“…One way of doing that is to model subduction and its surface response, and vary all key subduction parameters over their individual Earth-like ranges as done in e.g., Crameri et al (2017). Other generic modelling examples are quantifying crustal thickness at mid-ocean ridges for various spreading velocities (e.g., Katz, 2008), reproducing general magma dynamics (e.g., Spiegelman, 1993) or magma transport behaviour (e.g., Yamato et al, 2012), the onset of convection in a planetary mantle (Turcotte and Schubert, 2012, section 6.19), testing for what Rayleigh numbers and Clapeyron slopes a phase transition induces layered convection (e.g., Christensen and Yuen, 1985), quantifying the amount of entrainment of a dense layer into mantle plumes (e.g., Lin and van Keken, 2006a, b;Jones et al, 2016), investigating the plate tectonic regimes of a planet, which might range from a stagnant lid with only one plate to a mobile lid, similar to modern plate tectonics (e.g., Petersen et al, 2017;Lourenço et al, 2016;Lourenço et al, 2020), investigating under which conditions the flow in the Earth's outer core would cause an Earth-like dynamo (Christensen, 2011;Christensen and Wicht, 2015;Wicht and Sanchez, 2019), and mapping out the dominance of inner-core convection, rotation, or translation depending on its viscosity and conductivity (e.g., Deguen et al, 2013).…”