Figure $29-81$ shows a wire segment of length $\Delta s=3.0 \mathrm{~cm},$ centered at the origin, carrying current $i=2.0 \mathrm{~A}$ in the positive $y$ direction $(\mathrm{as}$ part of some complete circuit). To calculate the magnitude of the magnetic field $\vec{B}$ produced by the segment at 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 $(a)(0,0,5,0 m),(b)(0,6.0 m, 0),$ (c) $(7.0 \mathrm{~m}, 7.0 \mathrm{~m}, 0),$ and (d) $(-3.0 \mathrm{~m},-4.0 \mathrm{~m}, 0)$