Physics > Electrostatics > 7.0 Electric field lines

  Electrostatics
    1.0 Introduction
    2.0 Electric charge
    3.0 Coulomb's law
    4.0 Principle of superposition
    5.0 Continuous charge distribution
    6.0 Electric field
    7.0 Electric field lines
    8.0 Insulators and conductors
    9.0 Gauss's law
    10.0 Work done
    11.0 Electric potential energy
    12.0 Electric Potential
    13.0 Electric dipole

7.2 Electric flux

Electric flux is a measure of the number of electric field lines crossing a surface.

If the electric field lines pass through a surface then the surface is said to have flux linked with it. It is given by, $$d\phi = \overrightarrow E .\,d\overrightarrow S \quad ...(i)$$
where,

$\overrightarrow E :$ Electric field
$d\overrightarrow S :$ Area vector of the small area element.

The area vector of a closed surface is always in the direction of outward drawn normal.



So, the total flux lined with whole of the body is the closed integral of equation $(i)$,
$$\phi = \oint {\overrightarrow {E\,} .\,d\overrightarrow S } $$
where,

$\oint {} :$ Represents closed integral done for a closed surface.


Note:

  • The SI unit of electric flux is $N{m^2}{C^{ - 1}}$.

  • Dimensional formula of electric flux is $\left[ {M{L^3}{T^{ - 3}}{A^{ - 1}}} \right]$.

  • Electric flux is a scalar quantity as it is a dot product of two vector quantity.

  • Electric flux is zero for a surface when electric field $\left( {\overrightarrow E } \right)$ is perpendicular to the area vector $\left( {d\overrightarrow S } \right)$ or electric field is parallel to the surface.



  • Electric flux can be negative if the angle between the electric field and the area vector is more than $\frac{\pi }{2}$.
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