A molecular drag pump is a type of vacuum pump that utilizes the drag of air molecules against a rotating surface. [1] The most common sub-type is the Holweck pump, which contains a rotating cylinder with spiral grooves which direct the gas from the high vacuum side of the pump to the low vacuum side of the pump. [2] The older Gaede pump design is similar, but is much less common due to disadvantages in pumping speed. [3] In general, molecular drag pumps are more efficient for heavy gasses, so the lighter gasses (hydrogen, deuterium, helium) will make up the majority of the residual gasses left after running a molecular drag pump. [4]
The turbomolecular pump invented in the 1950s, is a more advanced version based on similar operation, and a Holweck pump is often used as the backing pump for it. The Holweck pump can produce a vacuum as low as 1×10−8 mmHg (1.3×10−6 Pa).
The earliest molecular drag pump was created by Wolfgang Gaede, who had the idea of the pump in 1905, and spent several years corresponding with Leybold trying to build a practical device. [5] The first prototype device to meet expectations was completed in 1910, achieving a pressure of less than mbar. [6] By 1912, twelve pumps had been created, and the concept was presented to the meeting of the Physical Society in Münster on 16 September of that year, and was generally well received. [5]
Gaede published several papers on the principles of this molecular pump, [7] [8] and patented the design. [9] The working principle is that the gas in the chamber is exposed to one side of a rapidly spinning cylinder. Collisions between the gas and the spinning cylinder gives the molecules of gas momentum in the same direction as the surface of the cylinder, which designed to turn away from the vacuum chamber and toward a fore-line. A separate backing pump is used to lower the pressure at the fore-line (output of the molecular pump), since in order to function, the molecular pump needs to operate under pressures low enough that the gas inside is in free molecular flow. One important measure of the pump is the compression ratio, . This is the ratio of the pressure of the vacuum, to the pressure to the outlet, and is roughly constant across different pressures, but depends on the individual gas. [10]
The compression ratio can be estimated using the kinetic theory of gases by calculating the flow due to collisions with the rotating surfaces, and rate of diffusion in the reverse direction. [11] The compression ratio tends to be better for heavy molecules, since the thermal velocity of lighter gasses is higher and speed of the rotating cylinder has a less effect on these faster moving, lighter gasses.
This "Gaede molecular pump" was used in an early experiment testing vacuum gauges. [12]
The improved Holweck design was invented in the early 1920s by Fernand Holweck [13] [14] as part of his apparatus for his work in studying soft X-rays. It was manufactured by French scientific instrument maker, Charles Beaudouin. [15] He applied for a patent on the device in 1925. [16] The main difference from the Gaede pump was the addition of a spiral, cut into either to the spinning cylinder, or to the static housing. Holweck pumps have been frequently modeled theoretically. [2] [17] [18] Holweck's classmate and collaborator, H. Gondet, would later suggest other improvements to the design. [5] [19]
Another design was given by Manne Siegbahn. [20] He had produced a pump which was used in 1926. [21] About 50 of Siegbahn's pumps were made from 1926 to 1940. [5] These pumps were generally slower than comparable diffusion pumps, so were rare outside of Uppsala University. Larger, faster pumps of the Siegbahn type began to be made around 1940 for use in a cyclotron. [22] In 1943, Seigbahn published a paper regarding these pumps, which were based on a rotating disk. [23]
While the molecular drag pumps of Gaede, Holweck, and Siegbahn are functional designs, they have remained relatively uncommon as stand-alone pumps. One issue was pumping speed: alternatives such as the diffusion pump are much faster. Secondly, a major issue with these pumps is reliability: with a gap between moving parts in the tens of micrometers, any dust or temperature change threatens to bring the parts into contact and cause the pump to fail. [24]
The turbomolecular pump overcame many of these disadvantages. Many modern turbomolecular pumps contain built-in molecular drag stages, which allows them to operate at higher foreline pressures.
As a stage in turbo molecular pumps, the most widely used design is the Holweck type, due to a significantly higher pumping speed than the Gaede design. While slower, the Gaede design has the advantage of tolerating a higher inlet pressure for the same compression ratio, and being more compact than the Holweck type. [3] While the Gaede and Holweck designs are significantly more widely used, Siegbahn-type designs continue to be investigated, due to their significantly more compact design compared with Holweck stages. [25]
The compression ratio is the ratio between the volume of the cylinder and combustion chamber in an internal combustion engine at their maximum and minimum values.
Diffusion pumps use a high speed jet of vapor to direct gas molecules in the pump throat down into the bottom of the pump and out the exhaust. They were the first type of high vacuum pumps operating in the regime of free molecular flow, where the movement of the gas molecules can be better understood as diffusion than by conventional fluid dynamics. Invented in 1915 by Wolfgang Gaede, he named it a diffusion pump since his design was based on the finding that gas cannot diffuse against the vapor stream, but will be carried with it to the exhaust. However, the principle of operation might be more precisely described as gas-jet pump, since diffusion plays a role also in other high vacuum pumps. In modern textbooks, the diffusion pump is categorized as a momentum transfer pump.
