DeBroglie Wavelength: Proton at Room Temp Scattering Behavior

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Discussion Overview

The discussion revolves around the scattering behavior of protons at room temperature, specifically focusing on the implications of their deBroglie wavelength in relation to their interactions as classical particles. The scope includes theoretical considerations and mathematical reasoning related to particle physics and quantum mechanics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant suggests that two low-energy proton beams with large wavelengths may scatter either as small hard particles or as larger entities, raising questions about the nature of their interaction.
  • Another participant proposes considering the protons as classical particles and calculating the distance of closest approach based on their Coulomb potential energy and kinetic energy.
  • A claim is made regarding the distance of closest approach being about 2Å, with a follow-up question about the distribution of a room temperature proton and its implications for scattering effects.
  • One participant challenges the calculations presented, providing an alternative value for the distance based on a different potential energy assumption.
  • Another participant corrects the formula for electric potential energy, leading to a discussion about the terminology used in classical electromagnetism versus quantum mechanics.

Areas of Agreement / Disagreement

Participants express differing views on the calculations and interpretations of potential energy and scattering behavior, indicating that multiple competing perspectives remain unresolved.

Contextual Notes

There are unresolved mathematical steps and potential confusion regarding the definitions of electric potential and potential energy in different contexts, which may affect the clarity of the discussion.

edpell
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A proton at room temperature with an energy of 0.025eV has a deBroglie wavelength of about 1A (1E-10 meters). If we shoot two proton beams at each other with is low energy and large wavelength what happens? Do they scatter as if they are small hard particles of size about 1 fermi (1E-15 meters) or do they scatter as if they are big fuzzballs of size about 1A?
 
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It might be instructive to consider the two protons as classical particles and find the distance of closest approach: the distance at which the Coulomb potential energy equals their total initial kinetic energy.
 
About 2A. So if we say they are each 0.7A they never interpenetrate.

Is this correct? How do we think about the distribution of a room temperature proton? Is it 100% within 1 deBroglie wavelength? Is there a tail to the distribution so we might see an effect in the scattering?
 
Check your math. I get r = about 290 Å for a potential energy of 0.05 eV (8 x 10-21 J)

$$PE = \frac{q^2}{4 \pi \epsilon_0 r}$$
 
I think it is

$$PE = \frac{q}{4 \pi \epsilon_0 r}$$
 
The electric potential V (in volts, in MKS units) at a distance r from a charge q is given by your formula.

When you put a second charge q2 at that location, the electric potential energy of the system (in joules, in MKS units) is given by PE = q2V. When the two charges are equal in magnitude (q2 = q) this leads to my formula.

Unfortunately, in classical electromagnetism, we usually use V to refer to potential (volts), whereas in QM we often use V to refer to potential energy (joules or electron-volts), which causes confusion.
 

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