(a) We know that for Compton effect
"\\lambda ' - \\lambda = \\lambda_e (1-cos \\theta)"
where "\\displaystyle \\lambda_e = \\frac{h}{m_e c}=2.43" pm.
The energy lost by the photon during the collision is
"\\displaystyle \\frac{hc}{\\lambda} - \\frac{hc}{\\lambda'}= hc\\frac{\\lambda'-\\lambda}{\\lambda\\lambda'} \\simeq hc\\frac{\\lambda'-\\lambda}{\\lambda^2} = 12 400 \\; \\textrm{eV } \\cdot \\textrm{\u00c5} \\frac{4.86 \\cdot 10^{-2} \u00c5}{20700^2 \u00c5^2} ="
"= 12 400 \\; \\textrm{eV } \\cdot \\textrm{\u00c5} \\frac{4.86 \\cdot 10^{-2} \u00c5}{20700^2 \u00c5^2}=1.41 \\cdot 10^{-6} \\textrm{eV} = 1.41\\; \\mu \\textrm{eV}"
(b) In a photoelectric process, the entire energy of the incident photon is converted into kinetic energy of the electron
"\\displaystyle K = \\frac{hc}{\\lambda} = \\frac{12 400 \\; \\textrm{eV } \\cdot \\textrm{\u00c5}}{20700\\; \u00c5} = 0.6\\; \\textrm{eV}"
A Compton collision could not eject an electron from a metal surface since the kinetic energy "1.41\\; \\mu \\textrm{eV}" transferred to the electron is much too small.
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