An infinitely long thin straight wire has a uniform linear charge density of $\frac{1}{3} ~Cm^{-1}$. The magnitude of the electric field intensity at a point $18 ~cm$ away is (given $\varepsilon_0 = 8.85 \times 10^{-12} ~C^2 N^{-1} m^{-2}$):

  • A
    $0.33 \times 10^{11} ~NC^{-1}$
  • B
    $3 \times 10^{11} ~NC^{-1}$
  • C
    $0.66 \times 10^{11} ~NC^{-1}$
  • D
    $1.32 \times 10^{11} ~NC^{-1}$

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