Potential Energy of a Charge Configuration

AI Thread Summary
Calculating the total potential energy of a charge configuration involving multiple charges typically requires summing the potential contributions from each charge. In the example of a 2D square with charges at each corner, there is no shortcut to avoid this summation process. The consensus is that a detailed calculation is necessary, as quick methods do not exist for such configurations. The discussion highlights a frustration with tedious calculations in exams, contrasting with the professor's usual approach. Ultimately, understanding the underlying concepts remains essential despite the workload involved.
CogitoEAS
Messages
9
Reaction score
0
Is there a quick way to figure out the total potential energy between more than 2 charges without having to find the potential at each point and the. Multiplying it by the charge at that point and adding it all up?

For example - a 2D square with a charges Q, 2Q, -3Q, and another Q at each corner and let's say each side of the square has length "d"

I'm basically wondering if there's a way to calculate the total potential energy of this charge configuration without a page and a half of work
 
Physics news on Phys.org
There really isn't a "quick" way that I know of. You pretty much have to do a sum when calculating the potential energy. That's just the way it's done.
 
Thank you -I figured as much. I just have a professor who typically writes problems that aren't very tedious especially when you understand the concept(s). I saw a problem like this on an old exam and thought the busywork I had to do was a little uncharacteristic of his testing style.

Thanks again.
 
I was using the Smith chart to determine the input impedance of a transmission line that has a reflection from the load. One can do this if one knows the characteristic impedance Zo, the degree of mismatch of the load ZL and the length of the transmission line in wavelengths. However, my question is: Consider the input impedance of a wave which appears back at the source after reflection from the load and has traveled for some fraction of a wavelength. The impedance of this wave as it...
Back
Top