Lenz's Law and Conservation of Energy
Lenz's Law, formulated by Heinrich Friedrich Lenz in 1834, specifies that the polarity of the induced emf in a circuit is such that it generates a current opposing the change in magnetic flux through that circuit. This law is represented in equations by the negative sign in Faraday’s law of electromagnetic induction, suggesting that induced currents work against the very cause of their induction.
For instance, if a bar magnet's North pole approaches a coil, the induced current flows in a direction that produces a magnetic field opposing the increase in flux caused by the magnet. Conversely, if the magnet is withdrawn, the current direction reverses to counteract the decrease in magnetic flux.
Open circuits also experience induced emf due to changing magnetic flux, though no current flows. The significance of Lenz's law lies in its alignment with the conservation of energy principle, as it discourages the existence of perpetual motion machines by demanding that work must be done to move magnets against induced currents. Energy is dissipated as Joule heating in the process. This interplay highlights the interconnected nature of electricity and magnetism, and reinforces foundational principles in electromagnetism.