Rutherford and electric force

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Discussion Overview

The discussion revolves around Rutherford's interpretation of electric force in relation to his atomic model and the implications of Thomson's plum pudding model. Participants explore the nature of electrostatic forces and how they differ based on atomic structure, particularly when comparing the two models. The conversation also touches on gravitational forces in black holes versus stars, drawing parallels to atomic interactions.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant questions Rutherford's reasoning, suggesting that electrostatic force depends solely on charge and distance, not on the distribution of charge within an atom.
  • Another participant explains that in Thomson's model, the atom is neutral and exerts little force on incoming alpha particles, while Rutherford's model allows for direct interaction with the nucleus.
  • A participant argues that the strength of the Coulomb field increases significantly as an alpha particle approaches the nucleus, contrasting it with a hypothetical spread-out charge scenario.
  • There is a query about which explanation regarding the electric force is correct, highlighting the differing perspectives presented.
  • A participant introduces a comparison between gravitational forces of black holes and stars, suggesting that density plays a critical role in the strength of the gravitational field.
  • Another participant supports this by explaining that the gravitational field behaves differently inside a star compared to a black hole, drawing an analogy to atomic structure and electrostatic forces.

Areas of Agreement / Disagreement

Participants express differing views on the nature of electrostatic forces in atomic models, with no consensus reached on which explanation is correct. The discussion also introduces a parallel debate regarding gravitational forces, further complicating agreement.

Contextual Notes

Participants reference concepts such as Coulomb's law and gravitational fields without resolving the mathematical implications or assumptions underlying their arguments. The discussion remains open-ended regarding the implications of atomic structure on force interactions.

Who May Find This Useful

Readers interested in atomic theory, electrostatics, and gravitational physics may find the discussion relevant to their understanding of these concepts.

Cheman
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Rutherford and electric force...

Rutherford thought that most of the alpha particles would pass through the cloud of positive charge if the thomson model was correct - but why did he think this would be the case? I've read that apparently the charge would be spread over a greater area so it would therefore be weaker, but surely electronstatic force has nothing to do with the size of an object - just its charge and distance from the other charged particle? Surely an alpha particle at distance X from gold atom would experience exactly the same sized repulsive force from the a gold atom whether this was concentrated in a nucleus or in a larger cloud? - both would have the same field as both have the same charge.

Am I wrong?

Thanks. :smile:
 
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If I recall correctly, Thompson's plum pudding model included the electrons embedded in the positive charged matrix. So the atom was, of course, neutral, and thus exerted little force on the incoming alpha particle. In a planetary model, the alpha particle can get inside any shielding due to electrons, and interact directly with the positively charged nucleus. The rest is history.
Regards,
Reilly Atkinson
 
Cheman said:
...surely electronstatic force has nothing to do with the size of an object - just its charge and distance from the other charged particle? Surely an alpha particle at distance X from gold atom would experience exactly the same sized repulsive force from the a gold atom whether this was concentrated in a nucleus or in a larger cloud? - both would have the same field as both have the same charge.
Outside the atom there would be no difference. But the alpha particle penetrates the atom and approaches the nucleus to 10^-14 meter or so. The coulomb field is very strong there (the potential is several miljon volts there).

If the nuclear charge would be spread out over the whole atom (10000 times larger) there would be no field close to the center. Compare it to the field of the Earth and the field of a black hole with the same mass. (Well, that is always attractive, but you get the idea.)
 
Both of you have given a slightly different reason - which one is right?

On that point actually, although moving to a macromolecular scale, why does a black hole exert and greater gravitational force that a sun of the same mass? After all, gravity only relies on the mass of the 2 objects and the distance between them. (you only need to look at the equation. :wink: )

Thanks.
 
It is the density that is critical, not the overall charge/mass itself. Take the example of the black hole.

While the gravitational field may be the same far from the balck hole as the sun, in the sun, once you pass through the surface of the sun, the gravitational field decreases until you get to the centre where it becomes zero. In a black hole, there is no such surface as all the mass is stored in a singularity (for want of a better word) in the centre of the black hole. This means that as you get closer to the black hole, the gravitational force will keep on rising, resulting in huge fields that make black holes as unique as they are.

The same analogy can be applied to the case of the atom/nucleus, in Thompsons model, the electrostatic force would begin to decrease as one penetrates the atom, whereas in Rutherford's model, the electrostatic forces increase rapidly as you penetrate the atom.

Claude.
 

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