Fluid flow dynamics in CO2 sequestration in deep saline aquifers

Slides:



Advertisements
Similar presentations
Solution of Benchmark Problems for CO 2 Storage Min Jin, Gillian Pickup and Eric Mackay Heriot-Watt University Institute of Petroleum Engineering.
Advertisements

FOR FURTHER INFORMATION Figure 1: High-level workflow for the assessment of potential interaction of CO 2 geological storage with other basin resources,
Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corporation,
Field-scale simulations of CO 2 injection in saline aquifer in north Taiwan Presenter:Adviser: Date:2010/12/31 Date:2010/12/31.
Hydrodynamic analysis of spreading regimes and multi-component gas diffusion in the underground storage of radioactive wastes I.Panfilova, A.Pereira, S.C.Yusuf,
Example: Electrokinetic valve
Carbon Deposition in Heterogeneous Catalysis
10. In-Situ Stress (Das, Chapter 9)
INFLUENCE OF CAPILLARY PRESSURE ON CO 2 STORAGE AND MONITORING Juan E. Santos Work in collaboration with: G. B. Savioli (IGPUBA), L. A. Macias (IGPUBA),
Fluidyn FLOWCOAST FLOOIL 3D Fluid Dynamics Model to Simulate Oil slick movement in coastal waters or rivers FLOOIL.
Carbon Storage. Presentation titlePage 2 Overview of Geological Storage.
© NERC All rights reserved CCS main geological issues Storage capacity Injectivity Containment.
Imbibition Assisted Recovery
Increasing atmospheric concentrations of greenhouse gases are known to be causing a gradual warming of the Earth's surface and potentially disastrous changes.
Enclosure Fire Dynamics
Mathematics of non-Darcy CO 2 injection into saline aquifers Ana Mijic Imperial College London Department of Civil and Environmental Engineering PMPM Research.
ESS 454 Hydrogeology Instructor: Michael Brown
Press the button to start Permeability Permeability Home DevelopersReferencesSummary 1: What is Permeability 2: The Darcy Law 3: Measurements Back Next.
Predicting Vapor Intrusion Risks in the Presence of Soil Heterogeneities and Anthropogenic Preferential Pathways Brown University Ozgur Bozkurt, Kelly.
Earth Science Division E RNEST O RLANDO L AWRENCE B ERKELEY N ATIONAL L ABORATORY B ERKELEY L AB 9/30/03 G. Michael Hoversten Sally Benson Erika Gasperikova.
Upscaling of two-phase flow processes in CO 2 geological storage Orlando Silva (1), Insa Neuweiler 2), Marco Dentz (3,4), Jesús Carrera (3,4) and Maarten.
LA-UR Assessing wellbore leakage and its potential impact with CO 2 -PENS Rajesh J. Pawar Los Alamos National Laboratory.
1:1 scale wellbore experiment for a better understanding of well integrity in the context of CO 2 geological storage, Mont Terri underground rock laboratory.
Modeling of Rock Structure Changes due to Stress Induced by CO 2 Sequestration EGEE 520 – 2007 Denis Pone.
Salt precipitation in porous media and multi-valued solutions G. G. Tsypkin Institute for Problems in Mechanics RAS, Moscow, Russia Petroleum engineering.
Geometry Group Summer 08 Series Toon Lenaerts, Bart Adams, and Philip Dutre Presented by Michael Su May
19 Basics of Mass Transport
Is there really enough space to “put it back”
Ran Qi, Valcir T Beraldo, Tara C LaForce, Martin J Blunt Design of CO 2 storage in aquifers 17 th Jan Imperial College Consortium on Pore-Scale Modelling.
PRINCIPLES OF GROUNDWATER FLOW. I.Introduction “Groundwater processes energy in several forms”
Lecture 20 Ground Water (3) Ground water movement
Class 8. Oceans Figure: Ocean Depth (mean = 3.7 km)
CE 3354 Engineering Hydrology Lecture 21: Groundwater Hydrology Concepts – Part 1 1.
(Z&B) Steps in Transport Modeling Calibration step (calibrate flow & transport model) Adjust parameter values Design conceptual model Assess uncertainty.
Review Session 3. Advection Advection causes translation of the solute field by moving the solute with the flow velocity In 1-d all is does is shift the.
The Impact of SCCO 2 Injection Rate on Recovery efficiency from Gas- Condensate Reservoirs: Laboratory Investigation H. Sidiq, A. Al-bari, R. Amin September.
Recent progress and big ideas on geologic sequestration US/international perspective Susan D. Hovorka Gulf Coast Carbon Center Jackson School of Geosciences.
SHALE OIL EXTRACTION AND CO2 SEQUESTRATION BY A NOVEL METHOD OF HOT GAS INJECTION Michael Youtsos – Energy Group Cambridge University Engineering Department.
Underground Natural Gas Storage: ensuring a secure and flexible gas supply Jean-Marc Leroy GSE President Gas Coordination Group - 13 January 2010.
Geologic Sequestration: the Big Picture Estimation of Storage Capacity or How Big is Big Enough Susan Hovorka, Srivatsan Lakshminarasimhan, JP Nicot Gulf.
Lawrence Berkeley National Laboratory Earth Sciences Division 1 Cyclotron Road, MS Berkeley, CA D modeling of fault reactivation.
Methods  Two codes were coupled together to establish a robust simulator for thermo-hydro-mechanic-chemical coupling issue raised in CCS projects, as.
Date of download: 9/17/2016 Copyright © ASME. All rights reserved. From: Feasibility Investigation and Modeling Analysis of CO2 Sequestration in Arbuckle.
This study processes the optimization of heat extraction under the varied pressure and flow rate. Based on the validated model, two kinds of test tube.
PHILIP H. STAUFFER HARI S. VISWANTHAN RAJESH J. PAWAR MARC L. KLASKY
Chapter 5 Pressure Transient Testing (I)
Variable Density Flow and Transport in Tsunami Impacted Coastal Aquifers; Laboratory Investigations in Saturated Porous Media Meththika Vithanage1,2, Tissa.
Design of Port Injection Systems for SI Engines
Hasan Nourdeen Martin Blunt 10 Jan 2017
超臨界CO2在增強型地熱系統儲集層中取熱之研究-子計畫三 CO2在增強型地熱系統取熱模型之建構及效能分析
Dual Mesh Method in Dynamic Upscaling
Lecture 20 Ground Water (3) Ground water movement
Date of download: 11/13/2017 Copyright © ASME. All rights reserved.
Date of download: 12/31/2017 Copyright © ASME. All rights reserved.
Introduction Concern: intrusion into confined aquifer in glacial sediments.
Impact of Flowing Formation Water on Residual CO2 Saturations
Modeling and experimental study of coupled porous/channel flow
Potential for Geological Carbon Sequestration using deep saline aquifers in the Illinois Basin GIS Term Project Julien Botto.
Tarmat Layer Geo-mechanical Behavior under Producing Oilfield
Reactive transport of CO2 in a brine cavity
SENSITIVITY ANALYSIS OF THE PETROPHYSICAL PROPERTIES VARIATIONS ON THE SEISMIC RESPONSE OF A CO2 STORAGE SITE Juan E. Santos Instituto del Gas y del Petróleo,
in Fixed-bed Tubular Reactor
SERDP SYMPOSIUM 2008 POSTER NO. 138
COMSOL Simulation of Air Pollutant Particle Transmission in a Building
Introduction to Effective Permeability and Relative Permeability
Presented by: Brad Cross, ERM October, 2018
Lattice Boltzmann Simulation of Water Transport in Gas Diffusion Layers of PEMFCs with Different Inlet Conditions Seung Hun Lee1, Jin Hyun Nam2,*, Hyung.
A. Dollari*, Ch. Chatzichristos and A. G. Yiotis
Product design from PRS to Prototype using Comsol Multiphysics
Priyabrata Mandal, Priya Goel, Anusha Chandra, Dr. Sujay Chattopadhyay
Presentation transcript:

