Supporting information for: Changing tectonic controls on the long term carbon cycle from Mesozoic to present. Benjamin Mills, Stuart J. Daines & Timothy M. Lenton College of Life and Environmental Sciences, University of Exeter, Exeter, EX4 4QE, UK. Supporting Information 1 –COPSE model alterations. For this work we update a number of functions and forcings in the COPSE model. Silicate weathering is split into a ‘granite’ and ‘basalt’ contribution and an additional flux of carbon from the ocean to the crust is added to represent seafloor weathering. New forcings (BA, GA, CA) are added that represent the relative global area of basaltic, granitic and carbonate rocks, in order that this may influence the split between basalt and granite weathering. The degassing rate (D) forcing is updated in response to new data [1], and the uplift/erosion (U) forcing is modified so that it does not rely on input of strontium isotope ratios [2]. We also add a simple strontium cycle to the model. Full equations are documented below. Aside from the changes laid above, they follow the original COPSE model [3]. RO2 and RCO2 denote concentrations of oxygen and carbon dioxide relative to present day. Subscript zeros represent the present day size of fluxes and reservoirs. Model runs were performed using the MATLAB ODE suite variable timestep solvers [4]. List of fluxes: (* denotes fluxes that have been updated for this work, ** denotes new fluxes) 2 π πππ€ 5 πππππ€ 5 ππ₯πππ€ 0 0 0 Phosphorus weathering: πβππ π€ = ππβππ π€ (12 π πππ€ + 12 πππππ€ + 12 ππ₯πππ€ ) (1) P delivery to land surface: πππππ = πππππππππ β ππΈπΊ β πβππ π€ (2) Land organic carbon burial: ππππ = πππππ β πππππ β πΆπππππ (3) P delivery to oceans: ππ ππ = πβππ π€ − πππππ (4) Marine new production: πππ€π = 117 β min (16 , π) πππππ 0 π 1 (5) πππ€π 2 ) π0 Marine organic carbon burial: ππππ = πππππ ( Marine organic phosphorus burial: ππππ = Calcium-bound phosphorus burial: ππππ = πππππ ππππ Iron-sorbed phosphorus burial : ππππ = πππππ β Nitrogen fixation: ππππ₯ = πππππ₯ ((π Marine organic nitrogen burial: ππππ = Denitrification: (6) ππππ πΆππ ππ (7) ππππ (8) 0 (1−ππππ₯) (9) πππ₯ππππ (π−π/16) 0 −π0 /16) 2 ) ππππ πΆππ ππ (10) (11) ππππ₯ πππππ‘ = ππππππ‘ (1 + (1−π ππ₯ππππ )) (12) Temperature dependence of basalt weathering: πππππ = π 0.061(π−π0) {1 + 0.038(π − π0 )}0.65 (13) Temperature dependence of granite weathering: ππππππ = π 0.072(π−π0 ) {1 + 0.038(π − π0 )}0.65 (14) Temperature dependence of carbonate weathering: ππ = 1 + 0.087(π − π0 ) (15) Pre-plant silicate weathering: πππππππππ‘ = ππ β √π πΆπ2 Plant-assisted silicate weathering: ππππππ‘ = ππ β (1+π πΆπ2 ) (17) Pre-plant carbonate weathering: πππππππππ‘ = ππ β √π πΆπ2 (18) Plant-assisted carbonate weathering: ππππππ‘ = ππ β (1+π πΆπ2 ) (19) ππΆπ2 = πππππππππ‘ (1 − min(ππΈπΊ β π)) + ππππππ‘ β min(ππΈπΊ β π) (20) 0.4 2π πΆπ 2 0.4 2π πΆπ 2 (16) Climate forcing for silicates: 2 fCO2gran and fCO2bas result from the fCO2 function with plant-weathering feedbacks using fTgran and fTbas respectively. Climate forcing for carbonates: ππΆπ2 = πππππππππ‘ (1 − min(ππΈπΊ β π)) + ππππππ‘ β min(ππΈπΊ β π) Vegetation feedback: (πΆπ πππ−10) β 2 πππ−10) 2 ππΈπΊ = 2 β πΈ β (183.6+πΆπ (21) (π−π0 ) 2 (1 − ( ) ) β (1.5 − 0.5(π π2 )) β π πππππ (22) (πππππ −1+max(586.2π2 (ππ‘π)−122.102 ,0)) Evolution of plants: πππ£ππ = (πππππππππ‘ + (1 − πππππππππ‘ ) β π β ππΈπΊ) (23) Basalt weathering**: πππ π€ = %πππ 0 β ππ πππ€ β ππΆπ2πππ β ππΊ β πππ£ππ β π΅π΄ (24) Granite weathering**: πππππ€ = (1 − %πππ 0 ) β ππ πππ€ β ππΆπ2ππππ β ππΊ β π β πππ£ππ β πΊπ΄ (25) Silicate weathering*: π πππ€ = πππ π€ + πππππ€ (26) Carbonate weathering: πππππ€ = ππππππ€ β ππΆπ2 β ππΊ β π β πππ£ππ β πΏπ΄πΆπππ (27) Oxidative weathering: ππ₯πππ€ = πππ₯πππ€ β π β √π π2 (28) Marine carbonate carbon burial: ππππ = π πππ€ + πππππ€ (29) Seafloor weathering**: π ππ€ = ππ ππ€ β π· β (π πΆπ2 )πΌ (30) Pyrite sulphur weathering: ππ¦ππ€ = πππ¦ππ€ β π β πππ √π π2 Gypsum sulphur weathering: ππ¦ππ€ = πππ¦ππ€ β π β πΊππ β πππππ€ Pyrite sulphur burial: πππ π = ππππ π β π β π β ππππ πππ (31) 0 π 0 3 πΊππ πππππ€ 0 0 1 ππππ 0 (32) (33) π πΆπ΄πΏ β π0 πΆπ΄πΏ0 Gypsum sulphur burial: πππ π = ππππ π β Organic carbon degassing: πππππ = ππππππ (πΊ ) β π· Carbonate carbon degassing: πππππ = ππππππ (πΆ ) β π· β π΅ (34) πΊ (35) 0 πΆ 0 (36) Other calculations: Following COPSE, the global average surface temperature calculation is taken from the model of Caldeira and Kasting [5] and requires inputs of solar forcing, albedo and carbon dioxide concentration. Relative atmospheric O2: π π2 = π π0 (37) π +ππ2 π0 where kO2 = 3.762 πππ€π Ocean anoxic fraction: ππππ₯ = πππ₯ (1 − πππ₯ππππ (π π2 ) ( πππ€π0 ) , 0) Solar forcing: π= π0 (38) (39) π‘ π 1+0.38( ) where S0 = 1368Wm-2, τ=4.55x109 years. Following COPSE, the global average surface temperature calculation is taken from the model of Caldeira and Kasting [5] and requires inputs of solar forcing and carbon dioxide concentration. Albedo is calculated within the temperature function. Reservoir calculations: Ocean phosphate: ππ ππ‘ = πβππ π€ − ππππ − ππππ − ππππ 4 (40) ππ ππ‘ Ocean nitrate: = ππππ₯ − πππππ‘ − ππππ (41) Atmosphere/ocean carbon*: ππ΄ ππ‘ = πππππ + ππ₯πππ€ + πππππ + πΏπΌππππ − π πππ€ − ππππ − ππππ − π ππ€ + ππ¦ππ€ − πππ π (42) Ocean calcium (+ magnesium): ππΆπ΄πΏ ππ‘ = π πππ€ + πππππ€ + ππ¦ππ€ − ππππ − πππ π (43) Ocean sulphate: ππ ππ‘ = ππ¦ππ€ + ππ¦ππππ + ππ¦ππ€ + ππ¦ππππ − πππ π − πππ π (44) Buried organic C: ππΊ ππ‘ = ππππ − ππ₯πππ€ − πππππ (45) Buried carbonate C *: ππΆ ππ‘ = ππππ + π ππ€ − πππππ€ − πππππ (46) Buried pyrite S: ππππ ππ‘ = πππ π − ππ¦ππ€ (47) Buried Gypsum S: ππππ ππ‘ = πππ π − ππ¦ππ€ (48) Present day values: Source: Marine organic carbon burial: kmocb=4.5x1012 mol C yr-1 COPSE Calcium-bound P burial: kcapb=1.5x1010 mol P yr-1 COPSE Iron-sorbed P burial: kfepb=6x109 mol P yr-1 COPSE Nitrogen fixation: knfix=8.7x1012 mol N yr-1 COPSE Denitrification: kdenit=4.3x1012 Pyrite sulphur burial: kmpsb=5.3x1011 mol S yr-1 5 mol N yr-1 COPSE COPSE Gypsum sulphur burial: kmgsb=1x1012 Silicate weathering*: ksilw = 4.9x1012 mol C yr-1 for steady state Seafloor weathering**: ksfw = 1.75x1012 mol C yr-1 [6-8] Oxidative weathering: koxidw=7.75x1012 mol C yr-1 for steady state Reactive P weathering: kphosw=4.35x1010mol P yr-1 COPSE Pyrite sulphur weathering: kpyrw=5.3x1011 mol S yr-1 COPSE Gypsum sulphur weathering: kgypw=1x1012 mol S yr-1 COPSE Organic carbon degassing: kocdeg=1.25x1012 mol C yr-1 COPSE Carbonate carbon degassing: kccdeg=6.65x1012mol C yr-1 COPSE Atmosphere and ocean CO2: A0=3.193x1018 mol COPSE Ocean phosphate: P0=3.1x1015 mol COPSE Ocean nitrate: N0=4.35x1016 mol COPSE Ocean Ca (+Mg): CAL0 = 1.397x1019 mol COPSE Ocean sulphate: P0=4x1019 mol COPSE Atmosphere and ocean oxygen: O0=3.7x1019 mol COPSE Buried organic carbon: G0=1.25x1021 mol COPSE Buried carbonate carbon: C0=6.6x1021 mol COPSE Buried pyrite sulphur: PYR0=1.8x1020 mol COPSE Buried gypsum sulphur: GYP0=2x1020 COPSE 6 mol S yr-1 mol COPSE Ocean C:P burial ratio: CPsea = 250 mol/mol COPSE Ocean C:N burial ratio: CNsea = 37.5 mol/mol COPSE CO2-seafloor weathering