We know Magnetic field at centre of a coil having Current I, radius r and number of turns N is given as B=μ0NI2r
and at a distance x from the centre and on the axis is B=μ0NIx2(x2+r2) and its direction is given by right-hand screw rule i.e.
if the observer sees that the current is anticlockwise then the field will be towards the observer and vice-versa, as shown in the figure−1
Part a
Field at center O1 will be difference of field due to loop-1 and loop-2
AtO1 Bnet = μ0NI2r - μ0NIx2(x2+r2) towards observer
putting μ0=4π×10−7 ,N=6, r=.04 meter ,x= .06 meter and I = 1 all units in S.I. system
we get Bnet=5.07×10−5 Tesla towards the observer
Similarly, AtO1 the filed due to circle 2 will dominate so net filed will be
Bnet=5.07×10−5 Tesla in a direction away from the observer.
Part b
According to the above theory the field at the midpoint on the axis of joining the centres will be equal and opposite as current in loops is opposite so net field is zero there at O