Q.
A current carrying circular loop of radius R is placed in the x−y plane with centre at the origin. Half of the loop with x>0 is now bent so that it now lies in the y−z plane
For a circular loop of radius R carrying current I placed in x−y plane, the magnetic moment M=I×πR2. It acts perpendicular to the loop i.e., along z-direction. When half of the current loop is bent in y−z plane, then magnetic moment due to half current loop in x−y plane, M1=I(πR2/2) acting along z-direction. Magnetic moment due to half current loop in y−z plane, M2=I(πR2/2) along x -direction.
Effective magnetic moment due to entire bent current loop, M′=M12+M22 =(IπR2/2)2+(IπR2/2)2 =2IπR22<M
i.e., magnetic moment diminishes.