Electric potential distribution of a charged circular rod

In summary: Your Name]In summary, to calculate the electric potential at a point that is not on the rod's axis, you can use the distance formula in cylindrical coordinates or the Pythagorean theorem. These will give you the distance between the charge element and the point P.
  • #1
kth
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Homework Statement


Im trying to calculate the electric potential created by a circular rod of charge Q and radius R at a random point (not only on the rod's axis). The rod can be considered very thin.


Homework Equations





The Attempt at a Solution


V = k \int dq/r
My problem is how to express r in a better way. I know i have to use cylindrical coordnates (r,z) but how can i express the distance from the charge element dq when the point P is not on the rods axis?
 
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  • #2



Hello there,

To calculate the electric potential at a point that is not on the rod's axis, you can use the distance formula in cylindrical coordinates:

r = √(x^2 + y^2)

Where x and y are the coordinates of the point P. This will give you the distance from the charge element dq to the point P.

Another approach would be to use the Pythagorean theorem to find the distance between the charge element and the point P:

r = √(z^2 + (R - x)^2)

Where z is the distance from the center of the rod to the point P and x is the distance from the center of the rod to the charge element dq.

I hope this helps! Let me know if you have any other questions.
 
  • #3


I would suggest using the formula for electric potential in cylindrical coordinates, which is V = kλln(r/R), where λ is the linear charge density of the rod and R is the radius of the rod. This formula takes into account the distance from the charge element dq to the point P, which is represented by the natural logarithm term. Additionally, since the rod is considered very thin, we can assume that the linear charge density is constant throughout the rod. Therefore, the formula can be simplified to V = kQln(r/R)/L, where Q is the total charge of the rod and L is the length of the rod. This formula should give you the electric potential at any point P, even if it is not on the rod's axis.
 

FAQ: Electric potential distribution of a charged circular rod

What is electric potential distribution?

Electric potential distribution refers to the way electric potential (also known as voltage) is distributed or spread out in a given region. It is affected by factors such as the presence of charged objects, the distance between them, and their relative positions.

What is a charged circular rod?

A charged circular rod is a cylindrical object that has a net positive or negative charge. It is often used as a simplified model to study the behavior of electric fields and potentials in a 2-dimensional circular system.

How is the electric potential distribution of a charged circular rod calculated?

The electric potential distribution of a charged circular rod can be calculated using the equation V = kQ/r, where V is the electric potential, k is a constant, Q is the charge of the rod, and r is the distance from the center of the rod to the point of interest.

How does the electric potential distribution change as the distance from the charged circular rod increases?

As the distance from the charged circular rod increases, the electric potential decreases. This is because the electric potential is inversely proportional to the distance from the charged object, meaning that the further away you are, the weaker the electric potential will be.

How does the presence of other charged objects affect the electric potential distribution of a charged circular rod?

The presence of other charged objects can influence the electric potential distribution of a charged circular rod. If there are other positively charged objects nearby, the electric potential near the rod will decrease, and if there are negatively charged objects nearby, the electric potential will increase. This is due to the principle of superposition, which states that the total electric potential at a point is the sum of the electric potentials due to each individual charge.

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