The inequality of the electric field in the gas when a continuous discharge is passing through it is very obvious when the pressure of the gas is low. In this case the discharge presents a highly differentiated appearance of which a type is represented in fig. 15. Starting from the cathode we have a thin velvety luminous glow in contact with the surface; this glow is often called the "first cathode layer." Next this we have a comparatively dark space whose thickness increases as the pressure diminishes; this is called the "Crookes's dark space," or the "second cathode layer." Next this we have a luminous position called the "negative glow" or the "third cathode layer." The boundary between the second and third layers is often very sharply defined. Next to the third layer we have another dark space called the "Faraday dark space." Next to this and reaching up to the anode is another region of luminosity, called the "positive column," sometimes (as in fig. 15, a) continuous, sometimes (as in fig. 15, b) broken up into light or dark patches called "striations." The dimensions of the Faraday dark space and the positive column vary greatly with the current passing through the gas and with its pressure; sometimes one or other of them is absent. These differences in appearances are accompanied by great difference in the strength of the electric field. The magnitude of the electric force at different parts of the discharge is represented in fig. 16, where the ordinates represent the electric force at different parts of the tube, the cathode being on the right. We see that the electric force is very large indeed between the negative glow and the cathode, much larger than in any other part of the tube. It is not constant in this region, but increases as we approach the cathode. The force reaches a minimum either in the negative glow itself or in the part of the Faraday dark space just outside, after which it increases towards the positive column. In the case of a uniform positive column the electric force along it is constant until we get quite close to the anode, when a sudden change, called the "anode fall," takes place in the potential. [Illustration: _Discharge in Hydrogen Pressure 2.25 m.m. Current 0.568·10^-3 ampere_ FIG. 16.]