Fires and Explosions
Fires and Explosions
Definitions
Flammability
Flash Points
Flammability limits
Mixtures
Temperature Dependence
Pressure Dependence
Minimum Oxygen Concentration
Minimum Ignition Energy
Adiabatic Compression
Ignition Sources
Introduction
 We have been talking about source models for
the release of materials and about dispersion
models if the material is a toxicant.
Another concern is a release of flammable
materials where we need to worry about fires and
explosions.
Fire Triangle
Most are familiar with the Fire
Triangle.
In order for a fire to start or be
sustained you need to have a
Fuel, an oxidizer and an
ignition source.
If one of the three components
is eliminated, then there will
not be a fire (or explosion)
Fuel
Fuel must be present in certain concentrations.
Typical cases where fuel occur are if there is a leak,
during filling operations, transfer operations, or excessive
dusts.
Although we often cannot always eliminate these
sources we can help by having good ventilation to keep
vapors from building up.
Often we locate things out-doors, use grating on floors
so vapors don’t build up.
Oxidizers
Oxygen is the most common oxidizer, especially
that found in ambient air.
For oxygen, we often use “inerting” with nitrogen,
helium blankets over flammable materials to
reduce O2 content below that where you can
have combustion.
Ignition Sources
Heat is a common ignition source.
“Ignition sources are free!!!”
Although we can eliminate ignition sources, it is
almost inevitable that an ignition source will be
available if there is a large release of flammable
material that cannot be diluted quickly.
Fire Tetrahedron
The fire tetrahedron or fire
pyramid adds a fourth
component—chemical chain
reaction—as a necessity in
the prevention and control of
fires.
The free radicals formed
during combustion are
important intermediates in the
initiation and propagation of
the combustion reaction. Fire
suppression materials
scavenge these free radicals
Definitions
Combustion – a chemical reaction in which a
substance combines with an oxidizer and
releases energy.
Explosion – rapid expansion of gases resulting in
a rapid moving pressure or shock wave.
Mechanical Explosion – due to failure of vessel
with high pressure non reactive gas.
Explosions
Detonation – explosion (chemical reaction) with shock
wave greater than speed of sound
Deflagration – explosion (chemical reaction) with shock
wave less than speed of sound
BLEVE – Boiling Liquid Expanding Vapor Explosion –
when liquid is at a temperature above its atmospheric
boiling point. Vessel ruptures – flammable liquid flashes
and results in a fire/explosion
Explosions
Confined explosion – an explosion occurring
within a vessel or a building. Usually results in
injury to the building inhabitants and extensive
damage.
Unconfined explosion – an explosion occurring in
the open. Usually results from spill of a
flammable gas spill. These explosions are rarer
than confined since dilution occurs.
Explosions
 Dust Explosions - This explosion results from
the rapid combustion of fine solid particles. Many
solid materials become very flammable when
reduced to a fine powder.
Fires and Explosions
Definitions
Flammability
Flash Point
Flammability limits
Mixtures
Temperature Dependence
Pressure Dependence
Minimum Oxygen Concentration
Minimum Ignition Energy
Adiabatic Compression
Ignition Sources
Flammability
Flash Point (FP) – a property of material used to
determine the fire and explosive hazard. The
lowest temperature of a liquid at which it gives off
enough vapor to form an ignitable mixture with
air.
Needs to be determined experimentally.
Different methods to determine, open cup and closed
cup. Open cup is usually a few degrees higher.
National Fire Protection Association
Flammability classification
Flammable IA – Flash point < 73°F, boiling point < 100 °F
Flammable IB – Flash point < 73°F, boiling point > 100 °F
Flammable IC – 73°F < Flash point < 100 °F
Combustible II – 100 °F < Flash point < 140 °F
Combustible IIIA – 140 °F < Flash point < 200 °F
Combustible IIIB – Flash point > 200 °F
Mixture Flash Points
Flash Points of mixtures can be estimated only IF
one of the components is flammable. If more than
one is flammable then need to determine
experimentally.
For mixtures:
Determine the temperature at which the vapor pressure of
the flammable in the liquid is equal to the pure component
vapor pressure at its flash point.
Mixture Flash Points
Example
Methanol FP=54°F, Vapor Pressure @ 54°F is 62 mmHg
Determine the flash point of a solution that is 75wt% MeOH in water.
Solution:
Since only one component is flammable, can estimate mixture FP:
Mixture Flash Point Example Continued
 
Raoult's Law
62
98.4
0.63
Now need the temperature that corresponds
to this . Use Antoine's equation (Append II)
ln
in Kelvin, in mmHg
sat
sat
sat
sat
sat
P xP
P mmHg
P mmHg
x
P
B
P A
C T
T P

  
 

