Electric Field of a Uniformly Charged Disc at Large Distances

In summary, the equation for the electric field of a disc with radius a and surface charge density σ is given by E = (σ/2ε)(1 - 1/√(a^2/x^2 + 1)). When x is much greater than a, the term (a^2/x^2) becomes very small and can be approximated using a binomial approximation, resulting in a non-zero value for E.
  • #1
whatisreality
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Homework Statement


What is the field of a disc radius a, uniformly charged with surface charge density σ, for x>>a?

Homework Equations

The Attempt at a Solution


I've worked out the equation for the field of a disc:
##E = ## ##\frac{\sigma x}{2 \epsilon}## ##\frac{\sqrt{a^2+x^2}-x}{x \sqrt{a^2+x^2}}##

I'm also given a hint, which is that the answer shouldn't be zero. As far as I can tell, if x>>a, this definitely becomes zero! I have looked up my answer for E and it is right. To work out E for x>>a, I essentially ignored all a as irrelevant - is that wrong?

##E = ## ##\frac{\sigma x}{2 \epsilon}## ##\frac{\sqrt{x^2}-x}{x \sqrt{x^2}}## is most definitely zero!
 
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  • #2
For a finite value of ##x## that is much greater than ##a##, ##E## will be small but it won't be zero. You have "over approximated". In this type of problem, you want to keep the lowest order nonzero approximation.

Instead of approximating ##\sqrt{x^2+a^2}## in the numerator as ##\sqrt{x^2}##, find a more accurate approximation in terms of the small quantity ##a/x##.
Hint: https://en.wikipedia.org/wiki/Binomial_approximation

You might find it easier to first simplify your expression for E by cancelling some ##x##'s and splitting the fraction involving the square roots into the difference of two fractions. You will then have only one square root to worry about.
 
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  • #3
Simplifying the expression gives

##E = \frac{\sigma}{2\epsilon}(1 - \frac{1}{\sqrt{\frac{a^2}{x^2}+1}})##
And then use a binomial approximation for ##\sqrt{\frac{a^2}{x^2}+1}##.
Thank you, gave the right answer :)
 

FAQ: Electric Field of a Uniformly Charged Disc at Large Distances

1. What is the equation for the electric field of a disc?

The electric field of a disc can be calculated using the equation E = (σ/2ε0) * (1 - (z/√(z2 + R2))), where σ is the surface charge density, ε0 is the permittivity of free space, z is the distance from the center of the disc, and R is the radius of the disc.

2. How does the electric field of a disc vary with distance from the center?

The electric field of a disc is strongest at the center and decreases as the distance from the center increases. This can be seen in the equation E = (σ/2ε0) * (1 - (z/√(z2 + R2))). As z approaches infinity, the electric field approaches 0.

3. Does the electric field of a disc depend on the disc's charge?

Yes, the electric field of a disc is directly proportional to the surface charge density (σ) of the disc. This means that the stronger the charge on the disc, the stronger the electric field will be.

4. How does the electric field of a disc compare to that of a point charge?

The electric field of a disc and a point charge have different characteristics. While the electric field of a point charge is spherically symmetrical, the electric field of a disc is only symmetrical along the axis perpendicular to the disc. Additionally, the strength of the electric field of a disc varies with distance, while the electric field of a point charge remains constant at any distance.

5. Can the electric field of a disc be negative?

Yes, the electric field of a disc can be negative. This can occur if the surface charge density (σ) is negative, which would result in the electric field being directed towards the disc rather than away from it. However, in most cases, the electric field of a disc is positive, as the surface charge density is usually positive.

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