357792
Statement A :
Though light of a single frequency (monochromatic) is incident on a metal, the energies of emmited photoelectrons are different.
Statement B :
The energy of electrons emitted from inside the metal surface is lost in collision with the other atoms in the metal.
357793 When light of wavelength \(300\;nm\) falls on a photoelectric emitter, photoelectrons are liberated. For another emitter, light of wavelength \(600\;nm\) is sufficient for liberating photoelectrons. The ratio of the work function of the two emitters is
357792
Statement A :
Though light of a single frequency (monochromatic) is incident on a metal, the energies of emmited photoelectrons are different.
Statement B :
The energy of electrons emitted from inside the metal surface is lost in collision with the other atoms in the metal.
357793 When light of wavelength \(300\;nm\) falls on a photoelectric emitter, photoelectrons are liberated. For another emitter, light of wavelength \(600\;nm\) is sufficient for liberating photoelectrons. The ratio of the work function of the two emitters is
357792
Statement A :
Though light of a single frequency (monochromatic) is incident on a metal, the energies of emmited photoelectrons are different.
Statement B :
The energy of electrons emitted from inside the metal surface is lost in collision with the other atoms in the metal.
357793 When light of wavelength \(300\;nm\) falls on a photoelectric emitter, photoelectrons are liberated. For another emitter, light of wavelength \(600\;nm\) is sufficient for liberating photoelectrons. The ratio of the work function of the two emitters is
357792
Statement A :
Though light of a single frequency (monochromatic) is incident on a metal, the energies of emmited photoelectrons are different.
Statement B :
The energy of electrons emitted from inside the metal surface is lost in collision with the other atoms in the metal.
357793 When light of wavelength \(300\;nm\) falls on a photoelectric emitter, photoelectrons are liberated. For another emitter, light of wavelength \(600\;nm\) is sufficient for liberating photoelectrons. The ratio of the work function of the two emitters is