Step 1: The magnetic field inside an infinitely long, straight, current-carrying conductor is given by Ampère's Law:
\[
\oint \vec{B} \cdot d\vec{l} = \mu_0 I.
\]
Step 2: By applying the right-hand rule, the magnetic field at points inside the pipe cancels out. Therefore, the net magnetic field at any point inside the pipe is zero.