Effects of Vertical DIC Distribution on Storage Efficiencies of Direct Injection of CO2 into the Ocean Baixin Chen, M. Nishio, and M. Akai National Institute of Advanced Industrial Science and Technology (AIST), 1-2-1 Namiki, Tsukuba East, Tsukuba 305-8564, Japan 1 Why ocean sequestration? Large capacity (IPCC Srpt. on CCS 05) : “Roughly 2,300 to 10,700 GtCO2 would be added to the ocean (above the natural pre-industrial background) in equilibrium with atmospheric CO2 stabilization concentrations ranging from 350 ppm to 1000 ppm, regardless of whether the CO2 is initially released to the ocean or the atmosphere.” Actually, it is an artificially acceleration of natural oceanic uptaking of CO2 across air/sea interface. Over the past 200 years the oceans have taken up 500 GtCO2 from the atmosphere out of 1300 GtCO2 total anthropogenic emissions. . 2 Questions: Assessments on CO2 Ocean Sequestrations How long the CO2 injected could be kept in the ocean ? (efficiency) Is it safe for marine organisms and animals? (bio-impacts in near and far fields) The long-term impacts on global ecosystem ( ? ) 3 How to perform (IPCC Srpt. on CCS, 2005) 4 Injection of CO2 by moving-ships 5 CO2 Injection Nozzle & Droplet Size Distribution (Minamiura et al., GHGT-7, 2004) Nozzle and CO2 drops from Lab. Exp. Drop deformation Hydrate layer formed at the interface 6 How long the CO2 injected could be kept in the ocean ? Efficiency or retention : OGCMs (depth, locations) Caldeira et al. (GRL, JGR , 02) Orr et al. (Climate Change 02 and GHGT-5-00 ) ….. Box models (depth, bio-chemical systems) Herzog et al. (Climatic Change, 2003) Sohma et al, (JGR, 20050) …. In this study : If the injection parameters play the role on storage efficacy? 7 How to handle the injection parameters ? 1. Plume dynamics (coupling the injection parameters and currents) in short-term 2. For long-term efficiency, By OGCMs for long-term Using fine resolution: 10th meters vertically (Very difficult if not impossible currently) Nesting grids systems Good and will be trying By Box models OK (How about the horizontal transportation roles?) In this study : Implemented the initial vertical distribution of DIC from (1) to the existed data from (2). 8 Effect of injection parameters on storage efficiency: 1 C (t ) C 0 (h, t ) P[ x(h)]dx 0 C (t ) : the storage efficiency with an initial vertical distribution (pdf) C 0 (h, t ) : the storage efficiency without initial vertical distributions (OGCM data). h : the depth of the ocean (m) t : time (year) P[x(h)] : the mass pdf of DIC initial vertical distributionas a normalized depth (x (h)). 9 Long-term storage efficiency data interpolated from OGCMs 10 The data can be interpolated numerically (Caldeira et al. GRL 2002) Injection site: Tokyo Injection site: Tokyo T > 100 years T = 120 - 500 yrs T < 100 years T = 20 - 100 yrs 11 Initial Vertical Distributions of DIC produced by coupling injection parameters with ocean current from two-phase models 12 Near-field Two-phase Model Ocean surface Towing pipe Initial DIC distribution Turbulent diffusion X3 CO2 droplet Dynamics and biological impacts Injection ports installed nozzles X1 Can go to the bottom 13 Evolution of DIC Plumes T=1.0 min 1.34 1.26 1.17 0.89 0.65 0.00 (Chen et al., JGR, 05) T=23 min T=70 min Outline of CO2 Droplet Plume CO2 Rich-water Plume Injection rate : 100 kg/sec Initial drop size: 15 mm Injection depth : 2000 m Injection port : Horizontal 14 X=10 m X=180 m X=10 m X=10 m Vertical distributions of DIC Injection site: Tokyo at Depth of 2000 m 15 Effect of initial DIC vertical distribution on efficiency 16 CO2 Injection Parameters Injection type: Moving-ship Injection rate: 100kg/sec by moving-ship (0.1 Ggt C /year) Droplet sizes: 5, 10, 15, 20, 30, 40 mm Injection depth: 1000, 1500, 2000, 2500 m Injection site: Near Tokyo (T, S and current data ) 17 Effects of initial droplet size on efficiency Injection site: Tokyo 18 Effects of injection parameters on efficiencies Injection