Charging Conductors By Induction

Free electrons inside the conductor are repelled away from the charged rod. As more electrons move, they repel others already displaced, creating a distribution where no electron experiences net force. This redistribution leaves the end closer to the rod positively charged and the far end negatively charged, establishing an electric dipole.

When a polarized conductor is grounded via a metallic wire, free electrons flow to or from Earth, which acts as an infinite source or sink of charge. After removing the wire, the conductor retains a net charge opposite to the inducing charge. This permanent charge transfer distinguishes induction from temporary polarization.

A dipole consists of two oppositely charged poles. During induction, the conductor develops a positive charge at one end and negative charge at the other, creating this two-pole configuration. Although the conductor has no net charge initially, the spatial separation of opposite charges defines the dipole structure.

Earth is a good conductor and effectively an infinite source or sink of charges due to its size. When a conductor is grounded, Earth exchanges charges with it, allowing excess electrons to flow away or additional electrons to arrive. This charge exchange is essential for converting temporary polarization into permanent net charge on the conductor.

No, the inducing charged object does not lose or gain any charge during induction. The negatively charged rod, for example, remains negatively charged throughout. Induction involves only charge redistribution within the conductor and charge exchange between the conductor and Earth, not transfer from the inducing object.

Polarization occurs when a charged object redistributes free electrons in a nearby conductor without grounding, creating temporary opposite charges at each end. Permanent charging requires grounding, which allows charge to flow to or from Earth. Once the inducing object is removed, polarization disappears, but permanent charge remains on the grounded conductor.

Free electrons move until they reach a configuration where no electron experiences net attractive or repulsive force. Initially, electrons are attracted toward the positive inducing object, but as they accumulate, they repel incoming electrons. Equilibrium is reached when these opposing forces balance, stabilizing the charge distribution across the conductor.