Background: The gas laws assert that at “absolute zero” or 0 K, the gaseousness of the gases ends. Experimentally, gases become liquid or solid at 0 K. However, (i) 0 K is not the lowest limit of temperature; and (ii) at 0 K, the value of entropy is not zero. Activity continues at 0 K. There is (a) “Zero-point” energy; (b) the principle of “indeterminacy” holds; (c) 0 K is not the lower limit of “critical points” of the fluids and solids phases; (d) the structures of atoms comport in “clusters”; (e) electronic energy “mismatch” in superconductivity; and other phenomena stand against zero entropy at 0K. Purpose: Dissipation of matter means dissipation of energy. It may be possible to harvest the dissipating energy at below 0 K temperature for the use of human beings. Method: A number of statistical equations anchor at zero entropy at 0K. This anchor is arbitrary. At 0 K, gas stays as liquid, solid or plasma. Argumentatively, much below that temperature there is liquid–limit–temperature (LLT) where all liquids become solids or plasma. Below LLT, there is solid–limit-temperature (SLT) where freeze decay of matter sets in. At SLT, the articles and sub-particles constituting an atom dance away in to space. Result: Matter exists in the range between very cold temperature and very hot temperature. When matter dissipates then energy disperses with the dissipating matter. Conclusion: Laboratories need to reach the SLT temperature empirically and find means to harvest the dissipating energy.
Published in | American Journal of Modern Physics (Volume 4, Issue 5) |
DOI | 10.11648/j.ajmp.20150405.11 |
Page(s) | 217-220 |
Creative Commons |
This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited. |
Copyright |
Copyright © The Author(s), 2015. Published by Science Publishing Group |
Gas-Limit-Temperature, Liquid-Limit-Temperature, Solid-Limit-Temperature, Dissipation of Matter, Freeze-Decay
[1] | "The American Heritage, Science Dictionary, Houghton Muffin Company," triples point, 2015. |
[2] | Stewert, and James, Calculus, Early Transcedentals, 6th ed., 2008. |
[3] | R. Larson, and B. H. Bruce, Calculus, 9th ed., 2009. |
[4] | R. A. Adam, and C. Essex, Calculus, A Complete Course, 2009. |
[5] | J. K. Barthakur, "Existential Theory of Time, Special Issue: Physics of Time: Theory and Experiment," American Journal of Modern Physics, Vol. 4, pp. 19-25, 2015. |
[6] | J. K. Barthakur, "Limit of Low Temperature, Freeze Decay," Essays in the Year of Physics, 2005. |
[7] | J. K. Barthakur, "The Limitation in the Concept of Space Time Continuum", Indian Science Congress Association, The 89th Congress held in Lucknow, 2002. |
[8] | J. K. Barthakur, Theory of Time, Indian Philosophical Quarterly, 1995. |
[9] | J. K. Barthakur, "Black Hole Should Not Exist", Indian Science Congress Association, The 90th Congress held in Bangaluru, 2003. |
[10] | S. Braun et al. Negative Absolute Temperature for Motional Degrees of Freedom,Science 339, 52-55 (2013). |
[11] | A. Rapp, S.Mandt, and A.Rosch, Equilibration Rates and Negative Absolute Temperatures for Ultracold Atoms in Optical Lattices, Phys. Rev. Lett. 105, 220405 (2010). |
[12] | S. Mandt, A. Rapp, and A. Rosch, Interacting Fermionic Atoms in Optical Lattices Diffuse Symmetrically Upwards and Downwards in a Gravitational Potential, Phys. Rev. Lett. 106, 250602 (2011). |
[13] | P. Medley, D. M. Weld, H. Miyake, D. E. Pritchard, and W.Ketterle, Spin Gradient Demagnetization Cooling of Ultracold Atoms, Phys. Rev. Lett. 106, 195301 (2011). |
APA Style
Jitendra Kumar Barthakur. (2015). Limit of Low Temperatures, Freeze Decay, Dissipation of Matter, Harvest of Cold Energy. American Journal of Modern Physics, 4(5), 217-220. https://doi.org/10.11648/j.ajmp.20150405.11
ACS Style
Jitendra Kumar Barthakur. Limit of Low Temperatures, Freeze Decay, Dissipation of Matter, Harvest of Cold Energy. Am. J. Mod. Phys. 2015, 4(5), 217-220. doi: 10.11648/j.ajmp.20150405.11
AMA Style
Jitendra Kumar Barthakur. Limit of Low Temperatures, Freeze Decay, Dissipation of Matter, Harvest of Cold Energy. Am J Mod Phys. 2015;4(5):217-220. doi: 10.11648/j.ajmp.20150405.11
