Step 1: Concept
The magnetic field at a distance r from a long straight wire carrying current I is given by $B = \frac{\mu_{0}I}{2\pi r}$. The direction of the field is determined by the right-hand thumb rule.
Step 2: Meaning
Let the distance between the two parallel wires be $2d$. The midpoint is at a distance $d$ from both wires. Since the currents flow in the same direction, their magnetic fields at the midpoint oppose each other.
Step 3: Analysis
The magnetic field due to the first wire is $B_{1} = \frac{\mu_{0}I}{2\pi d}$ (pointing in one direction). The magnetic field due to the second wire is $B_{2} = \frac{\mu_{0}(2I)}{2\pi d} = 2B_{1}$ (pointing in the opposite direction). The net magnetic field $B$ is the difference between them: $B = B_{2} - B_{1} = 2B_{1} - B_{1} = B_{1}$. When the 2I wire is switched off, $B_{2}$ becomes zero.
Step 4: Conclusion
The remaining magnetic field at the midpoint is solely due to the first wire, which is $B_{1}$. Since $B = B_{1}$, the magnitude of the field remains $B$.
Final Answer: (C)