a circular loop of radius R is kept in a uniform magnetic field pointing perpendicular into the plane of paper. when a current I flows in the loop, the tension produced in the loop is
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Let a small elementary length dl cut into circle as shown in figure, dθ is the angle subtended by dl into centre of circle . so, elementary length , dl = Rdθ
Now, F = I(dl × B)
= Idl.Bsin90° [ because elementary length are perpendicular upon magnetic field ]
= BIRdθ
Also tension acts on just opposite side of force as you can see in figure .
So, at equilibrium condition ,
2Tsindθ/2 = BIRdθ
actually, dθ/2 is very small angle so, sindθ/2 ≈ dθ/2
Hence, 2Tdθ/2 = BIRdθ
T = BIR
hence tension in the loop is BIR
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