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NEET PHYSICSEasy

A current-carrying closed loop in the form of a right-angle isosceles triangle ABC is placed in a uniform magnetic field acting along AB. If the magnetic force on the arm BC is F, the force on the arm AC is:

A

-F

B

F

C

√2F

D

-√2F

Step-by-Step Solution

  1. Net Force on a Closed Loop: The net magnetic force on any closed current-carrying loop placed in a uniform magnetic field is always zero (ecFnet=0ec{F}_{net} = 0). This is derived from the integral of the force vector I(decl×ecB)I(d ec{l} \times ec{B}) over a closed path.
  2. Force Components: For the triangular loop ABC, the total force is the vector sum of the forces on its three arms: ecFAB+ecFBC+ecFAC=0ec{F}_{AB} + ec{F}_{BC} + ec{F}_{AC} = 0
  3. Force on Arm AB: The magnetic field is acting along the arm AB. Therefore, the angle θ\theta between the current vector IeclI ec{l} and the magnetic field B\vec{B} is either 00^{\circ} or 180180^{\circ}. Since the magnetic force magnitude is F=IlBsinθF = IlB \sin\theta and sin(0)=sin(180)=0\sin(0^{\circ}) = \sin(180^{\circ}) = 0, the force on arm AB is zero (ecFAB=0ec{F}_{AB} = 0) .
  4. Calculation: Substituting ecFAB=0ec{F}_{AB} = 0 into the equilibrium equation: 0+ecFBC+ecFAC=00 + ec{F}_{BC} + ec{F}_{AC} = 0 ecFAC=FBCec{F}_{AC} = -\vec{F}_{BC}
  5. Conclusion: Given that the force on arm BC is F\vec{F}, the force on arm AC must be F-\vec{F}.
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