Modeling and Analysis of a Hydrogen Release in a Large Scale Facility

Slides:



Advertisements
Similar presentations
1 Application of for Predicting Indoor Airflow and Thermal Comfort.
Advertisements

J. Amdahl,, NTNU Dept, Marine Technology Beregning av ulykkeslaster for offshore stålkonstruksjoner – NFS Accidental Fires Design criteria.
JET A VAPORIZATION IN A SIMULATED AIRCRAFT FUEL TANK (INCLUDING SUB-ATMOSPHERIC PRESSURES AND LOW TEMPERATURES) C. E. Polymeropoulos, and Robert Ochs Department.
MINISTERO DELL’INTERNO DIPARTIMENTO DEI VIGILI DEL FUOCO, DEL SOCCORSO PUBBLICO E DELLA DIFESA CIVILE DIREZIONE CENTRALE PER LA FORMAZIONE An Application.
IASFPWG – Seattle, WA Fuel Tank Ignition Experiments at Reduced Oxygen Concentrations International Aircraft Systems Fire Protection Working Group.
Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal.
Flammable extent of hydrogen jets close to surfaces Benjamin Angers*, Ahmed Hourri*, Luis Fernando Gomez, Pierre Bénard and Andrei Tchouvelev** * Hydrogen.
4th International Conference on Hydrogen Safety, San Francisco, USA, September, A. Kotchourko Karlsruhe Institute of Technology, Germany.
Review of Helium Venting Analyses
TS/CV/DC CFD Team CFD Simulation of a Fire in CERN Globe of Science and Innovation Sara C. Eicher CERN, CH.
ICHS 2007, San Sebastian, Spain 1 SAFETY OF LABORATORIES FOR NEW HYDROGEN TECHNIQUES Heitsch, M., Baraldi, D., Moretto, P., Wilkening, H. Institute for.
Total Flooding Systems
Experimental Investigation of Hydrogen Release and Ignition from Fuel Cell Powered Forklifts in Enclosed Spaces Isaac W. Ekoto, William G. Houf, and Greg.
Enclosure Fire Dynamics
Defining Hazardous Zones – Electrical Classification Distances Gary Howard,Andrei Tchouvelev, Vlad Agranat and Zhong Cheng Defining Hazardous Zones – Electrical.
CFD Modeling for Helium Releases in a Private Garage without Forced Ventilation Papanikolaou E. A. Venetsanos A. G. NCSR "DEMOKRITOS" Institute of Nuclear.
Large-Scale Hydrogen Deflagration and Detonations
Enclosure Fire Dynamics
Enclosure Fire Dynamics
Strategically Targeted Research in Intelligent Built.
Evaluation of Safety Distances Related to Unconfined Hydrogen Explosions Sergey Dorofeev FM Global 1 st ICHS, Pisa, Italy, September 8-10, 2005.
CNG STATION & GARAGE MODIFICATION CODES & STANDARDS Graham Barker Business Development Manager.
Modeling In-flight Inert Gas Distribution in a 747 Center-Wing Fuel Tank William Cavage AAR-440 Fire Safety Branch Wm. J. Hughes Technical Center Federal.
Analysis of Buoyancy-Driven Ventilation of Hydrogen from Buildings C. Dennis Barley, Keith Gawlik, Jim Ohi, Russell Hewett National Renewable Laboratory.
Pro-Science 4 th International Conference of Hydrogen Safety, September 12-14, 2011, SAN FRANCISCO, USA EXPERIMENTAL STUDY OF IGNITED UNSTEADY HYDROGEN.
Atrium Fire Protection
ICHS4, San Francisco, September E. Papanikolaou, D. Baraldi Joint Research Centre - Institute for Energy and Transport
Jet Fuel Vaporization and Condensation: Modeling and Validation C.E. Polymeropoulos Robert Ochs Rutgers, The State University of New Jersey International.
Page 1 SIMULATIONS OF HYDROGEN RELEASES FROM STORAGE TANKS: DISPERSION AND CONSEQUENCES OF IGNITION By Benjamin Angers 1, Ahmed Hourri 1 and Pierre Bénard.
Mitglied der Helmholtz-Gemeinschaft Simulation of the efficiency of hydrogen recombiners as safety devices Ernst-Arndt Reinecke, Stephan Kelm, Wilfried.
Funded by FCH JU (Grant agreement No ) 1 © HyFacts Project 2012/13 CONFIDENTIAL – NOT FOR PUBLIC USE 1.
