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JEE Main 20257 AprilMorning Shift
Exam
JEE Main
Year
2025
Date
7 April
Shift
Morning Shift
Subject
Physics
Chapter
Magnetic Effects of Current

JEE Main 2025 · 7 April · Morning Shift · Physics · Magnetic Effects of Current

Uniform magnetic fields of different strengths (B_1. and B_2), both...

Uniform magnetic fields of different strengths (B1\left(B_1\right. and B_2), both normal to the plane of the paper exist as shown in the figure. A charged particle of mass m and charge q , at the interface at an instant, moves into the region 2 with velocityvandreturnstotheinterface.Itcontinuestomoveintoregion1andfinallyreachestheinterface.Whatisthedisplacementoftheparticleduringthismovementalongtheinterface?<br/><imgsrc="https://cdn−question−pool.getmarks.app/pyq/jeemain/GJUcZpO6YRncsChthnpFYEw−AUdwPrN0tPsqTp0K−is.original.fullsize.png"/><br/>(Considerthevelocityoftheparticletobenormaltothemagneticfieldandand returns to the interface. It continues to move into region 1 and finally reaches the interface. What is the displacement of the particle during this movement along the interface?<br/><img src="https://cdn-question-pool.Quantrex.app/pyq/jee_main/GJUcZpO6YRncsChthnpFYEw-AUdwPrN0tPsqTp0K-is.original.fullsize.png"/><br/>(Consider the velocity of the particle to be normal to the magnetic field andB_2 \gt B_1))

Options

  1. AmvqB1(1−B2 B1)×2\frac{\mathrm{mv}}{\mathrm{qB}_1}\left(1-\frac{\mathrm{B}_2}{\mathrm{~B}_1}\right) \times 2
  2. BmvqB1(1−B1 B2)\frac{\mathrm{mv}}{\mathrm{qB}_1}\left(1-\frac{\mathrm{B}_1}{\mathrm{~B}_2}\right)
  3. CmvqB1(1−B2 B1)\frac{\mathrm{mv}}{\mathrm{qB}_1}\left(1-\frac{\mathrm{B}_2}{\mathrm{~B}_1}\right)
  4. DmvqB1(1−B1 B2)×2\frac{\mathrm{mv}}{\mathrm{qB}_1}\left(1-\frac{\mathrm{B}_1}{\mathrm{~B}_2}\right) \times 2

Correct answer

D. mvqB1(1−B1 B2)×2\frac{\mathrm{mv}}{\mathrm{qB}_1}\left(1-\frac{\mathrm{B}_1}{\mathrm{~B}_2}\right) \times 2

Step-by-step solution

As v→\overrightarrow{\mathrm{v}} is ⊥\perp to B→\overrightarrow{\mathrm{B}}, so charge particle will move in circular path, whose radius is given by
R=mvqB\mathrm{R}=\frac{\mathrm{mv}}{\mathrm{qB}}
Uniform magnetic fields of different strengths (B_1. and B_2), both normal to the plane of the paper exist as shown in
Starting point →A\rightarrow \mathrm{A}
Ending point →C\rightarrow \mathrm{C}
∴\therefore Net displacement =AC=\mathrm{AC}
AC=CD−ADAC=2mvqB1−2mvqB2AC=2mvqB1[1−B1 B2]\begin{aligned} & \mathrm{AC}=\mathrm{CD}-\mathrm{AD} \\ & \mathrm{AC}=\frac{2 \mathrm{mv}}{\mathrm{qB}_1}-\frac{2 \mathrm{mv}}{\mathrm{qB}_2} \\ & \mathrm{AC}=\frac{2 \mathrm{mv}}{\mathrm{qB}_1}\left[1-\frac{\mathrm{B}_1}{\mathrm{~B}_2}\right]\end{aligned}
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