Electric field on a tapered cylinder?

In summary, the conversation discusses the electric field on a tapered cylinder, specifically the voltage at a point that is 1/10th the diameter of the large end when a voltage is applied to the other end and the cylinder is grounded. The expert suggests using a moment method to calculate the charge at the point, which will result in field enhancement due to the smaller surface area. They also mention that there are closed form solutions available, but they can be complex and involve hypergeometric functions.
  • #1
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Electric field on a tapered cylinder?

I have a rod which is 1" in diameter, and 4 inches long, the last inch of one side of the rod tapers down to a point of 1/10th inch (.01).

The rod also has a cylinder which it fits in, which has a taper which follows the rods taper exactly. There is a gap between the rod and cylinder through the whole length of .01

cylinder.jpg


If a voltage were applied to the large diameter end of the inner rod of +100V. And the (outer) cylinder was grounded, What would the voltage be at the point which is 1/10th the diameter of the large end?

Since the rod and cylinder essentially form a capacitor, would the smallest area (tapered point) have the largest charge? Would the charge be magnified, or greater than the applied charge because of the reduced area?

How could the charge at the point be calculated?
 
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  • #2


My answer to any general calculating charge question is to use a moment method. There are usually closed form approximations you can make but since you are interested in the behaviour of the field around the taper then I do not know of any easy way of doing it via closed form. Maybe there is a way, I am not aware of it. But the point is going to give rise to field enhancement. The charge density there is going to be higher due to the smaller surface area and this is going to increase the electric field local to the point.
 
  • #3


There are closed form - or nearly so - solutions, but they are far from trivial. See Section 3.4 of Jackson.

I sure hope you like hypergeometric functions!
 

FAQ: Electric field on a tapered cylinder?

1. What is an electric field on a tapered cylinder?

An electric field on a tapered cylinder refers to the strength and direction of the electric force exerted on charged particles near the surface of a cylinder that has a varying diameter along its length.

2. How is the electric field on a tapered cylinder calculated?

The electric field on a tapered cylinder can be calculated using the formula E = Q / (2πεrL), where Q is the total charge on the cylinder, ε is the permittivity of the material, r is the distance from the center of the cylinder, and L is the length of the cylinder.

3. What factors affect the electric field on a tapered cylinder?

The electric field on a tapered cylinder is affected by the charge on the cylinder, the permittivity of the material, the length of the cylinder, and the distance from the center of the cylinder. It is also affected by the tapering of the cylinder, as the changing diameter causes the electric field to vary along its length.

4. How does the electric field on a tapered cylinder compare to that of a straight cylinder?

The electric field on a tapered cylinder is generally stronger than that of a straight cylinder, as the tapering of the cylinder causes the electric field to concentrate towards the smaller end of the cylinder. However, the exact strength of the electric field will depend on the specific dimensions and properties of the cylinder.

5. What are some real-world applications of the electric field on a tapered cylinder?

The electric field on a tapered cylinder has various applications in fields such as electronics, optics, and materials science. It is used in the design of capacitors, sensors, and antennas. It also plays a role in the electroplating process and the production of optical fibers. Additionally, the concept of the electric field on a tapered cylinder is important in understanding the behavior of lightning strikes on tall, tapered structures such as buildings and trees.

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