feedback α ≈0.23 mol/mol Follows [9, 10] Forcings: Attributes: Solar forcing: π= π0 π‘ π 1+0.38( ) where S0 = 1368Wm-2, τ=4.55x109 years. (COPSE) Relative global CO2 degassing*: π· = 1 for present day, scaling relationship from [1] Relative uplift rate*: π = 1 for present day, follows [2, 11] Evolution of land plants: πΈ = 1 for present day (COPSE) Weathering effect of plant evolution: π = 1 for present day (COPSE) Carbonate burial depth: π΅ = 1 for present day (COPSE) Relative basaltic area**: π΅π΄ = 1 for present day (section 4 and main paper). Relative total land area: LArel = 1 for present day (GEOCARB) Relative carbonate land area: LACrel = 1 for present day (GEOCARB) Relative granite area: GA = LA – LAC – BAcont where BAcont is the total basaltic area on continents (i.e. total basaltic area minus island arc and ocean island contributions) and LA and LAC are the total land area and carbonate land area respectively, calculated by scaling the relative areas to the present day areas (estimated from total land area and silicate area [12]). 7 Paleogeographical runoff effect**: ππΊ = 1 for present day, follows [12] Supporting Information 2 – Strontium isotope system A simple strontium cycle is added to COPSE for this work, based on previous Sr box models [13, 14]. The system calculates concentrations of oceanic and sedimentary strontium in order to estimate seawater 87Sr/86Sr based on the other model parameters. Fluxes of strontium are tied to existing model variables via first-order scaling relationships. Mantle input of Sr and metamorphism of sediments are assumed to be proportional to the global degassing rate, D. We also assume that the rate of strontium burial in sediments relates to the concentration of strontium in the ocean and the rate of carbonate sediment deposition. This follows the treatment of other species in COPSE. Sr fluxes: πππ π€ Sr input from basalt weathering: πππππ π€ = ππππππ π€ β π Sr input from granite weathering: πππππππ€ = ππππππππ€ β π Sr input from sediment weathering: πππ πππ€ = ππππ πππ€ β π Seafloor weathering: πππ ππ€ = ππππ ππ€ β Burial in sediments: πππ πππ = ππππ πππ β Mantle input: ππππππ‘ππ = πππππππ‘ππ β π· (54) Sediment metamorphism: πππππ‘ππ = ππππππ‘ππ β π· (55) πππ π€ πππππ€ πππππ€ πππππ€ 8 πππππ€ π ππ€ ππ ππ€ ππππ πππ β πππππ πππ0 (49) (50) (51) (52) (53) Other calculations Although these is no fractionation of Sr isotopes associated with the input and output fluxes to the ocean, decay of 87Rb to 87Sr influences the 87Sr/86Sr ratio over long timescales (and is responsible for the differing 87Sr/86Sr values between different rock types). The decay process is represented explicitly in the model: 87 ππ/ 86ππππππππ‘π = 87 ππ/ 86πππππ πππ‘ = 87 ππ/ 86ππ0 + 87π π/ 86ππππππππ‘π (1 − π −ππ‘ ) 87 ππ/ 86ππ0 + 87π π/ 86πππππ πππ‘ (1 − π −ππ‘ ) (56) (57) For each rock type, the rubidium-strontium ratio is then calculated such that the observed present day 87Sr/86Sr ratio is achieved for each rock type after 4.5 billion years: 87 π π/ 86ππ = ( 87ππ / 86ππππππ πππ‘ − 87ππ/ 86ππ0 ) (58) 9 (1−π −πβ4.5×10 ) Sr reservoir calculations: Ocean Sr: ππππ ππ‘ = πππππππ€ + πππππ π€ + πππ πππ€ + ππππππ‘ππ − πππ πππ − πππ ππ€ (59) Sr in sediments : ππππ ππ‘ = πππ πππ − πππ πππ€ − πππππ‘ππ (60) Isotope ratios are calculated by creating reservoirs consisting of Sr concentrations multiplied by their isotopic ratios. This method is common in isotope mass balance studies [15, 16]. Here ππππ denotes the 87Sr/86Sr ratio of reservoir X. Ocean [Sr] x 87Sr/86Sr: ππππ_πππ ππ‘ = πππππππ€ β πππππππππ‘π + πππππ π€ β ππππππ πππ‘ + πππ πππ€ β ππππ πππππππ‘ + ππππππ‘ππ β πππππππ‘ππ − πππ πππ β ππππππππ − πππ ππ€ β ππππππππ (61) Crustal [Sr] x 87Sr/86Sr: 9 ππππ_πππ ππ‘ = πππ πππ β ππππππππ − πππ πππ€ β ππππ πππππππ‘ − πππππ‘ππ β ππππ πππππππ‘ (62) The isotopic ratio of 87Sr to 86Sr in the ocean is then calculated by dividing the new reservoir by the known concentration. The 87Sr/86Sr ratio for carbonate sediments is calculated in the same way, with an additional term to account for rubidium decay within the crust: ππππππππ = πππ_πππ πππ , ππππ πππππππ‘ = πππ_πππ πππ + 87π π/ 86ππππππππππ‘π (1 − π −ππ‘ ) Present day Sr fluxes: (63) Source: Basalt weathering ππππππ π€ = 1.3 × 1010 × %πππ 0 mol/yr [13, 17] Granite weathering ππππππππ€ = 1.3 × 1010 × (1 − %πππ 0 ) mol/yr [13, 17] Sediment weathering ππππ πππ€ = 1.7 × 1010 mol/yr [13] Mantle input πππππππ‘ππ = 7.3 × 109 mol/yr [13] Sediment metamorphism ππππππ‘ππ = 1.3 × 1010 mol/yr [13] Seafloor weathering ππππ ππ€ = 3.26 × 109 mol/yr for steady state Burial in sediments ππππ πππ = 3.404 × 1010 mol/yr for steady state Here the split between Sr input fluxes from basalt and granite is assumed to follow the same apportioning as in the carbon system (35% of silicate weathering is attributed to basalts [17]). Sr burial in carbonate sediments and burial as carbonatized basalt is assumed to also follow the same stoichiometry as the carbon system, with the total flux dictated by assuming present day steady state for oceanic Sr concentration. 10 Other constants: Source: Present day ocean Sr πππ0 = 1.2 × 1017 [13] Sediment Sr πππ0 = 5 × 1018 [13] 87 ππππππ πππ‘ = 0.705 [13] 87 πππππππππ‘π = 0.715 [13, 18] 87 πππππππ‘ππ = 0.703 [13] 87 87 0.066 for correct present day 87Sr/86Sr 87 87 0.1 for correct present day 87Sr/86Sr 87 87 0.26 for correct present day 87Sr/86Sr 87 87 Sr/86Sr basalt Sr/86Sr granite Sr/86Sr mantle Rb/86Sr mantle Rb/86Sr basalt Rb/86Sr granite Rb/86Sr sediments π π/ 86ππππππ‘ππ = π π/ 86πππππ πππ‘ = π π/ 86ππππππππ‘π = π π/ 86ππππππππππ‘π = 0.5 for correct present day 87Sr/86Sr (assuming crustal average 87Sr/86Sr of 0.73 [19]) Initial ocean 87Sr/86Sr is set at the model start point in accordance with data (87Sr/86Sr≈0.708 for 230Ma), initial sedimentary carbonate 87Sr/86Sr is set so that the model returns present day values for ocean 87Sr/86Sr. This requires sediment 87Sr/86Sr = 0.714 at 230Ma. Supporting information 3 – Additional model scenarios Figures S1-S4 are plotted below and are referred to in the manuscript. Some discussion is added here also. 11 Figure S1. Sensitivity to assumed present day seafloor weathering rate ksfw. Panels show the upper (a,b) and lower (c,d) estimates for present day seafloor weathering rate [6-8]. As would be expected, a higher rate of seafloor weathering results in lower stable CO2 concentration. Lower predicted 87 Sr/86Sr results from less radiogenic input from silicate weathering (less is required to balance CO2 degassing) and reduced carbonate weathering at lower temperatures. Here α=0.23 and uncertainty on basalt area and degassing rate result in the upper and lower boundaries. 12 Figure S2. Model results for Hay et al. [2006] uplift scenario [20]. Sharp rise in uplift rates over the Cenozoic result in rapid increase in 87Sr/86Sr. However this exceeds the rate shown in data. One solution may be that uplift was between the Hay et al., estimates and those used in the main paper (following Berner [2]). 