site: Tokyo Time : 500 yrs S 1.0 c co 19 Efficiency and (Sensitivity) Injection depth H (m) By 8 OGCMs (Orr et al. GHGT-5) By 8 sites (MOM) (Tokyo, New York, Bombay …, By Caldeira et al. GRL 2002) By droplet sizes (D0 = 5 – 40 mm) 800 1500 15 – 37 (+0.42) 26 – 57 (+0.35) 50 – 82 (+0.25) 15 – 30 (+0.33) 40 – 57 (+0.17) 70 – 89 (+0.10) 20 – 25 (0.21)* 38 – 47 (0.20) * : H = 1000 m and D0 = 5 – 10 mm; 2000 50 – 60 (0.11) 3000 62 – 72 (0.10)** ** : H = 2500 m 20 Conclusions & discussions Within 500 years after releasing CO2 at rate of 0.1 Ggt C /year by moving-ship: Efficiency is related with not only depths and sits but also drop size injected. For droplets size D0 = 5 – 40 mm, the storage efficiencies could be reduced by range of 5% to 20% if release depth less than 2600m due to the rising plumes. Implement of DIC vertical pdf into OGCM for further checking. (Nesting grids system ?) The roles of injection parameters on biological impacts in near-field should is another challenge. 21 Thank you ! 22 In this study: Assessments on CO2 Ocean Sequestrations How long it could be kept in the ocean ? (efficiency) OGCMs (depth, locations) (Caldeira et al. in GRL, JGR 02; Orr et al. in Climate Change 02 and GHGT-5-00; …..) Box models (depth, bio-chemical systems) (Sohma et al, JGR-05, ….) How about the injection parameters? Is it safe for marine bio-masses? (bio-impacts) Lab. Exps. (Acute injury of fishes, Mortality and Injury of zooplankton by Portner; Shirayama; Ishimatsu; JO and IPCC SRPT. on CCS) for Near-field and short-terms. Long-term impacts on bio-eco system ( ? ) Do the Injection parameters play the role ? The impacts on global ecosystem ( ? ) 23 Methodologies: Implement the near-filed two-phase box model to the OGCM by: Provide the initial vertical distributions of DIC from near-filed model Use data of long-term storage efficiency from OGCMs and Box models to estimate the effects of initial-vertical DIC distribution. because the time scales : dtOGCM (2 ~ 3 hrs) > Tdiss (1~ 1.5 hrs) We checked the injection depths and D0s for two injection types (horizontal and vertical injection ports) at a fixed injection rate (100kg/sec). 24 Model validation (vs field Exp data by P. Brewer et al. 2002) 1.00 Modeling Prediction (Droplet A) Droplet Diameter (cm) Modeling Prediction (Droplet B) 0.80 0.60 0.40 0.20 :Observation Data of Droplet A (P. Brewer et al) :Observation Data of Droplet B (P. Brewer et al) 0.00 10 25 40 55 70 Elapsed Time (min) 25 Ascending /Descending of CO2 droplet in the ocean Ascending /descending Distances (m) 800 Release depth: 1000m Release depth: 2000m 600 Release depth: 2895m 400 200 0 -200 -400 Release depth: 2900m -600 Release depth: 3000m -800 0 3 6 9 12 15 18 21 24 Initial Diameter of CO2 Droplet (mm) 26 Model of an Individual CO2 Droplet (dissolution and movement) c d ln( mc ) dur s 3ur 2 (( 1.0 )g Cd ) ur dt c s 4D dt dD 1 D dc 2 ShD f Cs ( ) dt c 3 dt D Key Parameters: •Sh : Sherwood number •Cs: The solubility •α : The effective area coefficient •Cd: Drag coefficient 27 Sub-models of drag coefficient (Lab. data from Dr. Ozaki) 4.5 Drag Coefficient Cdr and Cdd 4.0 Terminal velocity of CO2 droplet (cm s-1) 20 : Cdr Rigid spheres Eq. (2) : Cdd Rigid spheres with deformation Eq.(1) 3.5 3.0 O: P=10.1MPa;T=275K O: P=15.1MPa;T=278K O: P=20.1MPa;T=278K Exp data (Ozaki et al) 2.5 2.0 1.0 0.5 Exp Data (Ozaki et al) 10 : Cdr Rigid spheres Eq. (2) 0 0 :Cdd Rigid spheres with deformation Eq.(1) 5 10 15 20 25 CO2 Droplets Diameter (mm) 1.0 1.5 2.0 2.5 3.0 Logarithmic Reynolds Number Re 15 Re 5 1.5 0.0 O: P=10.1MPa;T=275K O: P=15.1MPa;T=278K O: P=20.1MPa;T=278K Du r w ur =|ud – uw| The relative velocity 3.5 Cdd Cdr( Aeff / Aeq )Cd Cdr 24( 1 0.125 Re 0.72 ) / Re (1) (2) ( Aeff / Aeq )Cd 1.0 ( 5.6419 8.3484 10 3 Re 1.4596 10 6 Re 2 ) 10 4 Re 28 Near-filed Bio-impacts for two CO2 release types Elapsed time: 180 min Vertical release type Horizontal release type 29
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