Participants express disagreement regarding the implications of the Rutherford model on atomic spectra. While some acknowledge that it can describe certain aspects under specific conditions, others maintain that it fundamentally fails to explain the discrete nature of hydrogen's line spectra.

Contextual Notes

The discussion reflects a reliance on classical physics concepts while contrasting them with quantum mechanical principles, highlighting the limitations of the Rutherford model without resolving the underlying disagreements.

roshan2004
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Why the rutherford atomic model can't explain the line spectra of the hydrogen atom?
 
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the most essential is that a spiralling charge will emit radiation and thus loose energy making the atom collapse.
 
But,that only explains the unstability of atom.The question is about the spectra.
 
if the atom is unstable, will there be a spectra? Well, it will be continuous -> compare with bremsstrahlung spectra.
 
So,Can I say this-Because the atom is spiralling down towards the nucleus,it will continuoulsly be giving the radiation forming a single wavelength,continuous spectra.
 
I would not say that it will forming a single wavelength, that is a discrete spectrum. Your sentence is a self contradiction.
 
So,how do I explain the reason then...
 
you just drop the "forming a single wavelength" part.
 
How about this-Rutherford's model suggests that the electrons can float around at any energy level they want, and that photons of any frequency or wavelength can be emitted.
 
  • #10
no electrons can not float around as they want! The rutherford model is a classical, non-quantum, model where electrons are orbiting the nuclei as planets orbiting the sun.

But the electrons are then under a radial acceleration, centripetal acceleration, and accelerating charges will emit radiation of continuous spectrum - there will be no stable energy levels and no atom will be stable.
 
  • #11
So it means that they are continuously giving radiation of same type in rutherford which give a continuous radiation.
 
  • #12
the radiation is continuous in time and in wavelength
 
  • #13
Thanks mate,are there any links that you know which has got the lectures on bohr's model of atom along with rutherford's and sommerfield's.
 
  • #15
Why the orbit energy in bohr model is negative?
 
  • #16
all bound states has negative energy. (It all boils down to where you define the 0 level of energy).
 
  • #17
What is meant by bound states?
 
  • #18
have you not done classical mechanics with planetary orbits and stuff? :O

roughly speaking, a system is bound if it's kinetic energy in the centre of mass system is smaller than the potential energy.
 
  • #19
Thanks
 
  • #20
and since one often counts potential energy as negative, the energy of a bound system will become negative.
 
  • #21
Really appreciate all your labour mate.
 
  • #22
roshan2004 said:
Why the Rutherford atomic model can't explain the line spectra of the hydrogen atom?

In a certain approximation, it can. If your electron starts falling from infinity (or just from very distant place), it radiates a quasi-continuous spectrum. This is called a radiative recombination. But it stops falling into the potential well before reaching the nucleus: its "lowest" orbit is determined with quantum mechanics. In fact, the electron can be captured by the nucleus in some cases (http://en.wikipedia.org/wiki/K-capture). In this sense, it can "reach" the nucleus and form a neutral particle with a proton.

Bob.
 
  • #23
But electron capture is a quantum mechanical property and has nothing to do with an electron 'spiralling' down towards the nucleus etc.
 

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