Find the potential at a point: contradiction with teacher

In summary: However, if you wanted to use a more accurate approximation, using the Euler-Lagrange equation, the exact expression would be ##K \rho \pi r^2 \int_{L/2}^{L/2} \frac{dl}{\sqrt{(y^2+d^2)^2+z^2}}##
  • #1
BiGyElLoWhAt
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It's not really homework, it's something we did in class, but I don't understand why we did it this way.

Problem, you have a cylinder with uniform charge density rho and some point p which lies on the x-axis (i'll draw a picture). Find the potential at p.

Solution.

You have to integrate, so my idea (we solved this as a class and it never got to the point of me being able to throw it out there without questioning the class' and the teacher's answer)

We need to do this:
##\int K \frac{dq}{r}##
Rewrite
##K \int \frac{\rho dV}{r}##
Rewrite again
##K \int \int \int_{V} \frac{\rho dxdydz}{r}##
Rho is constant, pull it out. Make an expression for r:
1:Draw a vector from the origin (center of cylinder) to P
2:Draw a vector from the origin to some arbitrary point (x,y,z) inside the cylinder
3:Take the magnitude of the difference and that is r
So what we have now is this
##K\rho \int \int \int_{V} \frac{ dxdydz}{\sqrt{(d-x)^2+y^2+z^2}}##
In case I didn't make it clear before, p is on the x axis, that's why I got that particular expression for r, d is the distance p is from the origin.

So that is my final expression without crunching through it (we didn't do it in class, just setup the equation).

What we did in class:
Start out the same until you sub in for dV,
We used ##\pi r^2 dl =dV##
which, let me state, that I am not disputing, but, in order to solve this problem, you need a valid expression for r from each dV to p, and that's where I'm having my issue. We basically treated the volume charge density (it was explicitly stated to be a volume charge density) as if it were a linear charge density. I don't see how this is legitimate, especially when you consider the inverse proportionality with r. The teacher said it will all work out in the end, and later (after class) said that it "sort of averages out due to symmetry", but mathmatically it does not. At all. The farther you take p away from the cylinder, the closer it gets, but it's never perfect, and this was definitely some finite distance d.

I think the expression we had was
##K \rho \pi r^2 \int_{L/2}^{L/2} \frac{dl}{\sqrt{y^2 +d^2}}##

How can it be legitimate to do this? I asked him if we were just approximating, which I would have understood, but he said no. Am I missing something? Or am I right in thinking we cut some corners to get to that answer. (All of the charge is definitely NOT at the center of each dA cross section of the cylinder like we set it up to be despite the fact it's a volume charge density)

Thanks in advance
BYH
 
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  • #2
crap, forgot the picture, sorry
 

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  • #3
I would say this is an approximation for small r << d. The expression does not show the correct behaviour for small d.
 
  • #4
OK that's what I was thinking, because as p approaches infinity, the cylinder does look more and more like a thin straight rod.
 
  • #5


I can understand your confusion and frustration with the method used to solve this problem in class. It is important to always question and understand the reasoning behind the methods and equations used in scientific calculations.

In this case, it seems that your teacher may have simplified the problem by assuming that the charge density is evenly distributed throughout the cylinder, and therefore, the potential at any point on the x-axis can be calculated using the linear charge density equation. This is not a completely accurate representation of the problem, as you have pointed out, but it may have been used as a simplification for the sake of time and understanding in class.

However, as you correctly pointed out, this assumption may not hold true for all points along the x-axis, especially as the distance from the cylinder increases. In order to accurately calculate the potential at point p, a more precise method using integrals and the actual distribution of charge throughout the cylinder would need to be used.

It is important to understand the limitations and assumptions made in scientific calculations, and to always strive for more accurate and precise methods. I would suggest discussing your concerns with your teacher and perhaps exploring alternative methods for solving this problem. Keep questioning and seeking understanding in your scientific studies.
 

1. What does it mean to find the potential at a point?

Finding the potential at a point is a mathematical process used to calculate the electric potential at a specific location in space. It takes into account the distance and magnitude of all the charges in the surrounding area.

2. Why is there a contradiction with my teacher's explanation?

There could be a few reasons for this contradiction. It's possible that your teacher used a different method or formula to find the potential at a point, or they may have made a mistake in their explanation. It's best to clarify with your teacher and discuss the discrepancy.

3. Can I use different methods to find the potential at a point?

Yes, there are multiple methods that can be used to find the potential at a point, such as using Coulomb's law, Gauss's law, or the superposition principle. It's important to understand the concepts behind each method and choose the most appropriate one for the given situation.

4. How is the potential at a point related to electric potential energy?

The potential at a point is directly related to electric potential energy. Electric potential energy is the potential energy a charged particle has due to its position in an electric field. The potential at a point is the amount of electric potential energy per unit charge at that specific location.

5. Is finding the potential at a point important in real-life applications?

Yes, finding the potential at a point is important in many real-life applications, such as designing electrical circuits, understanding the behavior of lightning, and studying the properties of materials. It is also a crucial concept in the field of electrostatics and is used to explain many phenomena in the natural world.

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