Electric Fields in circular wire

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SUMMARY

The discussion focuses on calculating the electric field at the center of a circular wire ring with a uniformly distributed positive charge, q. The user initially derived the electric field using the formula E = kq/r^2 but encountered discrepancies with the book's answer. The resolution involved substituting the uniform line charge, λ, with the correct expression λ = q/(2πr), leading to the correct formula E = (q/(4π²εr²))sin(θ/2). This highlights the importance of careful variable substitution in electrostatics.

PREREQUISITES
  • Understanding of electric fields and Coulomb's law
  • Familiarity with the concept of uniform line charge
  • Knowledge of integration techniques in physics
  • Basic proficiency in mathematical notation and symbols used in electromagnetism
NEXT STEPS
  • Study the derivation of electric fields from continuous charge distributions
  • Learn about the applications of Gauss's law in electrostatics
  • Explore the concept of electric field symmetry in various charge configurations
  • Investigate the relationship between charge density and electric field strength
USEFUL FOR

This discussion is beneficial for physics students, educators, and anyone interested in understanding electrostatics, particularly in the context of charge distributions and electric fields in circular geometries.

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I'm stumped by the following problem:

A circular ring of fine wire carries a uniformly distributed positive charge, q. Find the magnitude and direction of the electric field at the center of the ring caused by just the charge on a portion of the ring subtending an angle [the] at the center, in terms of q, [the]and radius r.

The uniform line charge [lamb] = dq/dl
l = r[the] so dl = rd[the]
dq=[lamb]rd[the]

E = kq/r^2
dE = kdq/r^2 the dE's in the y direction cancel each other out because of symmetry.
E = k[lamb]r/r^2[inte]cos[the]d[the] from -[the]/2 to [the]/2

k = 1/(4[pi][ee])

so E= [q/(2r[pi][ee]]sin([the]/2)

The book show the answer to be: [q/(4[pi]^2[ee]r^2]sin([the]/2)

Can someone please point out where I'm going wrong?

Thanks
 
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You replaced λ with q.

Your result
E= [q/(2rΠε]sin(Θ/2)

should be
E= [λ/(2rΠε]sin(Θ/2)

Now, λ = q/(2Πr) so make that substitution & you'll get the book's answer
 
Thanks Gnome.

Boy that was simple. I guess I should read more carefully. I completely forgot that for a uniform line charge [lamb] = q/l.

Thanks again.
 

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