Mixture Flash Point Example Continued
 
Rearrange
-ln
From Appendix II
A is 18.5875
B is 3626.55
C is -34.29
3626.55
34.29 293.36
18.5875 ln 98.4
20.21 68.4
sat
B
T C
A P
T K
T C F
 
  

   
Flammability Limits
There is usually a range
of compositions of a
flammable vapor and air
where combustion occurs.
Too little fuel (lean
mixture) not enough fuel
to burn.
Too much fuel (rich
mixture) not enough
oxygen to burn
Flammability Limits
Table 6-1 gives upper flammability limits and
lower flammability limits for several common
substances.
Experimentally determined.
LFL can be estimated from Flash Point:.
vapor pressure at flash point
760 mmHg
Determine vapor pressure using Antoine Equation
LFL 
Mixture Flammability Limits
If you have a mixture of flammable components
you can calculate Lower Flammability Limit of the
mixture LFLmix using Le Chatelier’s relationship:
1
1
is flammability limit for component
is mole fraction of on combustible basis
is the number of combustible species
mix n
i
i i
i
i
LFL
y
LFL
LFL i
y i
n



Mixture Flammability Limits
You can also calculate an Upper Flammability
Limit of the mixture UFLmix using Le Chatelier’s
relationship:
1
1
mix n
i
i i
UFL
y
UFL



Flammability Limits – Temperature effect
Table 6-1 gives flammability limits for 25°C and
atmospheric pressure. If you are at a different
temperature you can modify flammability limits
 
 
25
25
1 0.75( 25)/
1 0.75( 25)/
is heat of combustion for component
T is in C
T c
T c
c
LFL LFL T H
UFL UFL T H
H
   
   


Flammability Limits – Pressure effects
 LFL is not affected by pressure
 UFL does depend on the pressure
Procedure
Correct for Temperature
Correct for Pressure
Calculate for mixture
10
20.6(log 1)
is in MPa absolute
P
UFL UFL P
P
  
Fires and Explosions
Definitions
Flammability
Flash Points
Flammability limits
Mixtures
Temperature Dependence
Pressure Dependence
Minimum Oxygen Concentration
Minimum Ignition Energy
Adiabatic Compression
Ignition Sources
Minimum Oxygen Concentration
(MOC)
 LFL is based on “air” but actually it is O2 that is
important. Often in industry they “inert” to dilute
the O2 concentration.
 Below the MOC the reaction cannot generate
enough energy to heat the entire mixture to the
extent required for self propagation.
MOC
2
2
2 2 2
2
Moles Fuel Moles O
Moles Fuel & Moles Air Moles Fuel
Moles O
Moles Fuel
Need to balance stoichiometry
2
4 2
Moles O
Moles Fuel
m x y
MOC
MOC LFL
x
C H O zO mCO H O
x y
z m
z
   
   
   
 
  
 
  
  
 
 
 
Fires and Explosions
Definitions
Flammability
Flash Points
Flammability limits
Mixtures
Temperature Dependence
Pressure Dependence
Minimum Oxygen Concentration
Minimum Ignition Energy
Adiabatic Compression
Ignition Sources
Minimum Ignition Energy (MIE)
Minimum energy input needed to initiate combustion
Most hydrocarbons have low MIE~0.25 mJ
Whereas the “spark” from walking across the room is
22mJ (almost 100X too much)
Again, we always assume that an ignition source will
exist
Table 6-2 gives MIEs for some substances
Fires and Explosions
Definitions
Flammability
Flash Points
Flammability limits
Mixtures
Temperature Dependence
Pressure Dependence
Minimum Oxygen Concentration
Minimum Ignition Energy
Adiabatic Compression
Ignition Sources
Adiabatic Compression
 When gases are compressed they heat up and
can ignite (this is how a diesel engine works, also
the cause of “knocking” in gasoline engines)
The adiabatic temperature rise is:
1
and absolute
f
f i
i
P
T T
P
T P



 
  
 
Fires and Explosions
Definitions
Flammability
Flash Points
Flammability limits
Mixtures
Temperature Dependence
Pressure Dependence
Minimum Oxygen Concentration
Minimum Ignition Energy
Adiabatic Compression
Ignition Sources
Ignition Sources
Ignition sources are free!!!
Table 6-3 gives the
results of a study by
Factory Mutual
Engineering Corporation
who studied over 25,000
industrial fires to
determine the source of
ignition.
In Class Problem
What is the UFL of a gas mixture composed of 1%
methane, 2% ethane and 3% propane by volume
at 50°C and 2 atmospheres:
Data:
Component MW Heat of Combustion
(kcal/mol)
Methane 16.04 212.79
Ethane 30.07 372.81
Propane 44.09 526.74
Solution
Procedure:
Correct for temperature
Correct for pressure (only for UFL)
Find for mixture.
Solution
 Correction for Temperature : UFL from Table 6-
1  
 
