Electric potential at the center of a dipole

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SUMMARY

The electric potential at the center of an electric dipole is definitively zero. This conclusion arises from the fact that when a charge moves along the horizontal bisector of the dipole, the electric force acting on it remains perpendicular to its direction of motion. Consequently, the work done to maintain the charge's position along this line is nullified, leading to no net work required to bring a test charge from infinity to the center of the dipole.

PREREQUISITES
  • Understanding of electric dipoles and their properties
  • Knowledge of electric potential and electric fields
  • Familiarity with the concept of work in physics
  • Basic grasp of vector forces and their components
NEXT STEPS
  • Study the mathematical derivation of electric potential for dipoles
  • Explore the concept of electric field lines and their behavior around dipoles
  • Learn about the forces acting on charges in electric fields
  • Investigate the implications of electric potential in various physical systems
USEFUL FOR

Students of physics, educators teaching electromagnetism, and anyone interested in understanding the principles of electric fields and potentials in dipole systems.

kavan
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Potential at the center of an electric dipole is zero. This doesn't make intuitive sense, how can work required to bring an arbitrary charge from infinity to the center of a dipole be zero? Imagine a charge at some distance on horizontal bisector of the dipole, it will deflect from the horizontal line and get attracted to one or the other dipole charge...that means there will be some nonzero work involved to bring test charge to the center of the dipole. Can anyone please throw some light on it?
 
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kavan said:
Imagine a charge at some distance on horizontal bisector of the dipole, it will deflect from the horizontal line and get attracted to one or the other dipole charge...that means there will be some nonzero work involved to bring test charge to the center of the dipole.

No. If the particle moves along the bisector line, the electric force on it is always perpendicular to the direction of motion. Therefore the force that you exert on the charge to counteract the electric force and keep the charge from straying from the line, does no work.
 
Oh...got it. Thanks a lot, i was stuck with it for quite some time.
 

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