For demonstrating the photoelectric effect with visible light, for investigating the frequency dependency of the photoelectric current and for determination of Planck's constant based on the counter-field method. Vacuum photocell with large-surface alkaline cathode and annular platinum electrode which can be heated in order to clean off impurities from the cathode coating.
The photo cell is used to demonstrate the photoelectric effect. When the photocathode is irradiated with light, electrons are liberated from the photocathode and can be detected at the anode ring as a photoelectric current in a suitable circuit. This device can be used to show that the energy of the light is proportional to the frequency of the radiation and independent of the intensity of the radiation. When the photocathode is irradiated with monochromatic light, it is possible to determine Planck’s constant. In addition to confirming Planck’s calculations for the radiation of a black body, Einstein’s interpretation of these experiments confirmed the quantum nature of light.
L'effetto fotoelettrico fu scoperto nel 1887 dal fisico tedesco Heinrich Rudolf Hertz (1857 - 1894), osservando che oggetti elettricamente carichi perdevano la carica se esposti alla luce ultravioletta.
Dalla consultazione degli archivi storici, risulta: "CELLULA FOTOELETTRICA QUARZO BKE, INV. N. 862 DEL 27.04.1928 LA ROSA LIRE 700.00".
Rimozione a secco della polvere con pennelli a setola morbida. Pulitura delle superfici metalliche con etere di petrolio. Pulitura dell'ampolla di vetro con alcol.
Instruction Sheet Photo cell for determining Planck's constant 558 77, Leybold
Soresini F. (2004). Di tubo... in tubo. Storia dei tubi elettronici nel centenario del diodo, 1904-2004. Sandit Libri, Bergamo, pagg.121-123.
Leybold: Photo cell for determining planck's constant N. 558 77
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