If a unit test positive charge Qt is placed at any point in this field, it experiences a repulsive force and tends to move in the direction of the force.
Work Done
•
The electric field intensity is defined as the force on a unit test charge at
that point at which we want to find the value of . Consider an
electric field due to a positive charge Q. If a unit test positive charge Qt
is placed at any point in this field, it experiences a repulsive force and
tends to move in the direction of the force.
•
But if a positive test charge Qt is to be moved towards the positive
base charge Q then it is required to be moved against the electric field of the
charge Q. i.e. against the repulsive force exerted by charge Q on the test
charge Qt. While doing so, an external source has to do work to move
the test charge Qt against the electric field. This movement of charge requires
to expend the energy. This work done becomes the potential energy of the test
charge Qt, at the point at which it is moved.
•
Consider an earth's gravitational field. An object falls on the earth due to
the force exerted by earth's gavitational field. But to move an object away
from the earth's gravitational field, the work is required to be done by an
external source. The force in opposite direction to that exerted by earth's
gravitational field is required to be applied, to move an object against the
earth's gravitational field. In such a case, work is said to be done.
•
Thus, work is said to be done when the test charge is moved against the
electric field.
•
Consider a positive charge Q1 and its electric field If a
positive test charge Qt is placed in this field, it will move due to
the force of repulsion. Let the movement of the charge Qt is dl. The
direction in which the movement has taken place is denoted by unit vector
, in the direction of dl. This is shown Fig. 4.2.1
•
According to Coulomb's law the force exerted by the field is
given by,
•
But the component of this force exerted by the field in the direction of dl, is
responsible to move the charge Qt, through the distance dl.
•
We know that the component of a vector in the direction of the unit vector is
the dot product of the vector with that unit vector. Thus the component of in the direction of unit vector
is given by,
•
This is the force responsible to move the charge Qt through the distance dZ, in
the direction of the field.
•
To keep the charge in equilibrium, it is necessary to apply the force which is
equal and opposite to the force exerted by the field in the direction dl.
•
In this case, the work is said to be done.
Key
Point : Thus keeping the charge in equilibrium means we are
moving a charge Qt, through the distance dl in opposite direction to
that of field . Hence the work is done.
•
Thus there is expenditure of energy which is given by the product of force and
the distance.
•
Hence mathematically the differential work done by an external source in moving
the charge Qt through a distance dl, against the direction of field is given by,
Key
Point : Note that dW is a scalar quantity as is the dot product which is a scalar quantity.
•
Thus if a charge Q is moved from initial position to the final position,
against the direction of electric field then the total work done
is obtained by integrating the differential work done over the distance from
initial position to the final position.
The
work done is measured in Joules.
Key
Point : Note that at both the positions initial and final,
the charge Q is at rest and not moving, then only the equation (4.2.7) is
valid.
Review
Question
1.
Define a work done and obtain the line integral to calculate the work done in
moving a point charge Q in an electric field .
AU
: May-05, 10, 19, Dec.-19
Electromagnetic Theory: Unit II: (a) Electric Work Potential and Energy : Tag: : Electric Work Potential and Energy - Work Done
Electromagnetic Theory
EE3301 3rd Semester EEE Dept | 2021 Regulation | 3rd Semester EEE Dept 2021 Regulation