$A$ wire carrying a steady current $I$ is kept in the $x$-$y$ plane along the curve $y=A \sin \left(\frac{2 \pi}{\lambda} x\right)$. $A$ magnetic field $B$ exists in the $z$-direction. The magnitude of the magnetic force on the portion of the wire between $x=0$ and $x=\lambda$ is

  • A
    $0$
  • B
    $2 I \lambda B$
  • C
    $I \lambda B$
  • D
    $I \lambda B / 2$

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