Abstract
With the advent of temperatures near absolute zero, it is often claimed that at very low temperatures the effect of thermal wave propagation must be included by the hyperbolic heat conduction equation (HHCE). In this paper the non-linear convective–radiative HHCE is investigated. Opposite to common numerical analyses, analytical expressions are obtained for the temperature variations by the multi-step differential transformation method. Some conclusions about alteration of the specific heat of the material, temperature steeping, and Vernotte number have been formulated.
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Abbreviations
- \(A\) :
-
Dimensionless parameter describing variation of the thermal conductivity
- \(B\) :
-
Dimensionless parameter describing variation of the surface emissivity
- \(c\) :
-
Specific heat (J\(\,\cdot \,\)kg\(^{-1}\cdot \, \)K\(^{-1}\))
- \(c_\mathrm{a} \) :
-
Specific heat at the temperature \(T_\mathrm{a}\) (J\(\,\cdot \, \)kg\(^{-1}\cdot \, \)K\(^{-1}\))
- \(D\) :
-
Domain
- \(E\) :
-
Surface emissivity
- \(E_\mathrm{s} \) :
-
Surface emissivity at the temperature \(T_\mathrm{s} \)
- \(Fo\) :
-
Fourier number
- \(H\) :
-
Constant
- \(h\) :
-
Heat transfer coefficient (W\(\cdot \, \)m\(^{-2}\cdot \, \)K\(^{-1}\))
- \(Nr\) :
-
Dimensionless radiation–conduction parameter
- \(S\) :
-
Surface area (m\(^{2}\))
- \(T\) :
-
Temperature (K)
- \(t\) :
-
Temporal coordinate (s)
- \(T_\mathrm{a} \) :
-
Convection sink temperature (K)
- \(T_\mathrm{i} \) :
-
Initial temperature (K)
- \(T_\mathrm{s} \) :
-
Radiation sink temperature (K)
- \(V\) :
-
Volume (m\(^{3}\))
- \(Ve\) :
-
Vernotte number
- \(X(k)\) :
-
Transformed analytical function
- \(x(t)\) :
-
Original analytical function
- \(\alpha \) :
-
Measure of thermal conductivity variation with temperature (K\(^{-1}\))
- \(\beta \) :
-
Measure of surface emissivity variation with temperature (K\(^{-1}\))
- \(\rho \) :
-
Mass density (kg\(\cdot \, \)m\(^{-3}\))
- \(\sigma \) :
-
Stefan–Boltzmann constant (W\(\cdot \, \)m\(^{-2}\cdot \, \)K\(^{-4}\))
- \(\tau \) :
-
Thermal relaxation time (s)
- \(\theta \) :
-
Dimensionless temperature
- \(\theta _\mathrm{a} \) :
-
Dimensionless convection sink temperature
- \(\theta _\mathrm{s} \) :
-
Dimensionless radiation sink temperature
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Torabi, M., Yaghoobi, H. & Boubaker, K. Thermal Analysis of Non-linear Convective–Radiative Hyperbolic Lumped Systems with Simultaneous Variation of Temperature-Dependent Specific Heat and Surface Emissivity by MsDTM and BPES. Int J Thermophys 34, 122–138 (2013). https://doi.org/10.1007/s10765-012-1388-5
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DOI: https://doi.org/10.1007/s10765-012-1388-5