In photoelectric effect experiment, the stopping potential for a given metal is \(\mathrm{V}_0\) (in volt) when radiation of wavelength \(\lambda_0\) is used. If radiation of wavelength \(5 \lambda_0\) is used with the same metal, then the stopping potential is (in volt) ( \(\mathrm{h}=\) Planck's constant, \(\mathrm{c}=\) velocity of light, \(\mathrm{e}=\) electronic charge)