Charged Ring
This article will describe the Electric Field created by a uniformly charged thin ring and how to calculate the value of this field.
Claimed by Syed Hasnain Fall 2017 Claimed by Christopher Reny Spring 2018
The Main Idea
Charges may be arranged in a variety of ways. When points are uniformly distributed a finite distance away from some point, which we define as the origin, we call this curve as a ring. We can position a Point Charge at every point upon this ring. To analyze this continuous arrangement of charges, we say that their individual contributions are infinitesimally small, and then sum each of these contributions together to arrive at the electric field produced by this charge distribution. We can compute the net electric field of this charge distribution with Coulomb's Law and by applying integration principles.
A Mathematical Model
This mathematical model is based upon the individual Electric Field contributions of a number of point charges, each of which are defined by
[math]\displaystyle{ \vec{E} = \frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} }[/math].
We also say that this vector field is a member of a linear space of vectors. This is to say that we can apply the Superposition Principle meaning that we can sum any number of these electric field vectors and obtain another vector which is the electric field vector contributed by those charges. When we continuously sum all of the vectors produced by these charges, we get the electric field produced by the entire arrangement of charges.
The diagram above shows the electric field due to one infinitesimal piece of the ring, [math]\displaystyle{ dq }[/math]. In order to avoid rigorous computations, we can see that the electric field of the charges cancel out in the vertical direction. Only the horizontal component will remain. Since each piece, [math]\displaystyle{ dq }[/math], contributes a [math]\displaystyle{ d\vec{E} }[/math] of [math]\displaystyle{ \frac{1}{4\pi\epsilon_{0}}\frac{dq}{|\vec{d}|^{2}}\hat{d} }[/math], we can compute the horizontal component by multiplying the magnitude of [math]\displaystyle{ d\vec{E} }[/math] with [math]\displaystyle{ \cos{θ} }[/math].
[math]\displaystyle{ |d\vec{E}_{x}| = \frac{1}{4\pi\epsilon_{0}}\frac{dq}{r^2 + z^2}\cos{θ} = \frac{1}{4\pi\epsilon_{0}}\frac{dq}{r^2 + z^2}\frac{z}{(r^2 + z^2)^\frac{1}{2}} }[/math]
Now we integrate to sum all the electric field contributions of each infinitesimal [math]\displaystyle{ dq }[/math].
[math]\displaystyle{ \vec{E}_{x} = \frac{1}{4\pi\epsilon_{0}}\frac{z}{(r^2 + z^2)^\frac{3}{2}}\int_{}^{} dq = \frac{1}{4\pi\epsilon_{0}}\frac{Qz}{(r^2 + z^2)^\frac{3}{2}} }[/math]
See below for a more rigorous derivation.
A Computational Model
This simulation shows the result of the computation for a ring composed of 2000 electrons. This is why the vector is pointing into the ring rather than out of the ring, which would happen for a ring composed of positively charged points.
Rigorous Derivation
Define shape characteristics of the ring
The ring has some finite charge.
We see that this arrangement is circular, so a coordinate system with which we can define radial and angular coordinates would be useful. Naturally, this would be the polar coordinate system.
We also see that all charge is uniformly distributed some finite distance R from the center of the ring. It would be useful to let the center of the ring be the origin of our coordinate axes.
Here is a reasonable arrangement for this charged ring.
Since all charge is concentrated upon the edge of the circle, we can consider our charge distribution to be invariant with respect to radial distance. However, we do see that our charge distribution is function of theta.
Compute charge distribution function
Let us call the charge distribution as [math]\displaystyle{ \sigma }[/math]
We have a charge distributed on the edge of the circle, so
[math]\displaystyle{ \sigma=\frac{Q}{2\pi} }[/math]
where [math]\displaystyle{ Q }[/math] represents the charge of the ring.
What this equation means is that the charge is uniformly distributed along each unit of angular length. In this way, it is called angular charge density.
Compute infinitesimal charge contribution
Let us consider an infinitesimal section of the ring which contains exactly one point charge. The dimension of this section is given by [math]\displaystyle{ d\theta }[/math] which is the infinitesimal angular size. So, the infinitesimal charge contribution, [math]\displaystyle{ dQ }[/math], is
[math]\displaystyle{ dQ = \frac{Q}{2\pi}d\theta }[/math]
Compute infinitesimal electric field contribution
Let us define some arbitrary location at which we are observing this ring of charge.
[math]\displaystyle{ \vec{r} = x\hat{x}+y\hat{y} + z\hat{z} }[/math]
in polar coordinates, we see this becomes
[math]\displaystyle{ \vec{r} = Rcos(\theta)\hat{x} + Rsin(\theta)\hat{y} + z\hat{z} }[/math].
