The relation between the stopping potential $(V_0)$ and frequency $(v)$ is correctly represented in $[\phi = \text{Work function}]$

  • A
    $V_0 = \frac{\phi}{e} - \frac{hv^2}{e}$
  • B
    $V_0 = \frac{he}{v} + \frac{\phi}{e}$
  • C
    $V_0 = \frac{hv}{e} - \frac{\phi}{e}$
  • D
    $V_0 = \frac{hv}{e^2}$

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