In the experiment of the photoelectric effect,the stopping potential for a given metal is $V_{0}$ volts when radiation of wavelength $\lambda_{0}$ is used. If radiation of wavelength $2\lambda_{0}$ is used for the same metal,then the stopping potential (in volts) will be: [$e=$ charge on electron,$c=$ speed of light,$h=$ Planck's constant.]

  • A
    $V_{0} + \frac{hc}{2e\lambda_{0}}$
  • B
    $V_{0} - \frac{hc}{2e\lambda_{0}}$
  • C
    $\frac{V_{0}}{2}$
  • D
    $2V_{0}$

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