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# 1.6.4: Field on the Axis of and in the Plane of a Charged Ring

Field on the axis of a charged ring.

Ring, radius a, charge Q. Field at P from element of charge $$δQ = \frac{\delta Q}{4\pi\epsilon_0 (a^2+z^2)}$$. Vertical component of this $$= \frac{\delta Q \cos theta}{4\pi\epsilon_0 (a^2+z^2)}=\frac{\delta Qz}{4\pi\epsilon_0 (a^2+z^2)^{3/2}}$$. Integrate for entire ring:

Field $$E = \frac{Q}{4\pi\epsilon_0}\frac{z}{(a^2+z^2)^{3/2}}$$.

In terms of dimensionless variables:

$$E=\frac{z}{(1+z^2)^{3/2}}$$,

where E is in units of $$\frac{Q}{4\pi\epsilon_0 a^2}$$, and z is in units of a.

From calculus, we find that this reaches a maximum value of $$\frac{2\sqrt{3}}{9}=0.3849$$ at $$z=1/\sqrt{2}=0.7071$$.

It reaches half of its maximum value where $$\frac{z}{(1+z^2)^{3/2}}=\frac{\sqrt{3}}{9}$$.

That is, $$3-72Z+9Z^2+3Z^2=0$$, where $$Z=z^2$$.

The two positive solution are $$Z = 0.041889 \text{ and }3.596267$$.

That is, $$z = 0.2047 \text{ and }1.8964$$.

Field in the plane of a charged ring.

We suppose that we have a ring of radius a bearing a charge Q. We shall try to find the field at a point in the plane of the ring and at a distance $$r (0 ≤ r < a)$$ from the centre of the ring.

Consider an element δθ of the ring at P. The charge on it is $$\frac{Q\delta \theta}{2\pi}$$. The field at A due this element of charge is

$$\frac{1}{4\pi\epsilon_0}\cdot \frac{Q\delta\theta}{2\pi}\cdot \frac{1}{a^2+r^2-2ar\cos \theta}=\frac{Q}{4\pi\epsilon_0 .2\pi a^2}\cdot \frac{\delta\theta}{b-c\cos \theta}$$,

where $$b=1+r^2/a^2$$ and $$c = 2r / a$$. The component of this toward the centre is

$$-\frac{Q}{4\pi\epsilon_0 .2 \pi a^2}\cdot\frac{\cos \phi \delta\theta}{b-c\cos \theta}$$.

To find the field at A due to the entire ring, we must express $$\phi$$ in terms of θ, r and a, and integrate with respect to $$θ \text{ from }0 \text{ to }2π$$ (or from $$0 \text{ to }π$$ and double it). The necessary relations are

$p^2=a^2+r^2-2ar\cos \theta$

$\cos \phi = \frac{r^2+p^2-a^2}{2rp}.$

The result of the numerical integration is shown below, in which the field is expressed in units of $$Q/(4\pi\epsilon_0 a^2)$$ and r is in units of a.