Electric Field due to a Dipole (not on a z-axis)

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SUMMARY

The discussion focuses on calculating the electric field due to an electric dipole at a point P, located at a distance r much greater than the dipole separation d. The magnitude of the electric field is expressed as |E| = |E_y| = (2q/R)sin(θ), where R and sin(θ) are defined in terms of r and d. The electric field components from the dipole's charges cancel in the x-direction and add in the y-direction, leading to a simplified expression for the electric field. The participants emphasize the importance of temporarily introducing the angle θ for clarity in calculations.

PREREQUISITES
  • Understanding of electric dipoles and their properties
  • Familiarity with vector addition of electric fields
  • Knowledge of trigonometric functions, specifically sine
  • Basic principles of electrostatics, including Coulomb's law
NEXT STEPS
  • Study the derivation of the electric field of a dipole in detail
  • Learn about the implications of distance in electric field calculations
  • Explore the concept of dipole moments and their significance
  • Investigate the behavior of electric fields in different coordinate systems
USEFUL FOR

Students studying electromagnetism, physics educators, and anyone interested in understanding electric fields generated by dipoles.

Oijl
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Homework Statement


The figure shows an electric dipole. What is the magnitude of the dipole's electric field at point P, located at distance r >> d?

hrw7_22-38.gif



Homework Equations




The Attempt at a Solution



I suppose I could define the angle with which I could write Ey = Esin\theta, but this problem is a webassign.com problem, so it's online and I can't define anything.

The magnitude of the electric field at p due to the dipole would be very small, and I first estimated it to be zero (since the problem asks for an estimation anyway).

Without defining and using a theta, how could I represent the magnitude of the electric field?
 
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Just introduce theta temporarily. It goes away in the end since you know what it is.

The electric field vectors of the two charges add in the y direction and cancel in the x direction. Hence
<br /> |\vec E| = |E_y| = (2 q/R) \sin(\theta)<br />
where I will let you write down R and \sin(\theta) in terms of r and d.

The rest you can do.
 
loveequation said:
Just introduce theta temporarily. It goes away in the end since you know what it is.

The electric field vectors of the two charges add in the y direction and cancel in the x direction. Hence
<br /> |\vec E| = |E_y| = (2 q/R) \sin(\theta)<br />
where I will let you write down R and \sin(\theta) in terms of r and d.

The rest you can do.
In the dipole one is +ve charge and the other -ve charge.
The electric field E = 1/4πεο*q/[r2 + (d/2)2]
Their y-components cancel out and x-components add.
 
I maintain that the y components add. Think of the magnetic field lines of the Earth at the equator.
 

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