Outline Background Explosion Phenomena Experiments Correlation Conclusion/Summary Questions.
Wu. Y., International Conference on Hydrogen Safety, September Initial Assessment of the Impact of Jet Flame Hazard From Hydrogen Cars In.
IASFPWG – Seattle, WA Jet-A Vaporization Computer Model A Fortran Code Written by Prof. Polymeropolous of Rutgers University International Aircraft.
FDS5 Simulation Results for VESDA Performance in HKCEC 2MW Fire Test (For internal info only) AEG, Xtralis Jan
2 DGS-SEE SEMINAR ON FIRE PROTECTION FOR PHYSICS RESEARCH FACILITIES OCTOBER 2015 CERN FIRE SIMULATIONS IN THE PS ACCELERATOR TUNNEL TO DEFINE A.
Detection of Hydrogen Released in a Full-scale Residential Garage Thomas Cleary & Erik Johnsson Fire Research Division Engineering Laboratory National.
One Minute Paper Statics; reply. Fluid dynamics  Fluids in motion Pumps Fans Compressors Turbines Heat exchangers.
Modeling of hydrogen explosion on a pressure swing adsorption facility *B. Angers 1, A. Hourri 1, P. Benard 1 E. Demaël 2, S. Ruban 2, S. Jallais 2 1 Institut.
4th International Conference on Hydrogen Safety, San Francisco, USA, September, J. Yanez, A. Kotchourko, M. Kuznetsov, A. Lelyakin, T. Jordan.
Jet Fuel Vaporization and Condensation: Modeling and Validation Robert Ochs and C.E. Polymeropoulos Rutgers, The State University of New Jersey International.
Week 1 – Engineering Agenda
Sandra Nilsen et. al Determination of Hazardous Zones Case study: Generic Hydrogen Refuelling Station.
© GexCon AS JIP Meeting, May 2011, Bergen, Norway 1 Ichard M. 1, Hansen O.R. 1, Middha P. 1 and Willoughby D. 2 1 GexCon AS 2 HSL.
ERT 322 SAFETY & LOSS PREVENTION. (A) Spring operated reliefs in liquid and gas service. (B)Rupture disc reliefs in liquid and gas service. (C)Vents for.
MULTI-COMPONENT FUEL VAPORIZATION IN A SIMULATED AIRCRAFT FUEL TANK C. E. Polymeropoulos Department of Mechanical and Aerospace Engineering, Rutgers University.
Bernoulli Equation – Pitot tube  Horizontal  Velocity at stagnation point is 0  Incompressible fluid  Steady state  Velocity as function of pressure.
Duy Phan, EN-STI-RBS. Description of the hazards  An Oxygen Deficiency Hazard (ODH) exists when the concentration of O2 ≤ 19.5 % (by volume)  Cold burns.
Working group meeting 07/05/15. Agenda Overview of review and current action list Relief system – Summary of problem – Details of analysis, testing and.
First Law of Thermodynamics applied to Flow processes
S.G. Giannissi1,2, I.C.Tolias1,2, A.G. Venetsanos1
60 1. What is the mass M in the system as given in the
SIMULATION ANALYSIS ON THE RISK OF HYDROGEN
Liming Yuan, Alex C. Smith  Process Safety and Environmental Protection 
Tsinghua University, Beijing, China
Venting deflagrations of local hydrogen-air mixture
V. Shentsov, M. Kuznetsov, V. Molkov
Fire Study in Multiple Compartments
Audrey DUCLOS1, C. Proust2,3, J. Daubech2, and F. Verbecke1
E.Vyazmina / S.Jallais October 2015 ICHS 2015
HOMOGENEOUS HYDROGEN DEFLAGRATIONS IN SMALL SCALE ENCLOSURE
CAD and Finite Element Analysis
Anubhav Sinha, Vendra Chandra and Jennifer X. Wen
Sandia National Laboratories
Non-monotonic overpressure vs
E. Papanikolaou, D. Baraldi
Natural and Forced Ventilation of Buoyant Gas Released in a Full-Scale Garage : Comparison of Model Predictions and Experimental Data Kuldeep Prasad, William.
ICHS5 – 2013 September, Brussels, Belgium | ID161
CFD computations of liquid hydrogen releases
Context R&D activities in H2 technologies in France is driven by industrial research targeting real applications (DIMITHRY, H2E, HYPE, ...) Safety management.
Presentation transcript:

