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Photoelectric effect: The emission of electrons from a metal surface when electromagnetic radiation of suitable (sufficiently high) frequency falls on it is called the photoelectric effect. The emitted electrons are called photoelectrons.

Experimental set-up:

[Figure: an evacuated glass tube with a quartz window. Inside are a photosensitive plate C (emitter/cathode) and a metal plate A (collector/anode). Monochromatic light from a source passes through the quartz window onto C. A and C are connected to a battery through a potential divider (rheostat) and a commutator (reversing key), so that the potential of A relative to C can be varied and reversed. A voltmeter V is connected across A and C, and a microammeter (μA) is in series in the circuit.]

  • The tube is evacuated so that the photoelectrons do not collide with gas molecules.
  • The quartz window transmits ultraviolet as well as visible light.
  • When suitable light falls on C, photoelectrons are emitted. If A is positive with respect to C, they are attracted to A and a current (photocurrent) flows, read on the microammeter.
  • The potential divider changes the accelerating potential; the commutator reverses it so that A can be made negative (retarding potential).

Observations made with this set-up: the photocurrent increases with intensity of light; as the accelerating potential is increased the current reaches a saturation value; when A is made negative the current decreases and becomes zero at the stopping potential \(V_0\), which depends on the frequency but not on the intensity; no electrons are emitted below a threshold frequency \(\nu_0\) however intense the light; and emission is instantaneous.

Doubtly AI · 29 Oct 2026 AI-generated · not yet verified Report
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