What is the work done due to a charge moving on a equipotential surface?
Work in moving a charge on a equipotential surface is zero.
What is the work done on equipotential surface?
zero
Since ΔV = 0, for equipotential surfaces, the work done is zero, W = 0. Q. 2: A positive particle of charge 1.0 C accelerates in a uniform electric field of 100 V/m. The particle started from rest on an equipotential plane of 50 V.
What is the work done in moving a charge of 10 equipotential surface?
As the potential at two points on an equipotential surfaces is same, the work done in moving a charge of 10 μ C from any point on the equipotential surface to any other point on the equipotential surface is zero.
What is the amount of work to be done to move a unit charge by unit distance on an equipotential surface in an electrostatics field justify?
Answer: The work done to move any positive charge from any point on an Equipotential surface to another point on it is zero. For Equipotential surfaces,the electric field lines are always perpendicular to the surface(means that electric field vector and the line integral vector are mutually perpendicular).
What is the amount of work done while moving 1 C charge from one point to another through a distance of 10 cm on a equipotential surface explain?
The amount of work done in moving a unit positive charge through distance of 10 cm on an equipotential surface is. Work done on equipotential surface is zero.
How much work is done by the electric field in displacing a small charge from one point to another on the equatorial line of an electric dipole Why?
At every point on equatorial axis, the potential is zero, so work done W = qΔV = 0(zero).
What is the work done in moving a charge of 10 coulomb between two points on an equipotential surface?
Textbook solution To find the work done in moving a charge of between two points on an equipotential surface.
What is the work done in moving a charge between two points on the equatorial surface?
So the work done in moving the given charge between two equipotential surfaces is equal to zero.
How do you calculate work done when moving a charge?
When charges move in an electric field, something has to do work to get the charge to move. To move q, we apply a force to just barely overcome the repulsive force from Q. Let’s work it out: The amount of work done is force times distance, W = F ⋅ d W = F \cdot d W=F⋅dW, equals, F, dot, d .
What is the amount of work done to move a unit charge by unit distance?
What is the amount of work to be done on a unit charge?
The term electric potential is the amount of work done needed to move the unit of electric charge from a given point to the specific point in the electric field.
How do you calculate work done in equipotential surface?
Work Done in Equipotential Surface. The work done in moving a charge between two points in an equipotential surface is zero. If a point charge is moved from point V A to V B, in an equipotential surface, then the work done in moving the charge is given by. W = q 0(V A –V B) As V A – V B is equal to zero, the total work done is W = 0.
What is the work done to move a charge on equipotential?
The amount of work done to move a charge on an equipotential surface is Zero. The amount of work done on a charge Q when moving it from potential V1 to V2 is (V1 – V2 ) x Q. Since on an equipotential V1 is equal to V2 the net work is zero. Please log in or register to add a comment.
What is the total work done in moving the charge?
If a point charge is moved from point V A to V B, in an equipotential surface, then the work done in moving the charge is given by As VA – VB is equal to zero, the total work done is W = 0. The electric field is always perpendicular to an equipotential surface. Two equipotential surfaces can never intersect.
What is the direction of electric field on equipotential surface?
The electric field is always perpendicular to an equipotential surface. Two equipotential surfaces can never intersect. For a point charge, the equipotential surfaces are concentric spherical shells. The direction of the equipotential surface is from high potential to low potential.