Calculating the Electric field for a ring

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SUMMARY

The discussion focuses on calculating the electric field for a charged ring by utilizing the superposition principle. Participants clarify that a uniformly charged ring can be effectively replaced with two oppositely charged disks, simplifying the problem. The total charge distribution must be normalized to a total charge Q, and while a double integral can be used for calculations, symmetry allows for a simpler single integral approach. The conversation emphasizes the importance of understanding charge distributions and their impact on electric field calculations.

PREREQUISITES
  • Understanding of electric fields and charge distributions
  • Familiarity with the superposition principle in electrostatics
  • Knowledge of integration techniques, particularly double integrals
  • Concept of normalization in charge distributions
NEXT STEPS
  • Study the superposition principle in electrostatics
  • Learn how to calculate electric fields from charged disks
  • Explore the process of normalizing charge distributions
  • Practice solving double integrals in the context of electric fields
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Students and professionals in physics, particularly those focusing on electromagnetism, as well as educators seeking to explain electric field calculations involving charged distributions.

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Homework Statement
(II) A flat ring (inner radius R outer radius 4R ) is
uniformly charged. In terms of the total charge Q, determine the electric field on the axis at points (a) 0.25R and (b) 0.75R from the center of the ring. [Hint: The ring can be
replaced with two oppositely charged superposed disks.]
Relevant Equations
Gauss' Law
What i don't understand is why we are able to replace the ring with 'two oppositely charged superposed disks'?

Just trying to understand..
So we have a uniform charge which means that this'll just be a simplification of the problem than, correct?

Thanks in advance.
 
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By the superposition principle, the solution to the sum of two charge distributions is the sum of the solutions to the separate charge distributions. If you take a small disk and a large disk with the opposite surface charge density (not charge!) then the sum of the charge distributions is an annulus as described in the problem as the resulting charge distribution within R is zero and between R and 4R there will only be the larger disc. Make sure to normalise your charge distribution such that the total charge distribution is of total charge Q.
 
To me, the hint makes sense if the on-axis electric field due to a uniformly disk is assumed as given and there is no requirement to derive it. If there is such a requirement, I think doing the double integral would be simpler.
 
kuruman said:
I think doing the double integral would be simpler.
Well, the double integral is also relatively easily written as a single integral just by symmetry arguments, making that approach even simpler. However, the difference in complexity is inserting zero twice in the primitive function (which evaluates to zero if you use the most convenient choice of integration constant).
 

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