From the figures depicted here, for equilibrium of the small element, we have dl = Rdθ. Therefore, 2T sin (2dθ​) = BI (Rdθ)
Since dθ << sin (2dθ​) = 2dθ​ , we have T dθ = BIR dθ ⇒ T = BIR Also, it is given that L = 2πR. Hence, R = 2πL​ Therefore, T = 2πBIL​