Step 1: Field of a straight wire.
A long wire makes a field $B = \dfrac{\mu_{0}I}{2\pi r}$ at distance $r$. The direction is set by the right-hand rule.
Step 2: Set the midpoint distance.
Let the wires be $2d$ apart. The midpoint is $d$ from each wire.
Step 3: Fields at the midpoint.
Since the currents are in the same direction, at the midpoint their fields point opposite ways. So they subtract.
Step 4: Write each field.
Wire 1 (current $I$): $B_{1} = \dfrac{\mu_{0}I}{2\pi d}$. Wire 2 (current $2I$): $B_{2} = \dfrac{\mu_{0}(2I)}{2\pi d} = 2B_{1}$.
Step 5: Net field with both on.
\[ B = B_{2} - B_{1} = 2B_{1} - B_{1} = B_{1} \]So the given net field $B$ equals $B_{1}$.
Step 6: Switch off the $2I$ wire.
Now only wire 1 is left, giving field $B_{1}$. Since $B = B_{1}$, the field is still $B$. This is option 3.
\[ \boxed{\text{Field} = B} \]