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Earth

The rock cycle

Bury a grain of sediment and watch it lithify at 2 km, turn metamorphic at 300 °C and begin to melt at 700 °C; exhume the melt and it crystallizes, rises and weathers back to sediment at the surface. Beside it five reservoirs trade mass at set rates: the total never changes, each has its residence time, and after a few hundred million years they settle at the proportions the rates dictate.

The rock cycle — Actual application image
Actual application image

What happens

Five reservoirs - magma, igneous, sediment, sedimentary and metamorphic rock - exchange mass by first-order fluxes: crystallization, weathering, lithification, metamorphism and melting. The total is conserved exactly, the steady state is the null vector of the rate matrix and each reservoir’s residence time is the inverse of its outgoing rate; RK4 in 0.01 Myr steps. Beside them a sample is buried or exhumed along a 25 K/km geotherm and changes type at explicit thresholds: lithification at 2 km and 60 °C, metamorphism at 10 km and 300 °C after 2 Myr in its type, melting at 700 °C, crystallization below it, weathering to sediment after 1 Myr at the surface.

Try this

Bury the grain and read the depths of each transition against the geotherm; exhume it and watch it crystallize, metamorphose and weather. Let the reservoirs run for a few hundred Myr and compare them with the steady state.

The model and its limits

First-order fluxes with constant rates, a linear geotherm, type changes at fixed thresholds; the sample’s path is kinematic. A teaching cycle, not a geochemical budget.

Equations used in the module
Equations
dM/dt = A·M,  Σ M = const
A·M_∞ = 0,  τ_i = 1/|A_ii|
T = T_0 + Γ·z
f_melt = (T − 700)/300

Related experiments

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Floating continents — Actual application image

Earth

Floating continents

Stand five columns of crust of different thickness in the mantle: each floats so that the pressure at depth is the same, the thick column standing high on a deep root. Load one with an ice sheet and watch it sink towards rho_i H / rho_m over the mantle’s relaxation time, then take the ice away and watch it rebound; shave a kilometre off the mountain and see its surface drop by only a sixth of that while its root shallows by the rest.

Mantle convection — Actual application image

Earth

Mantle convection

Heat a layer of slow fluid from below: at a small Rayleigh number a disturbance dies away and the conducting profile stays, above the critical value hot plumes rise and cold sheets sink and the Nusselt number climbs above one. Make the lid rigid and watch the surface stop moving and the heat transport fall; raise the Rayleigh number and the cells speed up and thin their boundary layers.

Rift valley formation — Actual application image

Earth

Rift valley formation

Stretch a continent and watch the crust thin over the rift, sag into a valley of stepped blocks and fill with sediment and water; the crust that leaves the window is booked, so crust plus exported area never changes, and the profile stays mirror-symmetric. Stretch fast over a viscous mantle and the floor lags its equilibrium depth; turn the sediment off and the valley floor lies deeper on the same basement.