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PHYS2403 Simulation Lab

Experiment 8: Mantle Convection & Plate Tectonics

Despite being solid silicate rock, the Earth's mantle behaves as a highly viscous fluid over millions of years, convecting heat away from the hot core. This convective circulation is the engine driving plate tectonics. Use this simulation to examine convection onset, mantle plumes, slab subduction, and heat flow.

Rheology Settings

logΣ(viscosity)10^21.0 Pa·s
Mantle viscosity. Lower viscosity = faster flow (higher Ra).
Temp Contrast (ΔT)1500 K
Tectonic Injections

Mantle Temperature & Velocity FieldRa = 0.00e+0

Cold Surface Lithosphere (T=0)
Hot Core-Mantle Boundary (T=1)

Mid-Depth Temperature

Tracks mixing efficiency. Steady at 0.50 for conduction; oscillates for convection.

Conductive 0.51.00.50.0

Thermal Convection Physics

Critical Rayleigh Number

In flat layer models, convection occurs only when the buoyancy forces overcome viscous resistance and thermal diffusion. This onset is marked by the critical Rayleigh number, which is typically Ra_crit ≈ 1000. For Ra < 1000, heat transport is completely conductive and the temperature profile remains linear.

Solid State Creep

Although the Earth's mantle is composed of solid silicate minerals, high temperatures and confining pressures allow the rock to deform slowly by solid-state creep. Over geological timescales (tens of millions of years), this slow movement allows the mantle to flow and circulate, transferring core heat to the surface.