cryogenics makariy a. tanatarcanfield.physics.iastate.edu/course/090904.pdfthe branches of physics...
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CRYOGENICS
590B F08
Makariy A. Tanatar
Motivations
History
How do we get there?
Materials
Cryostats
Safety
Based on a lecture bySergey L. Bud’ko
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CryogenicsThe branches of physics and engineering that involve the study of very low temperatures, how to produce them, and how materials behave at those temperatures.
LT-13 International Conference Low Temperature PhysicsTemperatures below 120 K
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TemperatureCelsius( ºC)
Absolute(K)
TropicsHuman bodyRoom temperatureIce pointHome refrigeratorAntarctic winterSolid carbon dioxideLiquid oxygenLiquid nitrogenLiquid heliumAbsolute zero
4537200
-18-50-78
-183-196-269-273
318310293273255223195907740
Some typical temperatures
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cryo-transport of natural gas 100 t LH2 + 600 t LO2
medicine
research - physics
space
cryo-surgery and veterinary
medicine
Main industry:gas separationOxygen in metallurgy
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Why do we want low temperatures?
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Historical cryogenics events
1850 Mechanical refrigeration first applied
1877 Cailetet & Pictet liquefied O2 (90 K).
1892 James Dewar developed the vacuum flask
1908 Kamerlingh Onnes liquefied He (4.2 K).
1911 K. O. discovered superconductivity.
1926 Giauque reached 0.25 K by magnetic cooling.
1946 Collins developed commercial He liquefier.
1995 Connell & Wiemann achieved Bose-Einstein
condensation at 2x10-8 K.
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Usual refrigerator
We can make electronic Analogs
Thermoelectric coolingusing Peltier effect
Less efficient ~5-10%Compared to ~50%
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Cooling with cryogenic liquids
We can not get below the triple point, freezing
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Normal boiling point and latent heat of fluids
� Water : 373 K 2256 kJ/kg
� Ethylene : 169 K 481 kJ/kg
� Krypton : 120 K 116 kJ/kg
� Methane : 111 K 512 kJ/kg
� Xenon : 110 K 99 kJ/kg
� Oxygen : 90 K 213 kJ/kg
� Argon : 87 K 162 kJ/kg
� Nitrogen : 77 K 199 kJ/kg
� Neon : 27 K 86 kJ/kg
� Hydrogen : 20 K 443 kJ/kg SAFETY!
� Helium : 4.2 K 21 kJ/kg
Cooling with cryogenic liquids
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32 (0.8)34 (0.8)66 (1.6)300 – 4.24He
2.2 (0.16)1.4 (0.1)3.2 (0.2)77 – 4.24He
0.46 (0.28)0.53 (0.33)1.0 (0.63)300 - 77N2
CuSSAlTemperature change (K)
Cryoliquid
Amount of cryoliquids (in liters) to cool 1 kg of metal if only latent heat (latent heat + enthalpy of the gas) is used.
Cooling with cryogenic liquids
Use LN2
to precool the equipment (caution and patience needed)
Make use of the enthalpy of the cold He gas (very slow initial transfer, end of the transfer tube close to the bottom)
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Q=n∆H=nL,
Q cooling powern rate of evaporation, molecules/time∆H enthalpy of evaporation
L latent heat of evaporation
For a pump with constant volume rate V
Q=VP(T)L
Cooling below 4.2KEvaporating cryogenic liquid
Latent heat L [J/mole]
Temperature [K]
L approximately constant
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Cooling power proportional to vapor pressureQ~P(T)~exp(-1/T)
Exponentially small at low TWe can get by pumping on He-4 T~1K He-3 T~0.26 K
Evaporative cooling is used in 1K potHe-3 cryostat
Vapor pressure [mbar]
Temperature [K]
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Cooling with cryogenic liquids
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Summary:
Standard way to cool down in the physics labs
77 K liquid nitrogen4.2 K liquid helium~1 K pumped liquid helium (1K pot)~0.3K pumped liquid He3~1 mK dilution refrigerator~0.1 mK demagnetization refrigerator
Each process is used usually in a sequence to save resources
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Materials at low temperatures
Properties change!
Structural phase transition (brittle-ductile – Ti alloys)
CW paramagnetism, long range magnetic order, spin glass
Superconductivity (annoying traces of it – phosphor bronze, Ti-alloys, many solders)
Freezing/glassing (liquids, oils, greases)
Condensation/liquefaction (gases)
Change of mechanical properties (rubber, plastics)
Need to take into account for experiment design
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A; silver 99.999% pure, B; copper (OFHC), C; coalesced copper, D; electrolytic tough pitch, E; single crystal aluminum, F; machining copper,G; aluminum 1100 F, H; aluminum 6063-T5, I; phosphorus deoxidized copper, J; aluminum 2024-T4, K; brass
Thermal conductivity - high
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A; 50-50 Pb-Sn solderB; steel, SAE 1020C; beryllum copperD; constantanE; monelF; silicon bronzeG; inconnelH; 347 stainless steelI; fused quartzJ; teflon (PTFE)K; polymethylmethacrylate (PMMA) L; nylon
Thermal conductivity - low
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Thermal contraction
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Heat sources
(i) Heat conduction
stainless steel
thin walls
G10
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Heat sources
(ii) Heat radiation
polished surfaces
radiation shields
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Heat sources
(iii) Residual gas conduction
getters on cold walls
(iv) Thermoacoustic (Taconis) oscillations
change in geometry
introduction of damping element
standing waves in gas filled tubes with temperature gradient andclosed warm end
use of Taconis
oscillations
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Superinsulation
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Dewar flask
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Storage dewars
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Dipper
Fast, cheap (and dirty)
Can use storage dewar
Poor temperature control (easy to improve somewhat)
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Continuous flow cryostat
Cheap
Fast cooling
Relatively low He consumption
Relatively easy optical access
Base temperature?
