IA HYSAFE & JRC IET WORKSHOP Research Priorities and Knowledge Gaps in Hydrogen Safety. Hydrogen Ignition and Light up Probabilities.

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IA HYSAFE & JRC IET WORKSHOP Research Priorities and Knowledge Gaps in Hydrogen Safety Hydrogen Ignition and Light up Probabilities www.hsl.gov.uk An An Agency Agency of the of Health the Health and Safety and Executive Safety Executive

Contents Ignition sources Where is our knowledge of potential ignition sources lacking for hydrogen? Discussion of work carried out at HSL Light up probabilities for hydrogen releases Where is our knowledge in relation to hydrogen Probability of ignition in a particular flammable atmosphere Probability of a flammable atmosphere existing

EN1127-1:2011 gives the following potential ignition sources :

Two questions : -Which ignition sources do we have sufficient understanding of? -Which are of practical, general concern? MechEx Project Corona discharge Spontaneous Ignition Review by Hawksworth and Astbury, 2007

MechEx Project: Investigated friction and impact ignition of various gases and dusts Some work carried out on hydrogen

MechEx Project: Friction ignition of Methane

MechEx Project: Friction ignition of Hydrogen

Mechanical sparks and frictional heating Data available for further use and analysis E.g. 0.7kW at 0.7 m/s for stainless steel on stainless steel contact gave a maximum surface temperature of 530ºC and caused ignition of hydrogen Note that temperature < AIT (artifact of measurement?) Proposed ignition criteria based on: Speed (m/s) Maximum potential power density (W/mm 2 ) Surface temperature (estimated from speed / pressure)

Mechanical sparks and frictional heating But, there are many variables (e.g. friction materials) Conservative? Do we know enough to realistically assess ignition potential for hydrogen? Modelling Simple engineering tools

Spontaneous Ignition : Cases reported of spontaneous or self ignition of hydrogen where no obvious ignition source could be found (eg spark) A number of mechanisms have been suggested (e.g. Hawksworth & Astbury, 2007) which may account for this phenomenon Experimental studies were conducted at HSL to investigate possible mechanisms which could result in self ignition of hydrogen Sudden adiabatic compression in shock wave formation after release of pressurised hydrogen ( diffusion ignition ) following on from the work of Dryer etc, using practical piping configurations Ignition of a premixed volume of hydrogen/air by corona discharge

Diffusion Ignition: Simplified schematic of release system at HSL Storage vessel 49 litre vessel no 1 PT Storage vessel 49 litre vessel no 2 PT Release point Downstream geometry Bursting disc holder PT Pipework internal diameter 11.9 Blast wall

Diffusion Ignition: Example of downstream geometry used A = ½ NPT with transducer adapter B = ½ NPT to 3/8 reducer C = 3/8 NPT to1/4 swagelok reducer

Diffusion Ignition at HSL: Fitting ID A B C D E F G H I J K Fitting Type ½ NPT pipe nipple 2 long with piezo transducer ½ to 3/8 NPT female brass reducing union 3/8 NPT male to ¼ male Swagelok tube reducer 3/8 BSP plug (flat face) with 5.7mm bore 3/8 BSP plug (flat face) with 6.7mm bore 3/8 BSP plug (flat face) with 7.7mm bore 3/8 BSP plug (flat face) with 8.7mm bore 3/8 BSP plug (flat face) with 9.7mm bore 3/8 BSP plug (flat face) with 10.7mm bore 3/8 BSP plug (flat face) with 2.7mm bore 3/8 BSP plug (flat face) with 9.2mm bore

Diffusion Ignition Results at HSL: Lowest burst pressure at which ignition occurred was 35.5 bar Highest burst pressure at which ignition did not occur was 573 bar Ignitions sometimes occurred even with minimum downstream restriction if burst pressure high (>240bar g)

Diffusion Ignition Results at HSL: Cavity pressure (bar) 100 90 80 70 60 50 40 30 20 10 0 Cavity pressure against burst pressure 0 50 100 150 200 250 300 350 400 450 500 550 600 650 Burst pressure (bar) Ignitions Non-Ignitions Modelling of diffusion ignition carried out (e.g. Wen, 2011) Do we know enough? CFD Simple engineering tools / guides

Corona discharge ignition Anecdotal evidence for corona ignition No previous quantitative data found Corona discharge ignition experiments carried out in premixed hydrogen / air mixtures at HSL Corona is not a single spark but a continuous current from a pointed electrode at a high potential Electrode

Schematic of corona ignition system Oxygen analyser Vent H 2 -Air injection HT Source (up to 30kV) Burst panel (conducting plastic sheet) Fine wire corona point HT cable + Insulated connection to corona wire) I Flow controller / mixer Keithley electrometer Electrometer output Hydrogen Air Data logger = Insulator (PTFE)

Corona ignition results

Corona ignition results H 2 -air mixtures (26 32% v/v) were ignited by corona discharge generated by raising a fine wire (0.38mm) to a high potential Ignitions occurred with positive corona discharges at a current of +150 A and a potential of +20kV for a wire point and plate electrode system with a 30mm separation No ignition was observed with negative currents of up to 290 A and potential of 28kV Could explain ignition in certain situations (e.g. high vent stacks in strong Earth s electric field) BUT : Limited data for one geometry only!

Light Up Probabilities Does an ignition source within a jet release of gas always result in an ignition and sustained combustion of the jet? Depends upon extent / duration of flammable atmosphere and ignition probability of ignition source Correlations exist for estimating average concentrations Concept of Flammability Factor (FF) being considered (e.g. Gant et al. 2011) Probability of ignition available for some ignition sources

Light Up Probabilities Mean, RMS and instantaneous concentrations of hydrogen (image ex. J.Keller) Average concentration correlations (e.g. Chen & Rodi)

Light Up Probabilities Definition of FF: proportion of time that the gas concentration is within the flammable range x Gas Concentration UEL LEL Time Flammable? Time Flammable at this position for 40% of the time (Flammability Factor = 0.4) Probability density functions used to predict FF

Light Up Probabilities Ignition sources themselves will also have a probability of igniting a particular flammable hydrogen/air mixture Example : electrostatic brush discharges (Gibson 1988) Can we do anything to minimise probability??..

Light Up Probabilities Methods have been developed for assessing the probabilities of ignition for hydrocarbon releases (e.g. as used in UK HSE MISHAP) Immediate versus delayed ignition (<30 seconds) Based on incident data For example, prediction of immediate ignition probability using minimum ignition energy and autoignition temperature (from Moosemillar 2009)

Light Up Probabilities UK HSE MISHAP Immediate ignition : T 9.5 1 3 AIT 0.0024 P Pimm. ign 1 5000e 2 3 MIE Delayed ignition : assumes that delayed ignition occurs for instances that do not meet the requirements for immediate ignition, i.e., an appreciable vapour cloud is allowed to develop which is then ignited by a remote ignition source such as fired heaters or rotating equipment etc.

Light Up Probabilities Is hydrogen as well defined? Should hydrogen be easier? low MIE (more likely ignition?) high buoyancy (less spread of flammable mixtures at ground level?)

Summary There are a number of gaps in the understanding the sensitivity of hydrogen to ignition sources Which are the priority? Methods could be applied to assessing the ignition potential for real world hydrogen releases Further work required?