 
 
25
50
50
50
Eq. 6-4 1 0.75( 25)/
Methane 15 1 0.75(25) / 212.79 16.32
Ethane 12.5 1 0.75(25)/372.81 13.13
Propane 9.5 1 0.75(25)/526.74 9.84
T c
UFL UFL T H
UFL
UFL
UFL
    
  
  
  
Solution cont.
Correction for Pressure (UFL only)
 
10
2 1 10
2 1
Propane
Eq. 6-5 20.6(log 1)
101
2 0.202
1000
20.6(log (0.202 ) 1)
6.290
22.61
19.40
16.13
P
atm atm
atm atm
Methane
Ethane
UFL UFL P
kPa MPa
P atm MPa
atm kPa
UFL UFL MPa
UFL UFL
UFL
UFL
UFL
   
   
 
   
   
  
 



Solution cont.
Mixture calculation
Equation 6-2 for mixtures
Mixture Vol% Mol frac Comb
Methane 1 0.1667
Ethane 2 0.3333
Propane 3 0.5000
Combustibles 6
1
1
mix n
i
i i
UFL
y
UFL



Solution Continued
Since total combustibles in air 1+2+3=6 < 18 then
the system is in the combustible range (below
UFL)
1
18.0 %
0.1667 0.3333 0.5
22.61 19.40 16.13
Mixture
UFL vol
 
 

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FlammabilityFlammabilityFlammabilityFlammability.ppt

