Thermal inertia
Thermal inertia is a term commonly used to describe the observed delays in a body's temperature response during heat transfers. The phenomenon exists because of a body's ability to both store and transport heat relative to its environment. Since the configuration of system components and mix of transport mechanisms (e.g. conduction, convection, radiation, phase change) varies substantially between instances, there is no generally applicable mathematical definition of closed form for thermal inertia.[1]. Materials with larger heat capacity are typically associated with a slower temperature response.
Whether thermal inertia is an intensive or extensive property depends upon context. Some authors have identified it as an intensive material property, for example in association with thermal effusivity. It can be calculated more generally as an extensive quantity for a building or other finite bounded system that functions for example as a thermal reservoir. A thermal time constant is then often useful as a simple parametrization for thermal inertia.
Description
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A system containing one or more components with large heat capacity indicates that dynamic, or transient, effects must be considered when modelling system behavior. Steady-state calculations, many of which produce valid estimates of equilibrium heat flows and temperatures without an accounting for thermal inertia, nevertheless yield no information on the pace of changes between equilibrium states. Nowadays the temporal behavior of complex systems may be precisely evaluated with detailed numerical simulation, or a thermal time constant estimated from a lumped system analysis.[2][3]: 627 A larger heat capacity generally means a longer time for the system to reach equilibrium. The transition rate also occurs in conjunction with a system's heat transfer properties.
Analogies of thermal inertia to the temporal behaviors observed in other disciplines of engineering and physics can sometimes be used with caution.[4] In building design, thermal inertia is also known as the thermal flywheel effect, and the heat capacity of a structure's mass (sometimes called the thermal mass) can produce a delay between diurnal heat flow and temperature which is similar to the delay between current and voltage in an AC-driven RC circuit. Thermal inertia is less directly comparable to the mass-and-velocity term used in mechanics, where inertia restricts the acceleration of an object. In a similar way, thermal inertia can be a measure of heat capacity of a mass, and of the velocity of the thermal wave which controls the surface temperature of a material.
Thermal effusivity
[edit]For a semi-infinite rigid body where heat transfer is dominated by the diffusive process of conduction only, the thermal inertia response at a surface can be approximated from the material's thermal effusivity (e). It is defined as the square root of the product of the material's bulk thermal conductivity and volumetric heat capacity, where the latter is the product of density and specific heat capacity:[5][6]
- is thermal conductivity, with unit W⋅m−1⋅K−1
- is density, with unit kg⋅m−3
- is specific heat capacity, with unit J⋅kg−1⋅K−1
Thermal effusivity has units of a heat transfer coefficient multiplied by square root of time:
- SI units of W⋅m−2⋅K−1⋅s1/2 or J⋅m−2⋅K−1⋅s−1/2.
- Non-SI units of kieffers: Cal⋅cm−2⋅K−1⋅s−1/2, are also used informally in older references.[i]
When a constant flow of heat is abruptly imposed upon a surface, e performs nearly the same role in limiting the surface's initial dynamic "thermal inertia" response ( Udyn ≈ e ⋅ t −1/2 ) as the rigid body's usual heat transfer coefficient (U) plays in determining the surface's final static surface temperature.[7][8]
See also
[edit]References
[edit]- ^ Coined by the planetary geophysicist Hugh H. Kieffer.
- ^ Sala-Lizarraga, Jose; Picallo-Perez, Ana (2019). Exergy Analysis and Thermoeconomics of Buildings. Elsevier. pp. 272–273. doi:10.1016/B978-0-12-817611-5.00004-7. ISBN 9780128176115. S2CID 210737476.
- ^ Keshavarz, P.; Taheri, M. (2007). "An improved lumped analysis for transient heat conduction by using the polynomial approximation method". Heat and Mass Transfer. 43 (11): 1151–1156. doi:10.1007/s00231-006-0200-0.
- ^ Gerald R. North (1988). "Lessons from energy balance models". In Michael E. Schlesinger (ed.). Physically-based Modelling and Simulation of Climate and Climatic Change (NATO Advanced Study Institute on Physical-Based Modelling ed.). Springer. ISBN 978-90-277-2789-3.
- ^ Veto, M.S.; Christensen, P.R. (2015). "Mathematical Theory of Thermal Inertia Revisited" (PDF). 46th Lunar and Planetary Science Conference.
- ^ Dante, Roberto C. (2016). Handbook of Friction Materials and Their Applications. Elsevier. pp. 123–134. doi:10.1016/B978-0-08-100619-1.00009-2.
- ^ Carslaw, H.S.; Jaeger, J.C. (1959). Conduction of Heat in Solids. Clarendon Press, Oxford. ISBN 978-0-19-853368-9.
- ^ van der Maas, J.; Maldonado, E. (1997). "A New Thermal Inertia Model Based on Effusivity" (PDF). International Journal of Solar Energy. 19 (1–3): 131–160. Bibcode:1997IJSE...19..131M. doi:10.1080/01425919708914334.
- ^ Bunn, J.P. (1983). "The thermal response of a homogeneous slab to a constant heat flux". Building and Environment. 18 (1–2): 61–64. Bibcode:1983BuEnv..18...61B. doi:10.1016/0360-1323(83)90019-7.