From: Thermal modeling of subduction zones with prescribed and evolving 2D and 3D slab geometries
Quantity | Symbol | Values, reference values and/or SI units |
---|---|---|
Velocity | \(\varvec{u}\) | \(u_\text {conv} = {5}\,\hbox {cm}\,\hbox {yr}^{-1}\) |
Dynamic pressure | p | \(\hbox {Pa}\) |
Temperature | T | \(T_0 = {273}\,\hbox {K}\), \(T_\text {max} = {1573}\,\hbox {K}\) |
Time | t | \(t_\text {slab} = {11}\,\hbox {Myr}\) |
Position | \(\varvec{x}\) | \(\hbox {km}\) |
Radial distance | r | \(r = \Vert \varvec{x} \Vert _2\) |
Radius of the Earth | \(r_0\) | \({6371}\,\hbox {km}\) |
Depth | d | \(d = r_0 - r\) |
Plate depth | \(d_\text {plate}\) | \({50}\,\hbox {km}\) |
Coupling depth | \(d_c\) | \({75}\,\hbox {km}\) |
Slab thickness | \(d_\text {slab}\) | \({200}\,\hbox {km}\) |
Dynamic viscosity | \(\eta\) | \(\text {Pa}\,\text {s}\) (Eq. (5)) |
Stress tensor | \(\varvec{\sigma }\) | \(\hbox {Pa}\) |
Density | \(\rho\) | \({\left\{ \begin{array}{ll} {2700}\,\hbox {kg}\,\hbox {m}^{-3} &{} \varvec{x} \in {\Omega }_\text {plate} \text { and } {0}\,\hbox {km} \le d < {40}\,\hbox {km} \\ {3300}\,\hbox {kg}\,\hbox {m}^{-3} &{} \text {otherwise} \end{array}\right. }\) |
Thermal conductivity | k | \({\left\{ \begin{array}{ll} {2.5}\,\hbox {W}\,\hbox {m}^{-1}\,\hbox {K}^{-1} &{} \varvec{x} \in {\Omega }_\text {plate} \text { and } {0}\,\hbox {km} \le d < {40}\,\hbox {km} \\ {3}\,\hbox {W}\,\hbox {m}^{-1}\,\hbox {K}^{-1} &{} \text {otherwise} \end{array}\right. }\) |
Heat capacity | \(c_p\) | \({1250}\,\hbox {J}\,\hbox {kg}^{-1}\,K^{-1}\) |
Radiogenic heat source | Q | \({\left\{ \begin{array}{ll} {1.3}\,\upmu \hbox {W}\,\hbox {m}^{-3} &{} \varvec{x} \in {\Omega }_\text {plate} \text { and } {0}\,\hbox {km} \le d < {15}\,\hbox {km} \\ {0.27}\,\upmu \hbox {W}\,\hbox {m}^{-3} &{} \varvec{x} \in {\Omega }_\text {plate} \text { and } {15}\,\hbox {km} \le d \le {40}\,\hbox {km} \\ {0} &{} \text {otherwise} \\ \end{array}\right. }\) |
Surface heat flux | \(q_\text {surf}\) | \({65}\,\hbox {mW}\,\hbox {m}^{-2}\) |