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Physics · Ch 8 — Heat and Thermodynamics

Heat Transfer

8.2.7

Heat Transfer

There are three distinct modes by which heat physically moves. Conduction is direct transfer through matter in contact, from hot to cold, without bulk motion of the material -- quantified by thermal conductivity KK, defined through the steady-state flow rate Qt=KA ΔTL\dfrac{Q}{t}=\dfrac{KA\,\Delta T}{L} across a slab of area AA, thickness LL, temperature difference ΔT\Delta T (Figure 8.11; SI unit W m⁻¹K⁻¹); Table 8.3 shows diamond and silver conduct extremely well while air and cork are extremely poor conductors, which is why cookware uses metals like aluminium and copper. Convection is heat transfer by the actual bulk movement of fluid molecules, driven by density differences created when part of a fluid is heated (illustrated by the sea-breeze/land-breeze cycle, arising from land's lower specific heat than water). Radiation is heat transfer purely by electromagnetic waves, requiring no medium at all …

Figure 8.11Steady-state heat flow by conduction

What this figure shows. A rectangular slab of material of thickness d and cross-sectional area A, with its left face held at a higher temperature T2 and its right face held at a lower temperature T1 (T2 > T1), and an arrow labelled Q showing the direction of steady heat flow from the hot face through the material to the cold face. The figure sets up the geometry behind the thermal-conductivity formula Q/t = KA(ΔT)/L, where the heat flow rate depends on the material's conductivity K, the cross-sectional area A, the temperature difference across the …

Table 8.3Thermal conductivities of some materials at 1 atm
MaterialThermal Conductivity (W m⁻¹K⁻¹)MaterialThermal Conductivity (W m⁻¹K⁻¹)
Diamond2300Water0.56
Silver420Human tissue0.2
Copper380Wood0.17
Aluminum200Helium0.152
Steel40Cork0.042