Unified mechanics theory
Unified mechanics theory[1][2][3][4] unifies the laws of newton and the laws of thermodynamics in the ab-initio level. As the result, the governing equation of any system automatically includes entropy generation [energy loss, dissipation, degradation, damage, etc.].[1] Unified mechanics theory introduces an additional linearly independent axis into Newtonian space-time coordinate system. The additional axis is called Thermodynamic State Index (TSI) axis. The TSI axis can have values between zero and one. Calculating the TSI axis coordinate of a material point requires deriving the thermodynamic fundamental equation of the material, without use of empirical curve fitting methods, using principals of physics and mathematics. Evolution of the TSI axis follows the Boltzmann entropy formulation of the second law of thermodynamics.
Universal laws
The universal law of Unified mechanics theory is given by[1]
Second law
where is mass, is velocity, is the thermodynamic state index.
Third law
where is the acting force, is the strain energy of the reacting system, is the displacement of the reacting system, is the stiffness of the reacting system.
Thermodynamics state index
where is the thermodynamic index, is the user defined value of TSI, the molar mass, is the gas constant.
is the change in entropy
When a material in ground (reference) state, it is assumed to be free of any possible defects. It can be assumed that “damage” in a material is equal to zero. Therefore TSI will be . However does not have to be taken as zero initially. In the final stage, material reaches a critical thermodynamic state, such that entropy is maximum. At this stage, entropy production rate will become zero, and . The function of is to adequately capture the specimen’s critical states of interest. For example, in the electromigration analysis of microelectronics solder joint, is used because 10% change in electrical resistance is considered failure in microelectronics.[5]
Thermodynamic state index coordinate system
The following example can explain this coordinate system
A 5-year-old boy with terminal illness and a 100-year-old sick person would have different coordinates in the time axis. But they have the same coordinate on TSI axis. Because using Newtonian space-time coordinates without incorporating thermodynamics, the physical state of a system [ a person] cannot be defined. On the other hand, in the unified mechanics theory their thermodynamic state is represented by the TSI axis in addition to the space-time coordinates. On TSI axis at , 5-year-old boy with terminal illness and a sick 100-year-old man will have the same thermodynamic state index coordinate. Essentially, a person’s age according to calendar does not give any information about that person’s thermodynamic physical state.[1]
Major difference between Newtonian Classical Mechanics and Unified Mechanics
- In Newtonian mechanics there is no axis to define derivative with respect to entropy. As a result all derivatives with respect to entropy are assumed to be zero.
- In Newtonian mechanics entropy generation must be defined with an empirical function or pseudo-force (like a damping force in structural dynamics). In Unified mechanics entropy generation is included in the universal laws of motion. Hence no empirical curve fitting dissipation/degradation/void/fatigue/failure/damage evolution functions or pseudo-dissipation forces (like damping) are needed. However, the unified mechanics theory does require derivation of the fundamental equation.
Applications
Unified mechanics theory based model is a model that uses entropy as a damage metric with a pure physics-based damage evolution function.[6] It has been extensively studied and experimentally validated in the field of fatigue life prediction in the past 15 years, including the fatigue life under thermomechanical loading,[3][7][8] electrical-thermal-mechanical loading,[9][10][11] and fatigue life prediction in particulate composites.[12][13]
References
- ↑ Jump up to: 1.0 1.1 1.2 1.3 Basaran C (2021). Introduction to unified mechanics theory with applications. Cham: Springer. ISBN 978-3-030-57772-8. OCLC 1236262479. Search this book on
- ↑ Bin Jamal MN, Lee HW, Rao CL, Basaran C (2021-02-26). "Dynamic Equilibrium Equations in Unified Mechanics Theory". Applied Mechanics. 2 (1): 63–80. doi:10.3390/applmech2010005. ISSN 2673-3161.
- ↑ Jump up to: 3.0 3.1 Bin Jamal MN, Kumar A, Lakshmana Rao C, Basaran C (December 2019). "Low Cycle Fatigue Life Prediction Using Unified Mechanics Theory in Ti-6Al-4V Alloys". Entropy. 22 (1): 24. Bibcode:2019Entrp..22...24B. doi:10.3390/e22010024. PMC 7516445 Check
|pmc=value (help). PMID 33285799 Check|pmid=value (help). - ↑ Bin Jamal MN, Rao CL, Basaran C (2021-04-XX). "A unified mechanics theory-based model for temperature and strain rate dependent proportionality limit stress of mild steel". Mechanics of Materials. 155: 103762. doi:10.1016/j.mechmat.2021.103762. Check date values in:
|date=(help) - ↑ Basaran C, Li S, Hopkins DC, Veychard D (2009-07-XX). "Electromigration time to failure of SnAgCuNi solder joints". Journal of Applied Physics. 106 (1): 013707–013707–10. Bibcode:2009JAP...106a3707B. doi:10.1063/1.3159012. ISSN 0021-8979. Check date values in:
|date=(help) - ↑ Lee HW, Basaran C (2021-04-09). "A Review of Damage, Void Evolution, and Fatigue Life Prediction Models". Metals. 11 (4): 609. doi:10.3390/met11040609. ISSN 2075-4701.
- ↑ Temfack T, Basaran C (2015-10-XX). "Experimental verification of thermodynamic fatigue life prediction model using entropy as damage metric". Materials Science and Technology. 31 (13): 1627–1632. doi:10.1179/1743284715Y.0000000074. ISSN 0267-0836. Unknown parameter
|s2cid=ignored (help); Check date values in:|date=(help) - ↑ Egner W, Sulich P, Mroziński S, Egner H (2020-12-XX). "Modelling thermo-mechanical cyclic behavior of P91 steel". International Journal of Plasticity. 135: 102820. doi:10.1016/j.ijplas.2020.102820. Check date values in:
|date=(help) - ↑ Basaran, Cemal; Lin, Minghui; Ye, Hua (2003-12-01). "A thermodynamic model for electrical current induced damage". International Journal of Solids and Structures. 40 (26): 7315–7327. doi:10.1016/j.ijsolstr.2003.08.018. ISSN 0020-7683.
- ↑ Li S, Abdulhamid MF, Basaran C (2009-05-XX). "Damage Mechanics of Low Temperature Electromigration and Thermomigration". IEEE Transactions on Advanced Packaging. 32 (2): 478–485. doi:10.1109/TADVP.2008.2005840. ISSN 1521-3323. Unknown parameter
|s2cid=ignored (help); Check date values in:|date=(help) - ↑ Yao W, Basaran C (2013-09-14). "Computational damage mechanics of electromigration and thermomigration". Journal of Applied Physics. 114 (10): 103708–103708–12. Bibcode:2013JAP...114j3708Y. doi:10.1063/1.4821015. ISSN 0021-8979.
- ↑ Basaran C, Nie S (2007-02-XX). "A thermodynamics based damage mechanics model for particulate composites". International Journal of Solids and Structures. 44 (3–4): 1099–1114. doi:10.1016/j.ijsolstr.2006.06.001. Check date values in:
|date=(help) - ↑ Gunel E, Basaran C (2013-02-XX). "Influence of filler content and interphase properties on large deformation micromechanics of particle filled acrylics". Mechanics of Materials. 57: 134–146. doi:10.1016/j.mechmat.2012.10.012. Check date values in:
|date=(help)
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