Dipole (electrical) and Electric Field Concept

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SUMMARY

The discussion clarifies the concept of electric dipoles, which consist of two point charges of equal magnitude but opposite signs separated by a distance. It emphasizes that the electric field (E) at a point along the dipole axis, specifically when the dipole is oriented along the z-axis, will also point in the z-direction. This is explained through the principle of superposition, where the vector addition of the fields from each charge determines the resultant direction. The confusion arises from the distinction between fields along the dipole axis and those in the x-y plane.

PREREQUISITES
  • Understanding of electric dipoles and their properties
  • Familiarity with the principle of superposition in electric fields
  • Basic knowledge of vector addition in physics
  • Concept of electric field directionality
NEXT STEPS
  • Study the mathematical representation of electric dipoles
  • Learn about the principle of superposition in electric fields
  • Explore vector addition techniques in physics
  • Investigate the behavior of electric fields in different geometrical arrangements
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Students of physics, educators explaining electric field concepts, and anyone seeking to deepen their understanding of electric dipoles and their effects in electrostatics.

wk1989
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Hi all, I'm kind of confused right now about some concepts.

- Dipoles are essentially point charges of the same magnitude but different signs that are a certain distance away from each other, right?

-In my textbook, they were calculating a charged particle that is on the dipole axis. They got an a E that is in the direction of z (as opposed to x/y). Why is the direction of the electric field at the point P (on the dipole axis) z? The charges of the dipole and the charge at P are all on x, y plane, unless I misunderstood something.

-However, in earlier examples with charges on the same plane with other charges, the E they got was restricted in the x,y plane.

Why is this so? Am I missing something?

Thanks in advance!
 
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If the dipole axis is in the direction of z, then the field at a point on the axis will also point along the z direction. You can understand this using the principle of superposition. Work out what the field due to each charge will be and add them (vector addition).
 
The dipole axis is a line going through both charges. If that axis is the z-axis, then the field at some point along the z-axis will be parallel to the z-axis. On the other hand, the field at some point on the x-y plane that bisects the dipole (assume the dipole is at z = 0) will also be parallel to the z-axis.

(dx beat me too it!)
 
Never mind, I misunderstood what the textbook was saying, thanks for the input though.
 

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