Conservation of electric potential energy

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Homework Help Overview

The discussion revolves around the conservation of electric potential energy in the context of an alpha particle and a proton approaching each other. The original poster attempts to determine the distance of closest approach, considering their initial speeds and the relevant physical constants.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of conservation laws, particularly momentum and energy, in the context of the problem. There is a focus on how to incorporate momentum conservation into the calculations, especially given the lack of direct collisions.

Discussion Status

Participants are actively exploring the implications of conservation laws on the problem. Some guidance has been offered regarding the relationship between kinetic energy and electric potential energy, as well as how to approach the calculations in different reference frames.

Contextual Notes

There is a noted lack of clarity regarding the assumptions made about the system, particularly concerning the initial conditions and the behavior of the particles at the point of closest approach. The original poster expresses uncertainty about the material covered in their coursework.

xSpartanCx
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Homework Statement


An alpha particle is a nucleus of helium. It has twice the charge and four times the mass of the proton. When they were very far away from each other, but headed toward directly each other, a proton and an alpha particle each had an initial speed of 3.6×10−3c, where c is the speed of light. What is their distance of closest approach? There are two conserved quantities. Make use of both of them. (c = 3.00 × 10^8 m/s, k = 1/4πε0 = 8.99 × 10^9 N · m2/C2, e = 1.60 × 10^-19 C, mproton = 1.67 x 10^-27kg)

Homework Equations


1/2 m v^2 + 1/2 m v^2 = q(kq / r)

The Attempt at a Solution



I used the above equation to get 9.46 * 10^-14 as the radius, but that is not the correct answer. I made the assumption that the electric potential far away is 0 and that when the distance is closest they have no velocity.
 
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xSpartanCx said:
and that when the distance is closest they have no velocity.
That would violate momentum conservation.
 
mfb said:
That would violate momentum conservation.
How would I incorporate the conservation of momentum into this? There don't seem to be any collisions.
 
Last edited:
Momentum is always conserved, it does not matter if there are collisions or not. The particles will move at the point of closest approach, but what can you say about their relative motion? That will modify the energy balance, and conservation of momentum allows to find the additional parameter you have to consider.
 
mfb said:
Momentum is always conserved, it does not matter if there are collisions or not. The particles will move at the point of closest approach, but what can you say about their relative motion? That will modify the energy balance, and conservation of momentum allows to find the additional parameter you have to consider.
Shouldn't they get closer and closer, until they both have turned all of their kinetic energy into electric potential, then the electric energy converts back into velocity in the opposite direction? Like two magnets in a tube moving towards each other?

I don't know much about this, my physics professor never teaches us anything that he puts onto the online homework. I already have the correct answer, because it was a multiple choice and I guessed, but I don't know how to get it.
 
xSpartanCx said:
Shouldn't they get closer and closer, until they both have turned all of their kinetic energy into electric potential, then the electric energy converts back into velocity in the opposite direction?
In the center of mass frame, that happens. In the lab frame, they cannot both stop at the same time, that would violate conservation of momentum.

The helium nucleus is much heavier than the proton. Imagine a large truck hitting a car moving in the opposite direction. The car won't stop the truck. You do not have a direct contact here, but that does not matter - the conservation laws still apply.
 
mfb said:
In the center of mass frame, that happens. In the lab frame, they cannot both stop at the same time, that would violate conservation of momentum.

The helium nucleus is much heavier than the proton. Imagine a large truck hitting a car moving in the opposite direction. The car won't stop the truck. You do not have a direct contact here, but that does not matter - the conservation laws still apply.
Ah, I see. So I would use m1v1 - m2v2 = -vf(m1+m2) to get the velocity where they are not moving relative to each other, then use their kinetic energies to find what the electric potential is and then the distance between them. Thanks!
 

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