The magnetic field at the centre O due to the current through side AB is B1=4πaμ0I[sinθ1+sinθ2]
As the magnetic field due to each of the three sides is the same in magnitude and direction. So, the total magnetic field at O is sum of all the fields.
i.e. B=3B1=4πa3μ0I[sinθ1+sinθ2]
Here, tanθ1=ODAD ⇒tan60∘=a2l ⇒a=23l=239×10−2
Now B=3×4π×239×10−24π×10−7×2[sin60∘+sin60∘] =3×943×(10)−6(23+23) =4×10−6T