Modeling and Analysis of a Hydrogen Release in a Large Scale Facility C. Regis Bauwens and Sergey B. Dorofeev FM Global, Research Division 5th International Conference on Hydrogen Safety September 10th, 2013

Overview Background Scale Model Simulations Full Scale Simulations Extending Results Additional Considerations Questions

Background Increasing use of hydrogen powered forklifts within warehouses Indoor refueling of forklifts presents possible release scenarios Consequence of accidental release needs to be assessed

Background Modeling Approach FireFoam code used for CFD simulations tracked transport of H2 in warehouse estimated overpressure from mass above LFL Two sets of simulations scale model compared with experiments full scale warehouse

Scale Model Simulation Experiments (Ekoto et al. 2012) 2.7 x 4.6 x 3.6 m3 enclosure simulated release from a forklift varying release rate simulated H2 tank release measured H2 concentration, overpressure

Scale Model Simulation CFD Simulations non-uniform mesh, refined mesh where H2 is present tested multiple mesh resolutions, from 2.5 -10 cm 50,000 – 900,000 grid points

Scale Model Simulation

Scale Model Tests Concentration Results Total mass above LFL consistent across resolutions near dispenser at ceiling

Scale Model Tests Overpressure estimate quasi-static pressure rise pressure rises uniformly on all surfaces in warehouse assumptions : all H2 above LFL consumed well sealed enclosure

Scale Model Tests Maximum Overpressure Measured (Ekoto et al., 2012): 0.19 bar ceiling ignition 0.25 bar forklift ignition Model results: 0.24 bar

Scale Model Tests Summary simulation results closely match experimental concentration measurements grid independence found for mesh resolutions up to 10 cm quasi-static pressure rise method produces reasonable estimate for overpressure

Full Warehouse Simulation 62 x 62 x 8 m warehouse (approx. 200x200x25 ft) steady 3 minute release 5 release rates used 0.25, 0.5, 1.0, 2.0 and 4 kg/min

Full Warehouse Simulation Computational Mesh non-uniform mesh 10 cm grid resolution 0.24 m2 release outlet, low exit velocity, corner of warehouse

Full Warehouse Simulation Results H2 formed thin circular clouds below ceiling cloud thickness varied with release rate

Full Warehouse Simulation Results with lower release rates, proportionally less H2 remained above LFL

Full Warehouse Simulation Summary of CFD Results closed, unventilated warehouse > 0.02 bar light damage to roof/wall panels and broken windows expected > 0.10 bar major structural damage expected Release rate (kg/min) Mass above LFL (kg) Pmax (bar) 0.25 0.03 - 0.5 0.34 0.01 1 1.6 0.02 2 4.1 0.06 4 8.0 0.12

Extending Results Effect of Ventilation Systems fully closed warehouse assumption overly conservative ventilation systems can reduce pressure two ways provides venting/pressure relief removes hydrogen from warehouse hydrogen removal neglected highly dependent of vent placement

Extending Results Ventilation System Pressure Relief Estimate estimate H2 consumption time from cloud shape, size compares ventilation with volume production rate Extended warehouse sizes assume cloud shape, mass above LFL unchanged simply increase volume used in calculation

Extended Results Peak overpressure summary (Ventilated results assume 3 air changes/hour) Volume (m3) 1 kg/min 2 kg/min 4 kg/min Closed (bar) Ventilated (bar) 16,000 0.05 0.03 0.12 0.09 0.24 0.21 25,000 0.01 0.08 0.04 0.15 0.11 31,000 0.02 0.06 50,000 - 0.07 62,000 100,000

Additional Considerations Sprinkler Activation hydrogen cloud accumulates at ceiling sprinklers typically mounted within 18” of ceiling high temperature combustion products sprinkler activation can cause significant damage water damage to commodities impair fire protection of warehouse sprinkler activation experimentally confirmed

Additional Considerations Sprinkler Activation using CFD results for cloud size, area of sprinkler activation can be estimated Release Rate (kg/min) Cloud Radius (m) Percentage of Warehouse* Area (%) 0.25 8 1.3 0.5 19 7.4 1 34 23 2 46 43 4 54 60

Summary Model approach produces results consistent with scale model experiments Maximum overpressure highly dependent on release rate, size of warehouse Damage associated with sprinkler activation must also be considered

Questions?