Question:

A current carrying closed loop in the form of a right isosceles triangle \(XYZ\) is placed in a uniform magnetic field \(B\) acting along \(XY\) of the loop. If the magnetic force on the arm \(YZ\) is \(\sqrt{2}F\), then the force on the arm \(XZ\) is:

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The net magnetic force on a closed current loop placed in a uniform magnetic field is always zero.
Updated On: May 6, 2026
  • \(-\sqrt{2}F\)
  • \(\frac{F}{\sqrt{2}}\)
  • \(+2\sqrt{2}F\)
  • \(-F\)
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The Correct Option is A

Solution and Explanation

Step 1: Use magnetic force on a current carrying wire.
\[ F = I l B \sin\theta \]
where \(\theta\) is the angle between length of conductor and magnetic field.

Step 2: Force on arm \(XY\).

Since magnetic field is along \(XY\),
\[ \theta = 0^\circ \]
\[ F_{XY} = I l B \sin 0^\circ = 0 \]

Step 3: Force on arm \(YZ\).

Arm \(YZ\) is perpendicular to \(XY\), so it is perpendicular to magnetic field.
\[ F_{YZ} = IB(YZ)\sin 90^\circ \]
Given,
\[ F_{YZ} = \sqrt{2}F \]

Step 4: Use net force condition on closed loop.

In a uniform magnetic field, the net magnetic force on a closed current loop is zero.
\[ F_{XY} + F_{YZ} + F_{XZ} = 0 \]

Step 5: Substitute known force.

\[ 0 + \sqrt{2}F + F_{XZ} = 0 \]

Step 6: Solve for force on \(XZ\).

\[ F_{XZ} = -\sqrt{2}F \]

Step 7: Final answer.

\[ \boxed{-\sqrt{2}F} \]
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