Second sound: Difference between revisions
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==Second sound in other media== |
==Second sound in other media== |
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<sup>3</sup>He has second sound below 2.5 mK, <sup>6</sup>Li also close to 0 K. Superfluidity of <sup>6</sup>Li has been observed at a temperature of 50 nK at [[MIT]] in April 2005.<ref>{{ |
<sup>3</sup>He has second sound below 2.5 mK, <sup>6</sup>Li also close to 0 K. Superfluidity of <sup>6</sup>Li has been observed at a temperature of 50 nK at [[MIT]] in April 2005.<ref>{{cite web| url = http://web.mit.edu/newsoffice/2005/matter.html| title = MIT physicists create new form of matter| accessdate = 2010 November 22}}</ref>. Second sound has also been observed in some dielectric solids, such as Bi and NaF.{{Citation needed|date=October 2009}} |
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== References == |
== References == |
Revision as of 16:46, 22 November 2010
Second sound is a quantum mechanical phenomenon in which heat transfer occurs by wave-like motion, rather than by the more usual mechanism of diffusion. Heat takes the place of pressure in normal sound waves. This leads to a very high thermal conductivity. It is known as "second sound" because the wave motion of heat is similar to the propagation of sound in air.
Second sound is observed in liquid helium (3He as well as 4He) and in 6Li at temperatures below the lambda point. In this state, known as helium II, 4He has the highest thermal conductivity of any known material (several hundred times higher than copper).
Second sound in helium II
At temperatures below the lambda point 2.1768 K, 4He enters a superfluid state and has almost perfect heat conduction. The helium is in a macroscopic quantum state. At temperatures falling toward 0 K the speed of temperature and entropy waves increases. These can be generated and observed in a resonator. At a temperature of 1.8 K the temperature wave propagates at approximately 20 m/s.
Second sound in other media
3He has second sound below 2.5 mK, 6Li also close to 0 K. Superfluidity of 6Li has been observed at a temperature of 50 nK at MIT in April 2005.[1]. Second sound has also been observed in some dielectric solids, such as Bi and NaF.[citation needed]
References
- ^ "MIT physicists create new form of matter". Retrieved 2010 November 22.
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V. Narayanamurti and R.C. Dynes. Phys. Rev. Lett. 28, 1461, (1972). T.F. McNelly, S.J. Rogers, D.J. Chanin, R.J. Rollefson, W.M. Goubau, G.E. Schmidt, I. A. Krumhansl, R.O. Pohl, Phys. Rev. Lett. 24, 100 (1970). H.E. Jackson, C.T. Walker. Phys. Rev. B, V. 3 (4), p. 1428 (1971).
Bibliography
- C.T. Lane, H.A. Fairbank, and W.M. Fairbank, "Second Sound in Liquid Helium II," Phys. Rev. 71, 600 (1947). Retrieved on April 15, 2007.
- Sinyan Shen, Surface Second Sound in Superfluid Helium. PhD Dissertation (1973). http://adsabs.harvard.edu/abs/1973PhDT.......142S
- V. Peshkov, "'Second Sound' in Helium II," J. Phys. (Moscow) 8, 381 (1944)
- U. Piram, "Numerical investigation of second sound in liquid helium," Dipl.-Ing. Dissertation (1991). Retrieved on April 15, 2007.
- H.E. Jackson, C.T. Walker, and T.F. McNelly, "Second sound in NaF," Phys. Rev. Letters 25, 26 - 28 (1970)
- V. Narayanamurti, and R.C. Dynes, "Observation of second sound in Bismuth," Phys. Rev. Letters 28, 1461 - 1465 (1972)
See also