As shown in the figure, let the conductor Y carry current i2, situated in a magnetic field perpendicular to its length. It therefore, experiences a magnetic force, the magnitude of the force acting on a length l of Y is F=i2Bl=i2(2πμ0Ri2)l
From Fleming's left hand rule the direction of this force is towards X. Similarly, force per unit length of X due to Y is directed opposite to Y. Hence, the conductors attract each other.