Second sound explained

In condensed matter physics, 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. Its presence leads to a very high thermal conductivity. It is known as "second sound" because the wave motion of entropy and temperature is similar to the propagation of pressure waves in air (sound). The phenomenon of second sound was first described by Lev Landau in 1941.[1]

Description

Normal sound waves are fluctuations in the displacement and density of molecules in a substance;[2] [3] second sound waves are fluctuations in the density of quasiparticle thermal excitations (rotons and phonons[4]). Second sound can be observed in any system in which most phonon-phonon collisions conserve momentum, like superfluids[5] and in some dielectric crystals[6] [7] [8] when Umklapp scattering is small.

Contrary to molecules in a gas, quasiparticles are not necessarily conserved. Also gas molecules in a box conserve momentum (except at the boundaries of box), while quasiparticles can sometimes not conserve momentum in the presence of impurities or Umklapp scattering. Umklapp phonon-phonon scattering exchanges momentum with the crystal lattice, so phonon momentum is not conserved, but Umklapp processes can be reduced at low temperatures.[9]

Normal sound in gases is a consequence of the collision rate between molecules being large compared to the frequency of the sound wave . For second sound, the Umklapp rate has to be small compared to the oscillation frequency for energy and momentum conservation. However analogous to gasses, the relaxation time describing the collisions has to be large with respect to the frequency, leaving a window:

1
\tau\rm

\ll\omega\ll

1
\tauN

for sound-like behaviour or second sound. The second sound thus behaves as oscillations of the local number of quasiparticles (or of the local energy carried by these particles). Contrary to the normal sound where energy is related to pressure and temperature, in a crystal the local energy density is purely a function of the temperature. In this sense, the second sound can also be considered as oscillations of the local temperature. Second sound is a wave-like phenomena which makes it very different from usual heat diffusion.

In helium II

Second sound is observed in liquid helium at temperatures below the lambda point, 2.1768 K, where 4He becomes a superfluid known as helium II. Helium II has the highest thermal conductivity of any known material (several hundred times higher than copper).[10] Second sound can be observed either as pulses or in a resonant cavity.[11]

The speed of second sound is close to zero near the lambda point, increasing to approximately 20 m/s around 1.8 K,[12] about ten times slower than normal sound waves.[13] At temperatures below 1 K, the speed of second sound in helium II increases as the temperature decreases.[14]

Second sound is also observed in superfluid helium-3 below its lambda point 2.5 mK.[15]

As per the two-fluid, the speed of second sound is given by

c2=\left(

TS2
C
\rhos
\rhon

\right)1/2

where

T

is the temperature,

S

is the entropy,

C

is the specific heat,

\rhos

is the superfluid density and

\rhon

is the normal fluid density. As

T → 0

,

c2=c/\sqrt{3}

, where

c=(\partialp/\partial\rho)S ≈ (\partialp/\partial\rho)T

is the ordinary (or first) sound speed.

In other media

Second sound has been observed in solid 4He and 3He,[16] [17] and in some dielectric solids such as Bi in the temperaturerange of 1.2 to 4.0 K with a velocity of 780 ± 50 m/s,[18] or solid sodium fluoride (NaF) around 10 to 20 K.[19] In 2021 this effect was observed in a BKT superfluid[20] as well as in a germanium semiconductor[21] [22]

In graphite

In 2019 it was reported that ordinary graphite exhibits second sound at 120 K. This feature was both predicted theoretically and observed experimentally, andwas by far the highest temperature at which second sound has been observed.[23] However, this second sound is observed only at the microscale, because the wave dies out exponentially withcharacteristic length 1-10 microns. Therefore, presumably graphite in the right temperature regime has extraordinarily high thermal conductivity but only for the purpose of transferring heat pulses distances of order 10 microns, and for pulses of duration on the order of 10 nanoseconds. For more "normal" heat-transfer, graphite's observed thermal conductivity is less than that of, e.g., copper. The theoretical models, however, predict longer absorption lengths would be seen in isotopically pure graphite, and perhaps over a wider temperature range, e.g. even at room temperature. (As of March 2019, that experiment has not yet been tried.)

Applications

Measuring the speed of second sound in 3He-4He mixtures can beused as a thermometer in the range 0.01-0.7 K.[24]

Oscillating superleak transducers (OST)[25] use second sound to locate defects in superconducting accelerator cavities.[26] [27]

