A square conducting loop of side length L carries a current I. The magnetic field at the centre of the loop is
independent of L
proportional to L2
inversely proportional to L
linearly proportional to L
Magnetic field at the centre due to either arm
B= μ04π × IL/2 sin 450 + sin 450=μ04π × 22IL
Field at centre due to the four arms of the square
B=4B1 =4×μ04π × 22ILi.e., B ∝ 1L