What is the general calculus form of the Biot-Savart Law for the magnetic field due to a current-carrying wire?
It is \(\mu_0 / (4\pi) \int (I d\vec{l} \times \vec{r}) / r^3\), where \(I\) is current, \(d\vec{l}\) is an infinitesimal wire segment, and \(\vec{r}\) is the position vector.