$A$ long straight wire along the $z$-axis carries a current $I$ in the negative $z$-direction. The magnetic vector field $\vec B$ at a point having coordinates $(x, y)$ in the $z = 0$ plane is

  • A
    $\frac{{{\mu _0}I\,\left( {y\hat i - x\hat j} \right)}}{{2\pi \,\left( {{x^2} + {y^2}} \right)}}$
  • B
    $\frac{{{\mu _0}I\,\left( {x\hat i + y\hat j} \right)}}{{2\pi \,\left( {{x^2} + {y^2}} \right)}}$
  • C
    $\frac{{{\mu _0}I\,\left( {x\hat j - y\hat i} \right)}}{{2\pi \,\left( {{x^2} + {y^2}} \right)}}$
  • D
    $\frac{{{\mu _0}I\,\left( {x\hat i - y\hat j} \right)}}{{2\pi \,\left( {{x^2} + {y^2}} \right)}}$

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