$PQ$ and $RS$ are long parallel conductors separated by certain distance. $M$ is the mid-point between them (see the figure). The net magnetic field at $M$ is $B$ . Now, the current $2\,A$ is switched off. The field at $M$ now becomes
A$2\,B$
B$B$
C$\frac {B}{2}$
D$3\,B$
Medium
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B$B$
b $\vec {\mathrm{M}}=\mathrm{I} \vec {\mathrm{A}}$
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