$A$ thin non-conducting ring of radius $r$ has a linear charge density $\lambda = \lambda_0 \cos \phi$,where $\lambda_0$ is a constant and $\phi$ is the azimuthal angle. The magnitude of the electric field strength at the centre of the ring is

  • A
    $\frac{1}{4 \pi \varepsilon_0} \frac{\lambda_0}{r}$
  • B
    $\frac{1}{2 \pi \varepsilon_0} \frac{\lambda_0}{r}$
  • C
    $\frac{\lambda_0}{4 \varepsilon_0 r}$
  • D
    $\frac{\lambda_0}{2 \varepsilon_0 r}$

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