See also

References

  1. Landau, L. (1941). Theory of the superfluidity of helium II. Physical Review, 60(4), 356.
  2. Book: Feynman . Richard . Feynman Lectures on Physics . 4 October 2011 . Basic Books . 978-0465024933.
  3. Web site: Feynman . Sound. The wave equation . feynmanlectures.caltech.edu . Caltech . 20 July 2021.
  4. Book: Transport Phenomena . Smith . Henrik . Jensen . H. Hojgaard . 1989 . Oxford University Press . 0-19-851985-0 . Section 4.3: Second Sound .
  5. Second Sound: Waves of Entropy and Temperature . Srinivasan . R . Resonance . 3 . March 1999 . 16–24 . 10.1007/BF02838720 . 123957486 .
  6. Second Sound: The Role of Elastic Waves . Srinivasan . R . Resonance . 4 . June 1999 . 15–19 . 10.1007/bf02834631 . 124849291 .
  7. Prohofsky . E. . Krumhansl . J. . 10.1103/PhysRev.133.A1403 . Second-Sound Propagation in Dielectric Solids . Physical Review . 133 . 5A . A1403 . 1964 . 1964PhRv..133.1403P .
  8. Chester . M. . Second Sound in Solids . 10.1103/PhysRev.131.2013 . Physical Review . 131 . 5 . 2013–2015 . 1963 . 1963PhRv..131.2013C .
  9. Book: Ashcroft . Neil W. . Solid State Physics . Mermin . N. David . 1976 . Holt, Rinehart and Winston . 978-0-03-083993-1 . en.
  10. Superfluid helium as a technical coolant . Lebrun . Phillipe . July 17, 1997 . 4 . LHC-Project-Report-125 . CERN .
  11. Van Der Boog . A. G. M. . Husson . L. P. J. . Disatnik . Y. . Kramers . H. C. . Experimental results on the velocity of second sound and the viscosity in dilute 3He-4He mixtures . 10.1016/0378-4363(81)90176-5 . Physica B+C . 104 . 3 . 303–315 . 1981 . 1981PhyBC.104..303V .
  12. Wang . R. T. . Wagner . W. T. . Donnelly . R. J. . 1987 . Precision second-sound velocity measurements in helium II . Journal of Low Temperature Physics . 68 . 5–6 . 409–417 . 1987JLTP...68..409W . 10.1007/BF00682305. 120789592 .
  13. Lane . C. . Fairbank . H. . Fairbank . W. . 10.1103/PhysRev.71.600 . Second Sound in Liquid Helium II . Physical Review . 71 . 9 . 600–605 . 1947 . 1947PhRv...71..600L .
  14. De Klerk . D. . Hudson . R. . Pellam . J. . Second Sound Propagation below 1K . 10.1103/PhysRev.93.28 . Physical Review . 93 . 28–37 . 1954 . 1 . 1954PhRv...93...28D .
  15. Lu . S. . Kojima . H. . 10.1103/PhysRevLett.55.1677 . Observation of Second Sound in Superfluid ^He-B . Physical Review Letters . 55 . 16 . 1677–1680 . 1985 . 10031890. 1985PhRvL..55.1677L .
  16. Ackerman . C. . Bertman . B. . Fairbank . H. . Guyer . R. . Second Sound in Solid Helium . 10.1103/PhysRevLett.16.789 . Physical Review Letters . 16 . 18 . 789–791 . 1966 . 1966PhRvL..16..789A .
  17. Ackerman . C. . Overton . W. . 10.1103/PhysRevLett.22.764 . Second Sound in Solid Helium-3 . Physical Review Letters . 22 . 15 . 764–766 . 1969 . 1969PhRvL..22..764A .
  18. Narayanamurti . V. . Dynes . R. . 10.1103/PhysRevLett.28.1461 . Observation of Second Sound in Bismuth . Physical Review Letters . 28 . 22 . 1461–1465 . 1972 . 1972PhRvL..28.1461N .
  19. Jackson . H. . Walker . C. . McNelly . T. . Second Sound in NaF . 10.1103/PhysRevLett.25.26 . Physical Review Letters . 25 . 26–28 . 1970 . 1 . 1970PhRvL..25...26J .
  20. Christodoulou P, Gałka M, Dogra N et al . 10 June 2021 . Observation of first and second sound in a BKT superfluid . Nature . 594 . 7862 . 191–194 . 2008.06044 . 2021Natur.594..191C . 10.1038/s41586-021-03537-9 . 34108696 . 235394222.
  21. Beardo . Albert . López-Suárez . Miquel . Pérez . Luis Alberto . Sendra . Lluc . Alonso . Maria Isabel . Melis . Claudio . Bafaluy . Javier . Camacho . Juan . Colombo . Luciano . Rurali . Riccardo . Alvarez . Francesc Xavier . Reparaz . Sebastian . 2021-06-01 . Observation of second sound in a rapidly varying temperature field in Ge . Science Advances . en . 7 . 27 . eabg4677 . 2007.05487 . 2021SciA....7.4677B . 10.1126/sciadv.abg4677 . 2375-2548 . 8245038 . 34193427.
  22. Web site: 2021-07-18 . 'Second sound' appears in germanium . 2021-07-20 . Physics World . en-GB.
  23. Huberman . S. . Duncan . R.A. . 10.1126/science.aav3548 . Observation of second sound in graphite at temperatures above 100 K . Science . 2019 . 364 . 6438 . 375–379 . 30872535 . 1901.09160 . 2019Sci...364..375H . 78091609 .
  24. Book: Pitre . L. . The Comparison between a Second-Sound Thermometer and a Melting-Curve Thermometer from 0.8 K Down to 20 mK . 10.1063/1.1627108 . AIP Conference Proceedings . 684 . 101–106 . 2003 .
  25. Sherlock . R. A. . Oscillating Superleak Second Sound Transducers . 10.1063/1.1684354 . Review of Scientific Instruments . 41 . 11 . 1603–1609 . 1970 . 1970RScI...41.1603S . free .
  26. ILC Newsline . The sound of accelerator cavities . Hesla . Leah . 21 April 2011 . 26 October 2012 .
  27. Quadt . A. . Schröder . B. . Uhrmacher . M. . Weingarten . J. . Willenberg . B. . Vennekate . H. . 10.1103/PhysRevSTAB.15.031001 . Response of an oscillating superleak transducer to a pointlike heat source . Physical Review Special Topics: Accelerators and Beams . 15 . 3 . 2012 . 031001 . 1111.5520 . 2012PhRvS..15c1001Q . 118996515 .

Bibliography

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