Energy Conservation in Multiple Point Charges

In summary, the conversation discusses a problem involving four point charges forming a square and a particle with charge q being released and given a push to acquire speed v. It eventually ends up at the center of the square and is momentarily at rest. The conversation then discusses the use of energy conservation to determine the initial speed v of the particle, with the final equation being v= \sqrt {\frac{\ 3.31kq^2}{md}}. However, there is a mistake in the calculation of the potential energy as one of the distances is not correct. The conversation ends with a thank you to Galileo for pointing out the error.
  • #1
quicknote
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Can somebody please check over my solution. I cannot figure out what's wrong. My final answer is not right. I think I may have an error with the signs of the point charges or may have a dumb calculation error.

Thank youFour point charges, fixed in place, form a square with side length d.
The particle with charge q is now released and given a quick push; as a result, it acquires speed v. Eventually, this particle ends up at the center of the original square and is momentarily at rest. If the mass of this particle is m, what was its initial speed v?


See picture here: http://ca.geocities.com/canbball/index.html

By using energy conservation I get:
[tex]k_{i} = U_{f} -U_{i} [/tex]

[tex] \frac{\ 1}{2} *mv^2 =k[( \frac{\ -3q^2}{\frac{\ d}{\sqrt{2}}} + \frac{\ 5q^2}{\frac{\ d}{\sqrt{2}}} + ( \frac{\ 2q^2}{\frac{\ d}{\sqrt{2}}}) - (( \frac{\ -3q^2}{d} + ( \frac{\ 2q^2}{d} + ( \frac{\ 5q^2}{d})] [/tex]

after simplifying, I finally get:
[tex] v= \sqrt {\frac{\ 3.31kq^2}{md}} [/tex]ETA: Sorry, I'm not sure how to fix the tex...
 
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  • #2
Just scooping quickly, the distance(s) in U_i don't look right. The charge is not a distance d away from all three other charges.
 
  • #3
:blushing: You're right...one of the them is [tex] \sqrt{2} [/tex] away.

Thanks Galileo!
 

FAQ: Energy Conservation in Multiple Point Charges

What is energy conservation in multiple point charges?

Energy conservation in multiple point charges is a fundamental principle of physics that states that the total energy of a system remains constant, even as it undergoes changes or interactions with other systems. In the case of multiple point charges, this principle applies to the conservation of electrical potential energy.

How does energy conservation apply to multiple point charges?

In a system of multiple point charges, the total electrical potential energy is conserved as long as there are no external forces acting on the charges. This means that the total energy of the system, which includes both kinetic and potential energy, remains constant even as the charges interact and change positions.

What is the formula for calculating energy conservation in multiple point charges?

The formula for energy conservation in multiple point charges is given by: E = K + U, where E is the total energy of the system, K is the kinetic energy, and U is the potential energy. This formula is based on the principle that energy cannot be created or destroyed, only transformed from one form to another.

How can energy conservation in multiple point charges be applied in real-life situations?

Energy conservation in multiple point charges can be observed in various real-life situations, such as in electrical circuits, where the total energy of the system is conserved despite the flow of current between multiple charges. It can also be applied in the study of electromagnetic fields and their interactions with charged particles.

Are there any exceptions to the principle of energy conservation in multiple point charges?

Yes, there are some exceptions to this principle. For example, if external forces, such as friction or external electrical fields, are acting on the charges, then the total energy of the system may not be conserved. Additionally, in certain extreme scenarios, such as the collision of particles at high energies, some energy may be converted into mass according to Einstein's famous equation, E=mc².

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