13 Figure S3. Model runs for longer LIP emplacement times. As figure 8 but with LIP emplacement times (assumed to correspond to duration of degassing and seafloor weathering enhancement) taken from Courtilliot et al., [2003] [21], and shown in the LIP table below. Where emplacement time is unknown it is assumed to follow the average of the published times (~1.7Myrs). Timing is particularly important for the Ontong-Java plateau, which is the LIP with highest initial volume. Published emplacement timings for this LIP range from 500kyr to 3Myr [22], which our 1.7Myr assumption falls between. Longer emplacement times reduce the predicted CO2 perturbations as may be expected. However the Ontong-Java may still result in up to 50% increase in CO2. 14 Figure S4. Model runs for constant degassing rate, compared to the spatial weathering results of Lefebvre et al., [2013] (crosses) [23]. The spatial modelling of basalt weathering regimes is lacking in our work, due to the complex GCM climate dynamics required, which limit the timeframe in which a dynamic model can be run. Snapshots of terrestrial basalt weathering from the spatial model show much lower values at 65 and 15Ma, when compared to our model under the same (constant) degassing scenario. Granitic weathering follows a more similar pattern, but is lower in our model due to consideration of the seafloor weathering CO2 sink and our different results for basalt 15 weathering. The mismatch between results suggests that both LIP area decay and paleogeographic position are important for long term climate models. Supporting information 4 – Basalt area forcing The basalt area forcing as used in our model runs is attached as a .mat file. This includes the resulting upper, middle and lower estimates from figure 5, incorporating both the instant and delayed decay options. The time points are in Myrs. Supporting Information 5 – Phanerozoic LIP emplacements Estimation of terrestrial basaltic area requires information on the initial area and timings of large igneous province emplacements. Calculation of potential CO2 degassing relies on estimates of initial LIP volume. The attached excel table contains information on all large igneous provinces from 300Ma to present, and is based on the A10 database of the Large Igneous Provinces Commission (http://www.largeigneousprovinces.org/). Citation numbers in the excel table relate to the references here. For LIP volumes, red cells denotes where volumes have been estimated based on the volume-area relationship of the more recent, well-constrained LIPs: π = 3.2 × 105 β π 2×10 −6 π΄ where V is volume in km3 and A is area in km2. This approximation does not give a strong fit (r2=0.66), however the LIPs for which volume is estimated in this way to not contribute greatly to total LIP volume. All area estimates are taken directly, or inferred from literature data. The relevant publications are noted in the final column, where there is no reference, data comes directly from the A10 database. CO2 release is calculated from initial volume (see manuscript and [24]). 16 Supporting information references 1. Van Der Meer, D.G. et al., Plate tectonic controls on atmospheric CO2 levels since the Triassic. PNAS, 2014. 111: p. 4380-4385. 2. Berner, R.A., Inclusion of the weathering of volcanic rocks in the GEOCARBSULF model. American Journal of Science, 2006. 306: p. 295-302. 3. Bergman, N.M., T.M. Lenton, and A.J. Watson, COPSE: A new model of biogeochemical cycling over Phanerozoic time. American Journal of Science, 2004. 304(May): p. 397-437. 4. Shampine, L.F. and M.W. Reichelt, The Matlab ODE suite. SIAM J. Sci. 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