Fluid flow dynamics in CO2 sequestration in deep saline aquifers A. Mukherjee1, P. Dutta2 1. Department of Mining Engineering, IIEST Shibpur, Howrah, WB, India INTRODUCTION: A 2 dimensional heterogeneous saline porous reservoir (Fig. 1) 700 m x 910 m was fabricated using COMSOL Multiphysics software, using Elder Darcy’s Law module using data from [1]. It emphasises on fluid flow nature following CO2 injection. Fig. 3(a) – (b) show the nature of mass transfer processes taking place. (a) (b) Figure 3. (a)Diffusive flux and (b)convective flux within reservoir. Fig 4 (a)-(d) shows the flow of CO2 after the plume reaches the maximum possible height. Figure 1. Reservoir geometry COMPUTATIONAL METHODS: Using Darcy’s law we got the following expressions for fluid flow [2]: where, ρ is the brine density (kg/m3), t is the time (s), ε is the porosity, u is the Darcy velocity. (a) (c) (b) (c) (d) Figure 4. Plume behaviour at initial stage of CO2 injection (a) at 0 year (b) 10 years (c) 150 years and (d) 1000 years. CONCLUSIONS: On injection CO2 starts to dissolve and migrate both laterally and vertically. The saturation of CO2 first increases and then decreases with time. The extent of plume spread was found to be larger when a fixed plume height was considered. This is because higher the plume height higher the areal exposure of CO2. RESULTS: Fig. 2(a) – (d) show the fluid flow for 2500 years in the formation. After 230 years, gas started migrating up to the second domain. By 550 years it reached the second domain and started to migrate further upwards reaching the third domain. CO2 was filled in domain 2 and 3 simultaneously owing to injection pressure and permeability effect. References: Wurdemann H, Moller F, Kuhn F, Heidug W, Borm G, Schilling FR, CO2SINK—From site characterisation and risk assessment to monitoring and verification: One year of operational experience with the field laboratory for CO2 storage at Ketzin, Germany, 4(6), 2010. comsol manual (a) (b) (c) (d) Figure 2 Spatial and temporal variation of CO2 in the reservoir at (a) 230 years (b) 550 years (c) 900 years and (d) 2500 years.