Electromagnetic Induction
Table of Contents
Induction Voltage
If a conductor is moved inside a magnetic field, the Lorentz force pushes the electrons to one of its ends, until the electric force compensates for the Lorentz force completely. This can be described with the help of the following equation:
$$qE = qvB$$
By canceling out the charge $q$ and replacing $E$ with $U/l$, where $l$ is the length of the conductor, it follows for the induced voltage:
$$U = lvB$$
Induction Voltage
When moving an electrical wire of the length $l$ with the speed $v$ inside a magnetic field perpendicular to the field lines, a voltage is induced that can be calculated with the following formula: $$U_\mathrm{ind} = lvB$$
Faraday's Law of Induction
Faraday's Law of Induction
This equation states that the induced voltage equals the change of the magnetic flux in time. Since either $A$ or $B$ can change with respect to time, we can apply the product rule we learned in the differential calculus section which turns to
$$U_\mathrm{ind} = A\frac{\mathrm{d}B}{\mathrm{d}t} + \frac{\mathrm{d}A}{\mathrm{d}t}B$$
It follows from this relation that if either the area or the magnetic field changes, an induced voltage can be observed.The magnetic flux of a magnetic field with the strength $B$ through the area $A$ is defined as the product of $B$ and $A$: $$\Phi = BA$$ The induced voltage into a moving conductor is then given as $$U_\mathrm{ind} = \frac{\mathrm{d}\Phi}{\mathrm{d}t}$$
This page contains 800 words and 5059 characters.
Last modified: 2023-05-22 17:28:14 by mustafa