$A$ 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
    $\frac{\mu_0 I (y\hat{i} - x\hat{j})}{2\pi (x^2 + y^2)}$
  • B
    $\frac{\mu_0 I (x\hat{i} + y\hat{j})}{2\pi (x^2 + y^2)}$
  • C
    $\frac{\mu_0 I (x\hat{j} - y\hat{i})}{2\pi (x^2 + y^2)}$
  • D
    $\frac{\mu_0 I (x\hat{i} - y\hat{j})}{2\pi (x^2 + y^2)}$

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