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QJEEAdv15Ph7f41: JEE Advanced 2015 Physics - Class 12 JEEAdv15Ph7f41 Solution: A conductor (shown in the figure) carrying constant current I…

A conductor (shown in the figure) carrying constant current I is kept in the x-y plane in a uniform magnetic field B. If F is the magnitude of the total magnetic force acting on the conductor, then the correct statements is/are
JEE Advanced 2015 Paper 1 Offline Physics - Magnetism Question 35 English

Multiple Choice Options

  • A if B is along z^\widehat z , F ∝\propto (L + R)
  • B if B is along x^\widehat x , F = 0
  • C if B is along y^\widehat y , F ∝\propto (L + R)
  • D if B is along z^\widehat z , F = 0

Step-by-Step Verified Solution

The force on a conducting element of length dl→d\overrightarrow l , carrying a current I in a magnetic field B→\overrightarrow B , is given by d F→\overrightarrow F = I d l→\overrightarrow l ×\times B→\overrightarrow B . If the field is uniform, the total force on the conductor is given by

F→=∫agIdl→×B→=I(∫agdl→)×B→=I ag→×B→\overrightarrow F = \int_a^g {Id\overrightarrow l \times \overrightarrow B = I\left( {\int_a^g {d\overrightarrow l } } \right) \times \overrightarrow B = I\,\overrightarrow {ag} \times \overrightarrow B }

JEE Advanced 2015 Paper 1 Offline Physics - Magnetism Question 35 English Explanation

Note that B→\overrightarrow B is taken out of the integral sign because it is constant. The vector ag→=2(L+R)x^\overrightarrow {ag} = 2(L + R)\widehat x . The magnetic forces on the conductor in the given cases are

Case (A) : F→=I(2(L+R)x^)×(Bz^)\overrightarrow F = I(2(L + R)\widehat x) \times (B\widehat z)

=−2IB(L+R)y^= - 2IB(L + R)\widehat y

Case (B) : F→=I(2(L+R)x^)×(Bx^)=0→\overrightarrow F = I(2(L + R)\widehat x) \times (B\widehat x) = \overrightarrow 0

Case (C) : F→=I(2(L+R)x^)×(By^)\overrightarrow F = I(2(L + R)\widehat x) \times (B\widehat y)

=2IB(L+R)z^= 2IB(L + R)\widehat z

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