Figure $29-81$ shows a wire segment of length $\Delta s=3.0 \mathrm{cm},$ centered at the origin, carrying current
$i=2.0$ A in the positive $y$ direction $($ as
part of some complete circuit). To calculate the magnitude of the magnetic
field $\vec{B}$ produced by the segment at a $a$ point several meters from the origin,
we can use $B=\left(\mu_{0} / 4 \pi\right) i \Delta s(\sin \theta) / r^{2}$ as
the Biot- Savart law. This is because $r$
and $\theta$ are essentially constant over the segment. Calculate $\vec{B}$ (in unit-vector notation) at the $(x, y, z)$ coordinates (a) $(0,0,5.0 \mathrm{m}),(\mathrm{b})(0,6.0 \mathrm{m}, 0),(\mathrm{c})(7.0 \mathrm{m}, 7.0 \mathrm{m}, 0),$ and $(\mathrm{d})$
$(-3.0 \mathrm{m},-4.0 \mathrm{m}, 0)$