Two straight conducting plates form an angle $\theta$ where their ends are joined. $A$ conducting bar in contact with the plates and forming an isosceles triangle with them starts at the vertex at time $t=0$ and moves with constant velocity $\vec{v}$ to the right as shown in the figure. $A$ magnetic field $\vec{B}$ points out of the page. The magnitude of the emf induced at $t=1 \text{ s}$ will be

  • A
    $Bv \tan \frac{\theta}{2}$
  • B
    $Bv^2 \tan \frac{\theta}{2}$
  • C
    $2 Bv^2 \tan \frac{\theta}{2}$
  • D
    $2 Bv^2 \sin \frac{\theta}{2}$

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