Question:

A square current carrying loop is suspended in a uniform magnetic field acting in the plane of the loop. If the force on one arm of the loop is $\overrightarrow{F}$ .the net force on the remaining three arms of the loop is

Updated On: Jun 27, 2024
  • $3\vec{F}$
  • $-\vec{F}$
  • $-3\vec{F}$
  • $\vec{F}$
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The Correct Option is B

Solution and Explanation

When a current carrying loop is placed in a magnetic field, the coil experiences a torque given by $\tau=N B i A \sin \theta$. Torque is maximum when $\theta=90^{\circ}$, i.e., the plane of the coil is parallel to the field $\tau_{\max }=N B i A$ Forces $\overrightarrow{ F }_{1}$ and $\overrightarrow{ F }_{2}$ acting on the coil are equal in magnitude and opposite in direction. As the forces $\overrightarrow{ F }_{1}$ and $\overrightarrow{ F }_{2}$ have the same line of action their resultant effect on the coil is zero. The two forces $\overrightarrow{ F }_{3}$ and $\overrightarrow{ F }_{4}$ are equal in magnitude and opposite in direction. As the two forces have different lines of action, they constitute a torque. Thus, if the force on one arc of the loop is $\overrightarrow{ F }$, the net force on the remaining three arms of the loop is $- \vec{F}$.
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Concepts Used:

Moving Charges and Magnetism

Moving charges generate an electric field and the rate of flow of charge is known as current. This is the basic concept in Electrostatics. Another important concept related to moving electric charges is the magnetic effect of current. Magnetism is caused by the current.

Magnetism:

  • The relationship between a Moving Charge and Magnetism is that Magnetism is produced by the movement of charges.
  • And Magnetism is a property that is displayed by Magnets and produced by moving charges, which results in objects being attracted or pushed away.

Magnetic Field:

Region in space around a magnet where the Magnet has its Magnetic effect is called the Magnetic field of the Magnet. Let us suppose that there is a point charge q (moving with a velocity v and, located at r at a given time t) in presence of both the electric field E (r) and the magnetic field B (r). The force on an electric charge q due to both of them can be written as,

F = q [ E (r) + v × B (r)] ≡ EElectric +Fmagnetic 

This force was based on the extensive experiments of Ampere and others. It is called the Lorentz force.