A turbomolecular pump is a type of vacuum pump, superficially similar to a turbopump, used to obtain and maintain high vacuum. These pumps work on the principle that gas molecules can be given momentum in a desired direction by repeated collision with a moving solid surface. In a turbomolecular pump, a rapidly spinning fan rotor 'hits' gas molecules from the inlet of the pump towards the exhaust in order to create or maintain a vacuum.
A vacuum pump is a type of pump device that draws gas particles from a sealed volume in order to leave behind a partial vacuum. The first vacuum pump was invented in 1650 by Otto von Guericke, and was preceded by the suction pump, which dates to antiquity.
A vacuum is a space devoid of matter. The word is derived from the Latin adjective vacuus for "vacant" or "void". An approximation to such vacuum is a region with a gaseous pressure much less than atmospheric pressure. Physicists often discuss ideal test results that would occur in a perfect vacuum, which they sometimes simply call "vacuum" or free space, and use the term partial vacuum to refer to an actual imperfect vacuum as one might have in a laboratory or in space. In engineering and applied physics on the other hand, vacuum refers to any space in which the pressure is considerably lower than atmospheric pressure. The Latin term in vacuo is used to describe an object that is surrounded by a vacuum.
The following is a timeline of low-temperature technology and cryogenic technology. It also lists important milestones in thermometry, thermodynamics, statistical physics and calorimetry, that were crucial in development of low temperature systems.
A cryopump or a "cryogenic pump" is a vacuum pump that traps gases and vapours by condensing them on a cold surface, but are only effective on some gases. The effectiveness depends on the freezing and boiling points of the gas relative to the cryopump's temperature. They are sometimes used to block particular contaminants, for example in front of a diffusion pump to trap backstreaming oil, or in front of a McLeod gauge to keep out water. In this function, they are called a cryotrap, waterpump or cold trap, even though the physical mechanism is the same as for a cryopump.
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Ultra-high vacuum (UHV) is the vacuum regime characterised by pressures lower than about 100 nanopascals. UHV conditions are created by pumping the gas out of a UHV chamber. At these low pressures the mean free path of a gas molecule is greater than approximately 40 km, so the gas is in free molecular flow, and gas molecules will collide with the chamber walls many times before colliding with each other. Almost all molecular interactions therefore take place on various surfaces in the chamber.
Temperature programmed desorption (TPD) is the method of observing desorbed molecules from a surface when the surface temperature is increased. When experiments are performed using well-defined surfaces of single-crystalline samples in a continuously pumped ultra-high vacuum (UHV) chamber, then this experimental technique is often also referred to as thermal desorption spectroscopy or thermal desorption spectrometry (TDS).
A scroll compressor is a device for compressing air or refrigerant. It is used in air conditioning equipment, as an automobile supercharger and as a vacuum pump. Many residential central heat pump and air conditioning systems and a few automotive air conditioning systems employ a scroll compressor instead of the more traditional rotary, reciprocating, and wobble-plate compressors.
Wake Shield Facility (WSF) was a NASA experimental science platform that was placed in low Earth orbit by the Space Shuttle. It was a 3.7 m (12 ft) diameter, free-flying stainless steel disk.
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Chemical beam epitaxy (CBE) forms an important class of deposition techniques for semiconductor layer systems, especially III-V semiconductor systems. This form of epitaxial growth is performed in an ultrahigh vacuum system. The reactants are in the form of molecular beams of reactive gases, typically as the hydride or a metalorganic. The term CBE is often used interchangeably with metal-organic molecular beam epitaxy (MOMBE). The nomenclature does differentiate between the two processes, however. When used in the strictest sense, CBE refers to the technique in which both components are obtained from gaseous sources, while MOMBE refers to the technique in which the group III component is obtained from a gaseous source and the group V component from a solid source.
An ion pump is a type of vacuum pump which operates by sputtering a metal getter. Under ideal conditions, ion pumps are capable of reaching pressures as low as 10−11 mbar. An ion pump first ionizes gas within the vessel it is attached to and employs a strong electrical potential, typically 3–7 kV, which accelerates the ions into a solid electrode. Small bits of the electrode are sputtered into the chamber. Gasses are trapped by a combination of chemical reactions with the surface of the highly-reactive sputtered material, and being physically trapped underneath that material.
Fernand Holweck was a French physicist who made important contributions in the fields of vacuum technology, electromagnetic radiation and gravitation. He is also remembered for his personal sacrifice in the cause of the French Resistance and his aid to Allied airmen in World War II.
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Mechanically Stimulated Gas Emission
Wolfgang Max Paul Gaede was a German physicist and pioneer of vacuum engineering.
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