Mediocre temperature control
Hard to incorporate high field
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Going below 4.2 K – 4He
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4He cryostat with variable temperature insert
Workhorse for LT measurements
Good temperature control
Easy magnet accommodation
Allows for variety of sample holders
Not so cheap
Uses fair amount of cryogens
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Helium transferHe level detectors: acoustic, resistive
(SC), capacitive.
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History repeats itself
Refrigeration of 19th
century
Storage of winter ice (cold countries)
Refrigerators came later
Common now
Cryogenics 20th century
cryoliquids
Moving towards individual refrigerators
Closed cycle units
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How to get there? Closed cycle refrigerators…
Gifford-McMahon (G-M) or Pulse Tube (PT) cycle
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Close cycled refrigerators
GOOD
Turn-key
Easy optical (etc…) access
No liquid cryogens
Small footprint (but remember compressor)
Sometimes reasonably priced
NOT SO GOOD
“Usually” base T > 4 K
Noise, vibrations
“Small” cooling power at low temperatures
Long term maintenance cost?
Use in high fields?
Somewhat difficult to tweak
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One can buy
14T/100mK measurements platform (combination of PT cryocooler and magnetic refrigeration stage)
SQUID magnetometer with installed liquefaction unit.
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Safety
Temperature
Pressure
Energy (SC magnets)
Ice blocks
Relief valves
He level – magnet quench
Glass dewars
Nitrogen freezing
Liquid oxygen
Think
Learn
RECOVER!
Personal safety
Equipment safety
Loss of expensive materials
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Safety
Ref. [6]
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Safety
Temperature
Gas Pressure
Energy (SC magnets)
Damage to expensive equipment
Loss of mixture
Do not let it happen here!
Known cases in my experience
Kyoto: 15T magnet on energization attracted
rotary pump, which destroyed vacuum Dewar
Loss of the magnet
Kyoto: due to an air leak to cryogenic center
Liquefier was damaged, 0.5 mln $ loss
Sherbrooke: quench due to He
magnet bath exhaust damaged magnet
Critical field reduced from 15T to 0.7T
Sherbrooke: due to a leak, dipper
accumulated He liquid inside and exploded
on warming, fortunately no one was injured
Cornell: closed 1K pot with He liquid
inside and relieve valve frozen,
destroyed DF
Bristol: on a day like today, student opened OVC
vacuum valve
1 million worth of equipment
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Reading materials
Matter and methods at low temperatures
Author: Frank Pobell; Springer, 2007
Experimental techniques in low-temperature physics
Author: Guy K. White; Clarendon Press, 1979
Experimental low-temperature physics
Author: Anthony Kent; American Institute of Physics, 1993
Experimental techniques in condensed matter physics at low
temperatures
Author: Robert C Richardson; Eric N Smith Addison-Wesley Pub. Co., 1988
Experimental techniques for low-temperature measurements : cryostat
design, material properties, and superconductor critical-current testing
Author: J. W. Ekin; Oxford University Press, 2006
Hitchhiker’s guide to dilution refrigerators, Nathaniel Creig and Ted Lester
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Sir James Dewar, FRS (1842-1923)
Developed Cordite (smokeless gunpowder alternative) – with Sir Frederick Abel, 1889
Described several formulae for benzene, 1867
Studied physiological action of light, with Prof. J. G. McKendrick (conditions of retina)
Spectroscopical observations, with Prof. G.D. Living
Public liquefaction of oxygen and air, 1884
Cir. 1892 – vacuum flask
Liquid hydrogen, 1898, solid hydrogen, 1899
Gas-absorbing powers of charcoal, 1905
Surface tension of soap bubbles, during and after WW1
Last publication in 1923 (at 80 yrs age)
Was able to engage in quite
vitriolic arguments with
other scientists: “…argue
with Dewar was akin to
being a fly in molasses…”
Lost race for He liquefaction
Lost patent case against
Thermos in court
Was nominated many times
but did not get Nobel prize
Refused to retire from
Fullerian Professorship in
Chemistry at the Royal
Institution
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Electrical resistivity and heat capacity
appendix
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(1) 2024-T4 Aluminum
(2) Beryllium copper
(3) K-monel
(4) Titanium
(5) 304 Stainless steel
(6) C1020 Carbon steel
(7) 9% Nickel alloy steel
(8) Teflon
(9) Invar-36
Yield strength of engineering materials
appendix
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Variation of Young's modulus with temperature
appendix