Calculating electric fields due to continuous charge distributions

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SUMMARY

The discussion focuses on calculating electric fields due to continuous charge distributions, specifically for a linear semicircular rod with a linear charge density λ. The initial attempt to derive the electric field at the origin involved the equation dE = (adθλ)/(4πε₀a), which raised questions about the absence of a² in the denominator. The final result of the integral was confirmed to be E = (λsinφ)/(2πε₀), highlighting that the correct formulation requires a² for dimensional consistency. The conversation emphasizes the importance of unit checks and understanding the geometry of the charge distribution.

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  • Understanding of electric fields and charge distributions
  • Familiarity with calculus, specifically integration techniques
  • Knowledge of electrostatics, including Coulomb's law
  • Basic concepts of linear charge density (λ) and its implications
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  • Study the derivation of electric fields from continuous charge distributions
  • Learn about the application of integration in electrostatics problems
  • Explore the concept of linear charge density and its effects on electric fields
  • Review the principles of dimensional analysis in physics equations
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Students and educators in physics, particularly those focusing on electromagnetism and electrostatics, as well as anyone tackling problems involving continuous charge distributions.

al_famky
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calculating electric fields due to continuous charge distributions?

a question I came across doing some electric field questions, and the answer was really confusing.

Homework Statement


Charge is distributed along a linear semicircular rod with a linear charge density λ as in picture attatched. Calculate the electric field at the origin

Homework Equations




The Attempt at a Solution


for the first question, the magnitude of E was calculated with dE=\frac{adθλ}{4\pi\epsilon_{0}a}, but why is there only one "a" in the denominator, not a^{2}? The final result was this equation \int^{\phi}_{-\phi}\frac{λcosθdθ}{4\pi\epsilon_{0}}=\frac{λsin\phi}{2\pi\epsilon_{0}} which makes sense only if the "a" was dropped.
Thanks to anyone who'd be willing to explain the answers!
 
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Did you forget to attach the picture? Maybe I'm just stupid and don't know how to find it. I would want to make sure I understand the question correctly. The integral in your "attempt" goes from -\phi to +\phi. That makes me think that the rod is only a semicircle when \phi = \pi / 2. I'm guessing that's why it's called "semicircular" rather than "a semicircle". Is that correct?

Other than that, you're absolutely correct. It should be a^2 in the denominator of dE because otherwise the units are not even correct. As it is, the answer you've quoted has units of charge per unit length, which is the unit of electric potential, not electric field.

Finally, I'm assuming you understand where the factor of cos\theta in the integral comes from since you didn't ask about it specifically.
 
my apologies, I thought i did upload the picture.
But you got the gist of the problem from the without the picture anyways.
Unit check, the fundamental approach to going over problems---why didn't I think of that?
I do understand the cosθ, thanks for asking

Thank you for taking the time to reply!
 

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