Skip to main content
Fig. 13 | Progress in Earth and Planetary Science

Fig. 13

From: Deep mantle melting, global water circulation and its implications for the stability of the ocean mass

Fig. 13

Results of model calculations on ocean mass history. Regassing parameters (rate of regassing and duration of regassing pulse (τ1)) are chosen to reproduce the inferred rapid sea-level drop (2–3 m/Myrs (in the last ~ 100 Myrs); Fig. 6). Degassing parameters include the area of cool regions with excess degassing (SC) and the delay time (τ2) for degassing since the beginning of excess regassing (and the plume upwelling velocity (~ 1 m/year)). a History of the water content in the MTZ (τ1 = τ2=100 Myrs). b Sea-level change corresponding to the model shown in (a) using a relation \( \Delta z\approx -\overline{z}\frac{M_{MTZ}\Delta {X}_{MTZ}}{W_{\mathrm{ocean}}} \) (Δz: sea-level change, \( \overline{z} \): average depth of the oceans (= 3730 m), MMTZ: mass of the MTZ (= 4 × 1023 kg)), ΔXMTZ: change in the water content of the MTZ; Wocean: mass of oceans (=1.4 × 1021 kg)). b Same as (a) except that τ1=100 Myrs, and τ2=200 Myrs. c Same as (b) except that τ1=100 Myrs, and τ2=200 Myrs. Observed sea-level changes (Fig. 7) can be explained with SC=(3–10) × 1010 (m2) (i.e., a region with 200–350 km diameter)

Back to article page