Abstract
When a body is exposed to unsteady or transient thermal conditions, its temperature changes gradually, and if the exposure conditions remain constant it will eventually come to a new steady state or equilibrium. The rate of this process depends on the mass and thermal properties of the exposed body, and on the heat transfer conditions. As a general rule the lighter a body is (i.e. the less mass) and the larger its surface is, the quicker it adjusts to a new temperature level, and vice versa. The temperature development is governed by the heat conduction equation (Eq. 1.29) with the assigned boundary conditions. It can be solved analytically in some cases, see textbooks such as [1, 2], but usually numerical methods are needed. This is particular the case in fire protection engineering problems where temperature generally varies over a wide range, often several hundred degrees.
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References
Holman J (1986) Heat transfer, 6th edn. McGraw-Hill Book Company, New York
Incropera FP, deWitt DP (1996) Fundamentals of heat and mass transfer, 4th edn. Wiley, New York
The European Committee for Standardisation, CEN (2005) EN 1993-1-2, Eurocode 3: design of steel structures—general rules—structural fire design. The European Committee for Standardisation, CEN, Brussels
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Wickström, U. (2016). Unsteady-State Conduction. In: Temperature Calculation in Fire Safety Engineering. Springer, Cham. https://doi.org/10.1007/978-3-319-30172-3_3
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DOI: https://doi.org/10.1007/978-3-319-30172-3_3
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