What is the Electric Field at the Origin in a Semicircle?

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SUMMARY

The electric field at the origin due to a semicircular charge distribution of radius R and total charge Q can be calculated using the principles of continuous charge distribution. The charge per unit length is defined as λ = Q/(πR). The electric field components are derived from integrating the contributions of infinitesimal charge segments, leading to Ex = 0 and Ey = -2kλ/R. Thus, the total electric field at the origin points downward with a magnitude of 2kQ/(πR²).

PREREQUISITES
  • Understanding of electric fields and Coulomb's law
  • Familiarity with continuous charge distributions
  • Knowledge of integration techniques in calculus
  • Basic concepts of vector components in physics
NEXT STEPS
  • Study the application of Gauss's law for different charge distributions
  • Learn about electric field calculations for various geometric shapes
  • Explore the concept of charge density and its implications in electrostatics
  • Review integration methods for solving physics problems involving continuous distributions
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Students studying electromagnetism, physics educators, and anyone interested in understanding electric fields generated by charge distributions.

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Homework Statement


You have a semicircle of radius R and charge Q. We also have available a test charge +qo.

Find the Magnitude and direction of the electric field at the origin.

Homework Equations


Electric Field:
F = k (Q * qo)/(R^2)
E = F/qo = kQ/R^2


The Attempt at a Solution


I'm not sure how to solve this, I assumed it would be kQ/R^2 but I am mistaken. Can someone please explain? I'm looking for an explanation on line but not having any luck
 
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Wait? The charge Q is distributed over a semicircle? I'm guessing you're going to have to use Gauss' law. But could you make the problem statement clearer? Where's the origin?
 
Sorry, I've figured it out. I just thought it was a more simple problem than this... For future reference, this is how you solve it.

It's a continuous Distribution of charge so
1) Divide the charge into segments dQ for which you already know the field
2) Find the field of each dQ
3) Find E by summing all dQ

So, the charge per unit length would be : \lambda = Q/\piR
The charge on the slice dq = \lambdaRd\theta

The field generated by the slice would be dE = k dq/R^2 = k \lambda/R d\theta

Components of dE would be: dEx = dEcos\theta, dEy = -dEsin\theta

Add them all up you get:
Ex = k\lambda/R \int from 0 to pi of cos\theta d\theta = k\lambda/R sin\theta from 0 to pi which = 0

Ey = -k\lambda/R \int from 0 to pi of sin\theta d\theta = k\lambda/R cos\theta from 0 to pi which = -2k\lambda/R
 

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