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If it's a *Crookes* tube you're asking about, it's a discharge tube because the applied electrical field causes ionization and a resulting discharge of energy in the form (mostly) of light, depending on the gas or gases in the tube.
Johann Wilhelm Hittorf, a German physicist, is credited with discovering the gas discharge tube in the mid-19th century. His experiments with cathode rays in partially evacuated tubes laid the foundation for the development of early gas discharge tubes.
When viewing a discharge tube of gas through a hand-held spectroscope, bright lines appear because the gas inside the tube emits specific wavelengths of light when energized. The spectroscope separates the light into its component colors or wavelengths, allowing you to see the discrete emission lines characteristic of the gas present in the tube.
In a tube light, the gas inside the tube is typically a mixture of argon and mercury vapor. When electricity is applied to the tube, it ionizes the gas, creating a plasma by stripping electrons from the gas molecules. This ionization process allows for the generation of ultraviolet light, which then excites the phosphor coating on the inside of the tube, producing visible light.
The gas commonly used in discharge tubes for the study of cathode rays is low-pressure neon or argon. These gases allow for the observation of cathode rays because they ionize easily and produce visible light when the cathode rays collide with them. This ionization helps to create observable effects that demonstrate the properties of cathode rays, such as their trajectory and charge.
If it's a *Crookes* tube you're asking about, it's a discharge tube because the applied electrical field causes ionization and a resulting discharge of energy in the form (mostly) of light, depending on the gas or gases in the tube.
At very low pressure in a discharge tube, there are fewer gas atoms present to ionize and produce light. This results in fewer collisions and less emission of visible light, causing the discharge tube to appear dark.
Quenching in a Geiger-Müller (GM) tube refers to the process of reducing the afterglow or the residual ionization effect that occurs after a radiation detection event. When radiation ionizes the gas within the tube, it can lead to a delayed discharge or spurious counts if the ionization persists. Quenching agents, often added to the gas, help to quickly neutralize the ions and allow the GM tube to reset and become ready for the next detection event, thereby improving the accuracy and responsiveness of the device.
Johann Wilhelm Hittorf, a German physicist, is credited with discovering the gas discharge tube in the mid-19th century. His experiments with cathode rays in partially evacuated tubes laid the foundation for the development of early gas discharge tubes.
When viewing a discharge tube of gas through a hand-held spectroscope, bright lines appear because the gas inside the tube emits specific wavelengths of light when energized. The spectroscope separates the light into its component colors or wavelengths, allowing you to see the discrete emission lines characteristic of the gas present in the tube.
Argon is used in the Geiger-Muller tube as a quenching gas to stop the discharge of ions after each pulse. Keeping argon at low pressure allows for efficient quenching of the ionization process. Higher pressure could interfere with the detection process by preventing the resetting of the tube after each detection event.
In a tube light, the gas inside the tube is typically a mixture of argon and mercury vapor. When electricity is applied to the tube, it ionizes the gas, creating a plasma by stripping electrons from the gas molecules. This ionization process allows for the generation of ultraviolet light, which then excites the phosphor coating on the inside of the tube, producing visible light.
The gas commonly used in discharge tubes for the study of cathode rays is low-pressure neon or argon. These gases allow for the observation of cathode rays because they ionize easily and produce visible light when the cathode rays collide with them. This ionization helps to create observable effects that demonstrate the properties of cathode rays, such as their trajectory and charge.
Electric discharge occurs at low pressure and high potential because the low pressure reduces the number of gas molecules present, allowing for easier ionization and breakdown of the gas. The high potential creates a strong electric field, causing the free electrons to accelerate and gain energy before colliding with gas molecules, leading to ionization and discharge.
A discharge tube is a type of gas-filled tube that emits light when an electric current passes through it, commonly used in neon signs or plasma displays. On the other hand, a tube light is a type of fluorescent lamp that uses a phosphor coating inside a glass tube to produce light. While both types of tubes rely on gas and electric current to produce light, they differ in their construction and application.
When the pressure is reduced in a discharge tube, the mean free path of the gas molecules increases. This allows the gas molecules to gain more energy and move freely, colliding with the charged particles in the discharge tube and facilitating the flow of electric charge. As a result, the gases become partially ionized, creating a conductive path for the electricity.
It is necessary to maintain vacuum in a vacuum tube to provide the electrons a free path from cathode to anode without triggering ionization. If there was air or some other gas in the tube, the electron flow would cause it to ionize and the control grid would have reduced or even no control of the conduction of the tube. There are gas filled tubes that depend on this ionization: for example in thyratrons, once the control grid starts conduction ionization takes over and the grid has no more control, you have to turn off the B+ supply in some way to reset it.