\(\frac{2q}{ε_{0}}\)
\(\frac{2q}{ε_{0}}\)4\(\pi\)r2
infinite
Zero
\(\frac{q}{ε_{0}}\)
A hollow sphere encloses an electric dipole (+q and -q charges).
Gauss's Law
\[ \Phi = \frac{Q_{enc}}{\epsilon_0} \]
Where \( Q_{enc} \) is the net charge enclosed by the surface.
For a dipole: \( Q_{enc} = (+q) + (-q) = 0 \)
Determine Electric Flux \[ \Phi = \frac{0}{\epsilon_0} = 0 \]
1. Recall Gauss's Law:
Gauss's Law states that the net electric flux through any closed surface is equal to the total charge enclosed within the surface divided by the permittivity of free space (\(\epsilon_0\)):
\[\Phi = \frac{Q_{enclosed}}{\epsilon_0}\]
2. Determine the enclosed charge:
The electric dipole consists of two charges: +q and -q. The total charge enclosed by the hollow sphere is the sum of these two charges:
\[Q_{enclosed} = +q + (-q) = 0\]
3. Calculate the net flux:
Since the enclosed charge is zero, the net electric flux through the surface of the sphere is also zero:
\[\Phi = \frac{0}{\epsilon_0} = 0\]
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
An electric dipole is a pair of equal and opposite point charges -q and q, separated by a distance of 2a. The direction from q to -q is said to be the direction in space.
p=q×2a
where,
p denotes the electric dipole moment, pointing from the negative charge to the positive charge.