Recall that both sine and cosine are periodic with period of [math]\displaystyle{ 2\pi }[/math]. This will become important later.
The magnitude of this vector is
[math]\displaystyle{ |\vec{r}| = \sqrt{R^{2}+z^{2}} }[/math]
owing to the usage of the Pythagorean trigonometric identity.
Now, we have what we need to write the electric field vector contributed by each piece of the ring of charge. Let this vector field piece be [math]\displaystyle{ d\vec{E} }[/math].
[math]\displaystyle{ d\vec{E}=\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r}=\frac{1}{4\pi\epsilon_{0}}\frac{dQ}{(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z}) }[/math]
Compute electric field vector
So, now all that is left is to sum everything up. We are summing over the circumference of a circle, so our path is defined by [math]\displaystyle{ 0\leq\theta\leq 2\pi }[/math]. Let us now set up our integral.
[math]\displaystyle{ \vec{E}=\int_{0}^{2\pi}\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} d\theta=\int_{0}^{2\pi}\frac{1}{4\pi\epsilon_{0}}\frac{Q}{2\pi(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z})d\theta }[/math]
Since both sine and cosine are [math]\displaystyle{ 2\pi }[/math] periodic functions, the [math]\displaystyle{ x }[/math] and [math]\displaystyle{ y }[/math] components of [math]\displaystyle{ \vec{E} }[/math] go to [math]\displaystyle{ \vec{0} }[/math], which is very convenient. The result is
[math]\displaystyle{ \vec{E}=\frac{1}{4\pi\epsilon_{0}}\frac{Qz}{(z^{2}+R^{2})^{3/2}}\hat{z} }[/math].
Remark
If the path we are interested in is over a half circle, third-circle or quarter-circle, or indeed any circular section, simply adjust the bounds of integration and the charge density to the ones required by the curve of interest.
Example Problems
Straightforward
Find the function [math]\displaystyle{ E(x) }[/math] that represents the magnitude of the electric field along the center axis due to a uniformly charged ring of radius 0.04 m with total charge 8 C.
Solution
We can use the derived formula for the electric field due to a charged ring. Only the horizontal components of the electric field will remain as the rest will cancel out.
[math]\displaystyle{ E(x) = \frac{1}{4\pi\epsilon_{0}}\frac{(8 C)*x}{((0.04 m)^2 + x^2)^\frac{3}{2}} }[/math]
A Bit More Thinking
Find the electric field at a distance [math]\displaystyle{ z }[/math] along the center axis away from a uniformly charged semicircular ring of radius R and total charge Q.
Solution
We can tweak the same integral for a uniformly charged ring by changing the limits of integration.
[math]\displaystyle{ \vec{E}=\int_{0}^{\pi}\frac{1}{4\pi\epsilon_{0}}\frac{q}{|\vec{r}|^{2}}\hat{r} d\theta=\int_{0}^{\pi}\frac{1}{4\pi\epsilon_{0}}\frac{Q}{\pi(R^{2}+z^{2})^{3/2}}(Rcos(\theta)\hat{x}+Rsin(\theta)\hat{y}+z\hat{z})d\theta }[/math]
[math]\displaystyle{ \vec{E} = \frac{1}{4\pi\epsilon_{0}}\frac{Q}{\pi(R^{2}+z^{2})^{3/2}}(0\hat{x}+2R\hat{y}+{\pi}z\hat{z}) }[/math]
Connectedness
The idea of charge density is somewhat analogous to the idea of the mass density, which is useful in a variety of contexts, including the computation of the center of mass, the first and second moments of mass, which are useful in statics and rigid body dynamics. Instead of computing the uniform distribution of the mass of this ring, we are computing the uniform distribution of charge. This concept is also useful in visualizing what happens within a wire in a steady state circuit. The wire can be viewed to be a continuous length of rings of charge, which act as a channel through which electrons are transported, and that the electric field of these rings of charge pushes the electrons within the wire.
It is also important in the context of Maxwell's equations, specifically in Gauss's Law and in the Maxwell-Faraday equation, which are concerned with electron flux and induced fields, respectively.
See also
External Links/References
"Electric Field on the Axis of a Ring of Charge". University of Delaware Physics Library. Adapted from Stephen Kevan's lecture on Electric Fields and Charge Distribution. April 8, 1996. http://www.physics.udel.edu/~watson/phys208/exercises/kevan/efield1.html
Chabay, R., & Sherwood, B. (2015). Matter and Interactions (4th ed., Vol. 2, pp. 597-599). Wiley.