@article{10.11648/j.ajmp.20150405.11, author = {Jitendra Kumar Barthakur}, title = {Limit of Low Temperatures, Freeze Decay, Dissipation of Matter, Harvest of Cold Energy}, journal = {American Journal of Modern Physics}, volume = {4}, number = {5}, pages = {217-220}, doi = {10.11648/j.ajmp.20150405.11}, url = {https://doi.org/10.11648/j.ajmp.20150405.11}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajmp.20150405.11}, abstract = {Background: The gas laws assert that at “absolute zero” or 0 K, the gaseousness of the gases ends. Experimentally, gases become liquid or solid at 0 K. However, (i) 0 K is not the lowest limit of temperature; and (ii) at 0 K, the value of entropy is not zero. Activity continues at 0 K. There is (a) “Zero-point” energy; (b) the principle of “indeterminacy” holds; (c) 0 K is not the lower limit of “critical points” of the fluids and solids phases; (d) the structures of atoms comport in “clusters”; (e) electronic energy “mismatch” in superconductivity; and other phenomena stand against zero entropy at 0K. Purpose: Dissipation of matter means dissipation of energy. It may be possible to harvest the dissipating energy at below 0 K temperature for the use of human beings. Method: A number of statistical equations anchor at zero entropy at 0K. This anchor is arbitrary. At 0 K, gas stays as liquid, solid or plasma. Argumentatively, much below that temperature there is liquid–limit–temperature (LLT) where all liquids become solids or plasma. Below LLT, there is solid–limit-temperature (SLT) where freeze decay of matter sets in. At SLT, the articles and sub-particles constituting an atom dance away in to space. Result: Matter exists in the range between very cold temperature and very hot temperature. When matter dissipates then energy disperses with the dissipating matter. Conclusion: Laboratories need to reach the SLT temperature empirically and find means to harvest the dissipating energy.}, year = {2015} }
TY - JOUR T1 - Limit of Low Temperatures, Freeze Decay, Dissipation of Matter, Harvest of Cold Energy AU - Jitendra Kumar Barthakur Y1 - 2015/07/30 PY - 2015 N1 - https://doi.org/10.11648/j.ajmp.20150405.11 DO - 10.11648/j.ajmp.20150405.11 T2 - American Journal of Modern Physics JF - American Journal of Modern Physics JO - American Journal of Modern Physics SP - 217 EP - 220 PB - Science Publishing Group SN - 2326-8891 UR - https://doi.org/10.11648/j.ajmp.20150405.11 AB - Background: The gas laws assert that at “absolute zero” or 0 K, the gaseousness of the gases ends. Experimentally, gases become liquid or solid at 0 K. However, (i) 0 K is not the lowest limit of temperature; and (ii) at 0 K, the value of entropy is not zero. Activity continues at 0 K. There is (a) “Zero-point” energy; (b) the principle of “indeterminacy” holds; (c) 0 K is not the lower limit of “critical points” of the fluids and solids phases; (d) the structures of atoms comport in “clusters”; (e) electronic energy “mismatch” in superconductivity; and other phenomena stand against zero entropy at 0K. Purpose: Dissipation of matter means dissipation of energy. It may be possible to harvest the dissipating energy at below 0 K temperature for the use of human beings. Method: A number of statistical equations anchor at zero entropy at 0K. This anchor is arbitrary. At 0 K, gas stays as liquid, solid or plasma. Argumentatively, much below that temperature there is liquid–limit–temperature (LLT) where all liquids become solids or plasma. Below LLT, there is solid–limit-temperature (SLT) where freeze decay of matter sets in. At SLT, the articles and sub-particles constituting an atom dance away in to space. Result: Matter exists in the range between very cold temperature and very hot temperature. When matter dissipates then energy disperses with the dissipating matter. Conclusion: Laboratories need to reach the SLT temperature empirically and find means to harvest the dissipating energy. VL - 4 IS - 5 ER -