The threshold wavelength of a photosensitive material is equal to the frequency of H$_\alpha$ line of hydrogen. If a photon whose frequency equal to the frequency of H$_\beta$ line of hydrogen is incident on this photosensitive material, the maximum kinetic energy of the emitted photoelectrons is:
(R -- Rydberg's constant, h -- Planck's constant and c -- speed of light in vacuum)
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For hydrogen spectral lines, use the Balmer series formula:
\[
\nu = Rc \left( \frac{1}{2^2} - \frac{1}{n^2} \right)
\]
and apply the photoelectric equation:
\[
K.E._{\max} = h\nu_{\text{incident}} - h\nu_{\text{threshold}}
\]