For perpendicular wires, use Pythagoras theorem to find the resultant magnetic field when fields due to each wire are perpendicular components into the same direction (e.g., into the page).
The Biot–Savart law in vector form is expressed as:
\[
\vec{B} = \frac{\mu_0}{4\pi} \int \frac{I \, d\vec{l} \times \hat{r}}{r^2}
\]
The variables are defined as:
- \( \vec{B} \) represents the magnetic field.
- \( \mu_0 \) denotes the permeability of free space.
- \( I \) is the electric current.
- \( d\vec{l} \) is an infinitesimal vector element of the wire carrying the current.
- \( \hat{r} \) is the unit vector pointing from the current element to the point where the magnetic field is being calculated.
- \( r \) is the scalar distance between the current element and the field point.
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