Cathode Ray Tube

Cathode Ray Tube, an electron tube, or evacuated glass container, having at one end a device called an electron gun that projects a beam of electrons against a luminescent screen at the opposite end of the tube. A bright spot of light appears wherever the electrons strike the screen. Cathode ray tubes, or CRTs, are used as picture tubes in television receivers and as visual display screens in radar equipment, computer installations, and oscilloscopes.

Electrons are emitted from a heated cathode, or negative electrode, in the electron gun. A series of grids having a positive potential with respect to the cathode accelerate the electrons as they pass. The electrons next pass through a series of doughnut-shaped anodes that focus the stream of electrons so that they strike the luminescent screen as a fine point. Between the electron gun and the screen are either two sets of electric deflecting plates or two sets of magnetic deflecting coils. Electric deflecting plates are used in small CRTs, whereas magnetic deflecting coils are used in large CRTs in which a large deflection is required, as in television tubes.

In CRTs containing electric deflecting plates, a horizontal pair of plates controls the up-and-down motion of the electron beam, and a vertical pair controls the left-to-right motion of the beam. Both plates in each pair can be charged. If the charges on the two plates are equal, the beam will strike the centre of the luminescent screen. If the charges are unequal, or if one of them is positive while the other is negative, the electron beam will be deflected. The amount of deflection depends on the voltage applied to the plates. As the signal applied to the horizontal plates varies, so will the position of the spot of light on the face of the tube, which will move up or down in response to the changes in voltage. If the voltage of the vertical plates is varied, the beam of electrons can be made to sweep horizontally across the face of the tube.

Magnetic deflecting coils work in an analogous manner, except that the electron beam is deflected by variations in the strength of the magnetic fields through which it must pass.