Understanding symmetry in electric field calculations

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SUMMARY

The discussion focuses on calculating the electric field above the axis of a circular ring of charge, specifically addressing how symmetry cancels the radial components of the electric field. The integral used for the electric field is given by E=\frac{1}{4\pi\epsilon_0}\int{\frac{1}{r^2}\hat{r}dq}, where the integration simplifies due to the constant radius and height. The radial components cancel out because they are equal in magnitude but opposite in direction, leading to a net zero contribution in the radial direction while maintaining a resultant field along the axial (z) direction.

PREREQUISITES
  • Understanding of electric field concepts and vector calculus.
  • Familiarity with integration techniques in physics.
  • Knowledge of symmetry principles in electrostatics.
  • Basic understanding of charge distributions and their effects on electric fields.
NEXT STEPS
  • Study the derivation of electric fields from continuous charge distributions.
  • Learn about the application of Gauss's Law in electrostatics.
  • Explore the concept of vector fields and their properties in physics.
  • Investigate the effects of different charge configurations on electric field calculations.
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Physics students, educators, and anyone interested in mastering electrostatics and electric field calculations, particularly in relation to symmetry and charge distributions.

Vaentus
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Homework Statement


Consider the specific case of a point above the axis of a circular ring of charge, how do the calculations follow to cancel the radial components? I understand the concept of the symmetry but don't understand how to express it in the expression without just removing the term.

Homework Equations


[tex]E=\frac{1}{4\pi\epsilon_0}\int{\frac{1}{r^2}\hat{r}dq}[/tex]

The Attempt at a Solution


Integration of the integral is very straight forward due to the constant radius of the circle and constant height of the point as well as that dl can be simplified to RdΦ such that dΦ is from 0 to 2π but I still have a term in the radial direction that doesn't disappear.
 
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That question has already been answered in your other thread:
Electric field above a circular loop
... note: "the radial direction" is not just one direction - it is all directions perpendicular to the axial (z) direction. Some of those directions are opposite each other.
 

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