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File:Wostok-Station core32.jpg
Aerial photograph of Vostok Station, the coldest directly observed location on Earth.
File:LakeVostok-Location.jpg
The location of Vostok Station in Antarctica

The lowest natural temperature ever directly recorded at ground level on Earth is Template:Convert at the then-Soviet Vostok Station in Antarctica on 21 July 1983 by ground measurements.<ref>Template:Cite journal</ref>

On 10 August 2010, satellite observations showed a surface temperature of Template:Convert at Template:Coord, along a ridge between Dome Argus and Dome Fuji, at Template:Convert elevation.<ref>{{#invoke:citation/CS1|citation |CitationClass=web }}</ref> The result was reported at the 46th annual meeting of the American Geophysical Union in San Francisco, California, in December 2013; it is a provisional figure, and may be subject to revision.<ref name="bbc">{{#invoke:citation/CS1|citation |CitationClass=web }}</ref> The value is not listed as the record lowest temperature as it was measured by remote sensing from satellite and not by ground-based thermometers, unlike the 1983 record.<ref name="usatoday">{{#invoke:citation/CS1|citation |CitationClass=web }}</ref> The temperature announced reflects that of the ice surface, while the Vostok readings measured the air above the ice, and so the two are not directly comparable. More recent work<ref>Template:Cite journal</ref> shows many locations in the high Antarctic where surface temperatures drop to approximately Template:Convert. Due to the very strong temperature gradient near the surface, these imply near-surface air temperature minima of approximately Template:Convert.

Historical progressionEdit

On 21 January 1838, a Russian merchant named Neverov recorded a temperature of Template:Convert in Yakutsk.<ref name="noaa">{{#invoke:citation/CS1|citation |CitationClass=web }}</ref> On 15 January 1885, H. Wild reported that a temperature of Template:Convert was measured in Verkhoyansk.<ref name="noaa"/> A later measurement at the same place in February 1892 was reported as Template:Convert. Soviet researchers later announced a recording of Template:Convert in February 1933 at Oymyakon, about Template:Convert to the south-east of Verkhoyansk; this measurement was reported by Soviet texts through the 1940s as a record low, with the previous measurement from Verkhoyansk retroactively adjusted to Template:Convert.<ref>Template:Cite journal</ref>

The next reliable measurement was made during the 1957 season at the Amundsen–Scott South Pole Station in Antarctica, yielding Template:Convert on 11 May and Template:Convert on 17 September.<ref name="noaa"/> The next world record low temperature was a reading of Template:Convert, measured at the Soviet Vostok Station in 1968, on the Antarctic Plateau. Vostok again broke its own record with a reading of Template:Convert on 21 July 1983.<ref>{{#invoke:citation/CS1|citation |CitationClass=web }}</ref> This remains the record for a directly recorded temperature.

Laboratory coolingEdit

Template:Further

Early experimentsEdit

In 1904 Dutch scientist Heike Kamerlingh Onnes created a special lab in Leiden in the Netherlands with the aim of producing liquid helium. In 1908 he managed to lower the temperature to less than −269 °C (−452.2 F, 4 K), which is four degrees above absolute zero. Only in this exceptionally cold state will helium liquefy; the boiling point of helium being at −268.94 °C (−452.092 F). Kamerlingh Onnes received a Nobel Prize for his achievement.<ref>{{#invoke:citation/CS1|citation |CitationClass=web }}</ref>

Onnes' method relied upon depressurising the subject gases, causing them to cool by adiabatic cooling.Template:Citation needed This follows from the first law of thermodynamics;

<math>\Delta U = \Delta Q - \Delta W</math>

where U = internal energy, Q = heat added to the system, W = work done by the system.

Consider a gas in a box of set volume. If the pressure in the box is higher than atmospheric pressure, then upon opening the gas will do work on the surrounding atmosphere to expand. As this expansion is adiabatic and the gas has done work

<math>\Delta Q = 0</math>

<math>\Delta W > 0</math>

<math>\Rightarrow \Delta U < 0</math>

Now as the internal energy has decreased, so has the temperature.Template:Citation needed

Modern experimentsEdit

As of November 2000, nuclear spin temperatures below 100 pK were reported for an experiment at the Helsinki University of Technology Low Temperature Lab. However, this was the temperature of one particular type of motion—a quantum property called nuclear spin—not the overall average thermodynamic temperature for all possible degrees of freedom.<ref>The experimental methods and results are presented in detail in Tauno A. Knuuttila’s D.Sc. thesis which can be accessed from Aaltodoc. The university’s press release on its achievement is here.</ref> At such low temperatures, the concept of "temperature" becomes multifaceted since molecular motion cannot be assumed to average out across degrees of freedom.Template:Citation needed The corresponding peak emission will be in radio waves, rather than in the familiar infrared, so it is very inefficiently absorbed by neighboring atoms, making it difficult to reach thermal equilibrium.

The Low Temperature Laboratory recorded a record low temperature of 100 pK, or 1.0 × 10−10 K in 1999.<ref name="recordcold">{{#invoke:citation/CS1|citation |CitationClass=web }}</ref>

The current apparatus for achieving low temperatures has two stages. The first uses a helium dilution refrigerator to get to temperatures of millikelvins, then the next stage uses adiabatic nuclear demagnetisation to reach picokelvins.<ref name="recordcold"/>

Extremely low temperatures are useful for observation of quantum mechanical phases of matter such as superfluids and Bose–Einstein condensates, which would be disrupted by thermal motion.

See alsoEdit

ReferencesEdit

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External linksEdit