Equipotential surface
Equipotential surface: Any surface that has same electric potential at every point on the surface of the conductor known as equipotential surface.
Properties of equipotential surface:
- No work is done in moving test charge over an equipotential surface:
If the test charge q0 is moved from A to B, the work done will be
WAB = charge * potential difference
= q0 (VB - VA)
As the surface is equipotential, so VB – VA = 0
Hence work done is zero.
- Electric field is always normal to the equipotential surface at every point: If the field is not normal to the equipotential surface, it would have non zero component along the surface. So to move a test charge against this component, work has to be done but no work is required to move a test charge along the surface. So the electric field must be normal to the equipotential surface.
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Equipotential surfaces are closer together in the regions of strong field and farther apart in the regions of weak field:
- , thus the spacing between the equipotential surface will smaller in the region, where electric field is stronger and vice-versa.
- No two equipotential surfaces can intersect each other: If they intersect, then there will be two values of electric potential at the point of intersection, which is impossible.
Equipotential surfaces of a various charge systems.
- Equipotential surface of positive point charge: The equipotential surface of a single point charge are concentric spherical shells with their centres at point charge. The lines of force are radially outwards, so they are perpendicular to the equipotential surface.
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Equipotential surfaces of two equal and opposite point charges: Electric dipole: These are close together in the region in between the two charges.
- Equipotential surfaces of two equal positive charges:The equipotential surfaces are far apart in the regions in between the two charges, indicating aweak field in such regions.
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Equipotential surfaces for a uniform electric field: The lines of force are parallel straight lines and equipotential surface are equidistant parallel planes perpendicular to the lines of force.
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