Finding total energy when 3 point charges are far away

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Homework Help Overview

The problem involves calculating the total energy of a system consisting of two protons and an alpha particle arranged at the corners of an equilateral triangle. The context is centered around energy conservation principles as the particles are released and move apart.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the initial setup of energy conservation, questioning the treatment of potential energy and kinetic energy as the charges are moved apart. There is exploration of how to calculate the potential energy contributions from multiple charges and the implications of their arrangement.

Discussion Status

Participants are actively engaging with the problem, offering different perspectives on how to calculate the total energy and potential energy of the system. Some guidance has been provided regarding the contributions of individual charges to the overall potential energy, and there is an ongoing examination of the assumptions made in the initial calculations.

Contextual Notes

There is a discussion about the charge of the alpha particle and its implications for potential energy calculations. Participants also consider the scenario when the particles are far apart and the assumptions regarding energy conservation in that context.

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The question and detail:
Two protons and an alpha particle are held at rest at the corners of an equilateral triangle whose side length is 8.50×10^-10 m. The particles are released and move apart. What is their total energy when they are far apart? Use 1.60×10^-19 C for the magnitude of the charge on an electron.

I setup the problem using energy conservation: K_a + U_a = K_b + U_b:

K_a = total kinetic energy of the 3 charges when they're at rest
U_a = total potential energy of the 3 charges when they're at rest
K_b = total kinetic energy of the 3 charges when they're far apart
U_b = total potential energy of the 3 charges when they're far apart

K_a = 0 since the charges don't initially move
U_b = 0 when they're far away (when they're infinitely far away)

That leaves: U_a = K_b
where U_a = 3*(k*q_1*q_2)/r so
K_b = 3*(k*q_1*q_2)/r
and the answer I got was 3 * (8.9*10^9 * (1.6*10^-19)^2)/(8.50×10^-10) = 8.04*10^-19 which is incorrect.
Am I on the right track solving the problem? What am I overlooking?
 
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Your error was assuming that you simply triple the amount of energy of a single pair of charges.

Do it this way: place the first proton in empty space, how much work to do it? none, since no other charges are pushing it away.

Bring in the second proton. HOw much work? THe same amount that is equal to the potential energy when they are in place: (kq^2)/r

Now, when the alpha is brought in, it is being pushed away by two charges that are already there. The spot that the third charge (the alpha) goes into has a potential (voltage) that is the algebraic (not vector) sum of the potentials provided by the two protons in place. use the equation V=kq/r twice, once for each proton, to find the potential for that spot, then multiply the charge of the alpha to the potential to find potential energy. Add this to the potential energy of the two protons you already had for total energy.

since q_2 = 2(q_1), total energy is (5kq^2)/r
 
Let me see if I get this right, the potential to place the first proton is 0 so the work or potential energy required is 0.

The potential to place the second proton, due to the first proton, is (k*q)/r and the potential energy is (k*q^2)/r.

The potential to place the alpha particle is the sum of the potentials of both protons, (k*q)/r + (k*q)/r or 2(k*q)/r and the potential energy required is: q_alpha * 2(k*q)/r.

And the total energy is the sum of the potential energy of the system? 0 + (k*q^2)/r + q_alpha * 2(k*q)/r
Am I also correct that the alpha also has charge 1.6*10^-19? What about when the particles move very far away (towards infinity), would the total energy be 0?
 
The alpha particle has two protons and two nutrons, so its charge is twice that of the proton. Otherwise, your summary is correct.

When the particles move to "infinity," we assume that no other object has interfered with them, and all the total energy is still there in the form of KE. Inertia rules!
 

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