Unveiling the Magnetic Force Between Parallel Conductors
We calculate the force per unit length between two infinite parallel current-carrying wires using Ampère's law and the Lorentz force, and discuss how this result once defined the ampere.
Ampère's law,
\[\nabla\times\mathbf{B}\left(\mathbf{r}\right)=\mu_{0}\mathbf{j}\left(\mathbf{r}\right)\]
relates the magnetic induction \(\mathbf{B}\left(\mathbf{r}\right)\) to the current distribution \(\mathbf{j}\left(\mathbf{r}\right)\).
In this section we will learn the basic techniques to calculate the magnetic induction for a given current distribution. We will use integral methods like the law of Biot-Savart or differential methods for certain symmetries to solve Ampère's law directly.
We calculate the force per unit length between two infinite parallel current-carrying wires using Ampère's law and the Lorentz force, and discuss how this result once defined the ampere.
What happens if we take a wire, drill a hole in it and set some current in motion? Will we encounter a magnetic field?
The magnetic field of a thin and infinitely long wire is calculated using Biot-Savart's law.
We calculate the magnetic field of a wire with constant current. Using symmetries we verify the right-hand rule.
The magnetic field for a current distribution in form of a cylinder shell is determined.
Helmholtz coils are a devices that can provide a very homogeneous magnetic field. Let's find an approximation for their magnetic field!
Through physical reasoning we find that the spin of the electron cannot be explained by a classical rotation.