Electric Field Integration Outside a Cylinder

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The discussion revolves around calculating the electric field generated by a thin, hollow cylinder with a negative charge of -90nC, specifically at a point 5.0 cm from one end of the cylinder. The user is attempting to integrate the contributions of infinitesimal charge rings along the cylinder's length to find the total electric field at the specified location. They express difficulty in formulating the integration equation and seek guidance on how to represent the charge on each ring correctly. A suggestion is made to use "z" instead of "Δz" for clarity and to ensure the charge expression includes "dz" to facilitate integration. The conversation emphasizes the need for a clear mathematical representation to solve the problem effectively.
frostmephit
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Homework Statement


A thin, hollow cylinder missing its two end caps is shown to have a charge of -90nC. It has a radius of .5 cm and is 2.0 cm long. Find the charge on an \alpha particle 5.0cm away from the end of the cylinder closest to the particle. (The center of the cylinder is on the same axis as the alpha particle.)


Homework Equations


(Electric Field of a Ring)
E=1/(4\pi\epsilon\o) * q\Deltaz/(R^2+\Deltaz^2), where R is the radius of the cylinder and z is the distance from the center of the ring to the observation location, q is the charge, and the charge of an alpha particle is given by 2e


The Attempt at a Solution


The way I have gone about doing this is in such a manner as to divide the cylinder up into so many small rings, each with an infinitesimaly small charge. The problem is, I can't figure out how to create an equation representing the whole cylinder. I am aware that the charge on the rings would be equal to the surface area of one of them divided by the surface area of the greater cylinder times the charge, but I've been having trouble representing this as an equation for integration. Am I going in the right direction, and could someone please help?
 
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frostmephit said:

Homework Equations


(Electric Field of a Ring)
E=1/(4\pi\epsilon\o) * q\Deltaz/(R^2+\Deltaz^2), where R is the radius of the cylinder and z is the distance from the center of the ring to the observation location, q is the charge, and the charge of an alpha particle is given by 2e


The Attempt at a Solution


The way I have gone about doing this is in such a manner as to divide the cylinder up into so many small rings, each with an infinitesimaly small charge. The problem is, I can't figure out how to create an equation representing the whole cylinder. I am aware that the charge on the rings would be equal to the surface area of one of them divided by the surface area of the greater cylinder times the charge, but I've been having trouble representing this as an equation for integration. Am I going in the right direction, and could someone please help?
Okay. First, I'll recommend using z instead of Δz, for the distance from the alpha particle to the ring.

If each ring has a "length" of dz along the z-direction, what would be the charge q on that ring? You're expression for q should contain a "dz" in it, so that will (hopefully) suggest an integral.
 
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