The electric field strength is determined by the distribution of electric charges and the distance from them. The electric field strength \(E\) at a point is given by:
\[ E = \frac{F}{q} \]
where \(F\) is the force experienced by a test charge \(q\). The field strength depends on the source charge and the distance from it.
Here are several contexts where the electric field strength can be weakest:
1. **Far from the Source Charge**: For a point charge, the electric field strength decreases with the square of the distance from the charge, according to Coulomb’s law. Therefore, as you move farther from the charge, the field strength becomes weaker. Mathematically, for a point charge \(Q\), the electric field \(E\) at a distance \(r\) is given by:
\[ E = \frac{kQ}{r^2} \]
where \(k\) is Coulomb’s constant. As \(r\) increases, \(E\) decreases.
2. **Between Oppositely Charged Plates**: In a parallel plate capacitor, the electric field is uniform between the plates and strongest in the region directly between them. The field strength decreases as you move away from the plates, either towards the inside of the capacitor beyond the plate edges or outside the capacitor entirely.
3. **At the Center of a Symmetrical Charge Distribution**: For some symmetrical charge distributions like a charged ring or a charged spherical shell, the electric field strength is zero or weakest at specific points. For example:
- **Charged Ring**: At the center along the axis perpendicular to the plane of the ring, the electric field is weaker.
- **Charged Spherical Shell**: Inside a uniformly charged spherical shell, the electric field is zero everywhere.
4. **Near Regions of Cancellation**: In systems with multiple charges, the electric field strength can be very weak or even zero in regions where the fields from different charges cancel each other out. For example, in a dipole field (a system with two opposite charges), there are points along the axis of the dipole where the electric field can be very weak.
5. **In a Conducting Material**: Inside a conductor in electrostatic equilibrium, the electric field is zero. This is because free charges in the conductor rearrange themselves to cancel any internal electric fields.
In summary, the electric field strength is weakest far from the source charges and at points where multiple fields cancel out. It is also weaker inside regions of certain symmetrical charge distributions or conductors in electrostatic equilibrium.