Why electrons can't remain in the nucleus

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Homework Help Overview

The discussion revolves around estimating the momentum of an electron confined to an atomic nucleus and deducing a formula for its speed. Participants explore why electrons cannot remain in the nucleus, referencing concepts from quantum mechanics and the uncertainty principle.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to apply the uncertainty principle to estimate the electron's velocity and compares it to escape velocity. Questions arise about the implications of the calculated speed exceeding the speed of light and the relevance of special relativity in this context.

Discussion Status

Participants are actively engaging with the original poster's calculations, questioning the assumptions made regarding the electron's mass and the applicability of special relativity. Some suggest that the mass of the electron should not be treated as constant at high speeds, while others express confusion about how to reconcile these concepts.

Contextual Notes

There is an ongoing debate about whether special relativity should be considered in the calculations, as the problem is situated within a quantum mechanics course. The original poster is uncertain about the implications of their findings and the correct approach to take.

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Homework Statement


Estimate the momentum of an electron confined to an atomic nucleus of radius a, and deduce a formula for its speed. By comparing the speed to the escape velocity explain why electrons cannot remain in the nucleus.


Homework Equations


Uncertainty principle


The Attempt at a Solution


Uncertainty Principle: ∆x∆p≈h (1)

If the electron were confined to the nucleus, the uncertainty in its position ∆x would be the radius of the nucleus. This means that the uncertainty in its momentum is given by rearranging (1) to:

∆p= ∆(mv)≈h/∆x => ∆v≈h/(m ∆x) (2)

The uncertainty in the velocity ∆v is all we know about the velocity so this is the velocity that the electron may have. (Is this explained right? How may I word this better – I get confused between uncertainty and actual velocity.)

∆v≈(6.626×10^(-34))/(9.11×10^(-31)×10^(-15) )=(6.626×10^12)/9.11

= 7.3×10^11 (this is faster than speed of light so must be wrong?)

Potential Energy of an electron in the nucleus of a Bohr atom is PE= e^2/(4πε_0 a) where the radius of the nucleus is a~10^(-15) metres.

Putting in values => PE=2.3×10^(-13) Joules

Escape velocity can be calculated from KE = PE.

KE=(m_e v^2)/2=PE
=> v = √(2PE/m_e ) =√((2 ×2.3×10^(-13))/(9.11×10^(-31) ))=707 106 781
=> v ≈ 7×10^8 ms^(-1)

So Escape Velocity ≈7×10^8 ms^(-1)

This is faster than the speed of light so I must have done something wrong as this would imply that the electron cannot escape unless its velocity is greater than the speed of light, therefore the electron would be bound?
 
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Hi there,

From a first glance at your calculus, you do not take special relativity into it. Therefore, into classical physics, many problems can lead to solution where the speed of the object is greater than the speed of light.

Cheers
 
Hi, many thanks for your comment, however I don't think the question intends special relativity to be used - it's in part of a course on QM. Not sure if that's the right attitude to take?! However, can you see any QM related things I have missed or done wrong?
 
Hi there,

Not being an expert in QM, and having very bad memories from my classes in University, I don't see anything wrong with your equation, from QM point of view.

Eventhough, since you are talking about speed that are fractions of the speed of light, you anyways need to uses special relativity.

The problem that I see with you equation is that you suppose the mass of the electron constant, which is not true for speed that great.
∆p= ∆(mv)≈h/∆x => ∆v≈h/(m ∆x) (2)
is not right from that point of view. It should be something like:
[tex]\Delta p = \Delta (mv) \approx \frac{h}{\Delta x}[/tex]
Since the mass cannot be considered constant, this becomes:
[tex]\Delta v \approx \frac{h}{\Delta m \cdot \Delta x}[/tex]

Cheers
 
Many thanks for your suggestions - I am not sure how your suggestion would lead to a different answer - in other words I'm still confused!
 
Hi there,

I am just pointing out that electrons relevant speed in atoms must be viewed as relativistic particles. Therefore, the electron's mass is not it's rest mass anymore.

Cheers
 
In relativity, momentum is defined as
[tex]p = \frac{mv}{\sqrt{1 - v^2/c^2}}[/tex]
and kinetic energy is defined as
[tex]K = \left(\frac{1}{\sqrt{1 - v^2/c^2}} - 1\right)mc^2[/tex]
where in each case m is what used to be called the "rest mass" (which is constant) not the "relativistic mass" (which changes with velocity).

As for explaining how to get the velocity: you could say that an electron stuck in the nucleus, over time, has an average velocity of 0 (otherwise it wouldn't be stuck). But if the uncertainty in that velocity is ∆v, it means the electron would actually have a velocity in some range whose characteristic width is ∆v - in some sense, the "average" magnitude of velocity is ∆v (for some definition of average).
 

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