  • 2. Fires and Explosions Definitions Flammability Flash Points Flammability limits Mixtures Temperature Dependence Pressure Dependence Minimum Oxygen Concentration Minimum Ignition Energy Adiabatic Compression Ignition Sources
  • 3. Introduction  We have been talking about source models for the release of materials and about dispersion models if the material is a toxicant. Another concern is a release of flammable materials where we need to worry about fires and explosions.
  • 4. Fire Triangle Most are familiar with the Fire Triangle. In order for a fire to start or be sustained you need to have a Fuel, an oxidizer and an ignition source. If one of the three components is eliminated, then there will not be a fire (or explosion)
  • 5. Fuel Fuel must be present in certain concentrations. Typical cases where fuel occur are if there is a leak, during filling operations, transfer operations, or excessive dusts. Although we often cannot always eliminate these sources we can help by having good ventilation to keep vapors from building up. Often we locate things out-doors, use grating on floors so vapors don’t build up.
  • 6. Oxidizers Oxygen is the most common oxidizer, especially that found in ambient air. For oxygen, we often use “inerting” with nitrogen, helium blankets over flammable materials to reduce O2 content below that where you can have combustion.
  • 7. Ignition Sources Heat is a common ignition source. “Ignition sources are free!!!” Although we can eliminate ignition sources, it is almost inevitable that an ignition source will be available if there is a large release of flammable material that cannot be diluted quickly.
  • 8. Fire Tetrahedron The fire tetrahedron or fire pyramid adds a fourth component—chemical chain reaction—as a necessity in the prevention and control of fires. The free radicals formed during combustion are important intermediates in the initiation and propagation of the combustion reaction. Fire suppression materials scavenge these free radicals
  • 9. Definitions Combustion – a chemical reaction in which a substance combines with an oxidizer and releases energy. Explosion – rapid expansion of gases resulting in a rapid moving pressure or shock wave. Mechanical Explosion – due to failure of vessel with high pressure non reactive gas.
  • 10. Explosions Detonation – explosion (chemical reaction) with shock wave greater than speed of sound Deflagration – explosion (chemical reaction) with shock wave less than speed of sound BLEVE – Boiling Liquid Expanding Vapor Explosion – when liquid is at a temperature above its atmospheric boiling point. Vessel ruptures – flammable liquid flashes and results in a fire/explosion
  • 11. Explosions Confined explosion – an explosion occurring within a vessel or a building. Usually results in injury to the building inhabitants and extensive damage. Unconfined explosion – an explosion occurring in the open. Usually results from spill of a flammable gas spill. These explosions are rarer than confined since dilution occurs.
  • 12. Explosions  Dust Explosions - This explosion results from the rapid combustion of fine solid particles. Many solid materials become very flammable when reduced to a fine powder.
  • 13. Fires and Explosions Definitions Flammability Flash Point Flammability limits Mixtures Temperature Dependence Pressure Dependence Minimum Oxygen Concentration Minimum Ignition Energy Adiabatic Compression Ignition Sources
  • 14. Flammability Flash Point (FP) – a property of material used to determine the fire and explosive hazard. The lowest temperature of a liquid at which it gives off enough vapor to form an ignitable mixture with air. Needs to be determined experimentally. Different methods to determine, open cup and closed cup. Open cup is usually a few degrees higher.
  • 15. National Fire Protection Association Flammability classification Flammable IA – Flash point < 73°F, boiling point < 100 °F Flammable IB – Flash point < 73°F, boiling point > 100 °F Flammable IC – 73°F < Flash point < 100 °F Combustible II – 100 °F < Flash point < 140 °F Combustible IIIA – 140 °F < Flash point < 200 °F Combustible IIIB – Flash point > 200 °F
  • 16. Mixture Flash Points Flash Points of mixtures can be estimated only IF one of the components is flammable. If more than one is flammable then need to determine experimentally. For mixtures: Determine the temperature at which the vapor pressure of the flammable in the liquid is equal to the pure component vapor pressure at its flash point.
  • 17. Mixture Flash Points Example Methanol FP=54°F, Vapor Pressure @ 54°F is 62 mmHg Determine the flash point of a solution that is 75wt% MeOH in water. Solution: Since only one component is flammable, can estimate mixture FP:
  • 18. Mixture Flash Point Example Continued   Raoult's Law 62 98.4 0.63 Now need the temperature that corresponds to this . Use Antoine's equation (Append II) ln in Kelvin, in mmHg sat sat sat sat sat P xP P mmHg P mmHg x P B P A C T T P       
  • 19. Mixture Flash Point Example Continued   Rearrange -ln From Appendix II A is 18.5875 B is 3626.55 C is -34.29 3626.55 34.29 293.36 18.5875 ln 98.4 20.21 68.4 sat B T C A P T K T C F          
  • 20. Flammability Limits There is usually a range of compositions of a flammable vapor and air where combustion occurs. Too little fuel (lean mixture) not enough fuel to burn. Too much fuel (rich mixture) not enough oxygen to burn
  • 21. Flammability Limits Table 6-1 gives upper flammability limits and lower flammability limits for several common substances. Experimentally determined. LFL can be estimated from Flash Point:. vapor pressure at flash point 760 mmHg Determine vapor pressure using Antoine Equation LFL 
  • 22. Mixture Flammability Limits If you have a mixture of flammable components you can calculate Lower Flammability Limit of the mixture LFLmix using Le Chatelier’s relationship: 1 1 is flammability limit for component is mole fraction of on combustible basis is the number of combustible species mix n i i i i i LFL y LFL LFL i y i n   
  • 23. Mixture Flammability Limits You can also calculate an Upper Flammability Limit of the mixture UFLmix using Le Chatelier’s relationship: 1 1 mix n i i i UFL y UFL   
  • 24. Flammability Limits – Temperature effect Table 6-1 gives flammability limits for 25°C and atmospheric pressure. If you are at a different temperature you can modify flammability limits     25 25 1 0.75( 25)/ 1 0.75( 25)/ is heat of combustion for component T is in C T c T c c LFL LFL T H UFL UFL T H H          
  • 25. Flammability Limits – Pressure effects  LFL is not affected by pressure  UFL does depend on the pressure Procedure Correct for Temperature Correct for Pressure Calculate for mixture 10 20.6(log 1) is in MPa absolute P UFL UFL P P   
  • 26. Fires and Explosions Definitions Flammability Flash Points Flammability limits Mixtures Temperature Dependence Pressure Dependence Minimum Oxygen Concentration Minimum Ignition Energy Adiabatic Compression Ignition Sources
  • 27. Minimum Oxygen Concentration (MOC)  LFL is based on “air” but actually it is O2 that is important. Often in industry they “inert” to dilute the O2 concentration.  Below the MOC the reaction cannot generate enough energy to heat the entire mixture to the extent required for self propagation.
  • 28. MOC 2 2 2 2 2 2 Moles Fuel Moles O Moles Fuel & Moles Air Moles Fuel Moles O Moles Fuel Need to balance stoichiometry 2 4 2 Moles O Moles Fuel m x y MOC MOC LFL x C H O zO mCO H O x y z m z                               
  • 29. Fires and Explosions Definitions Flammability Flash Points Flammability limits Mixtures Temperature Dependence Pressure Dependence Minimum Oxygen Concentration Minimum Ignition Energy Adiabatic Compression Ignition Sources
  • 30. Minimum Ignition Energy (MIE) Minimum energy input needed to initiate combustion Most hydrocarbons have low MIE~0.25 mJ Whereas the “spark” from walking across the room is 22mJ (almost 100X too much) Again, we always assume that an ignition source will exist Table 6-2 gives MIEs for some substances
  • 31. Fires and Explosions Definitions Flammability Flash Points Flammability limits Mixtures Temperature Dependence Pressure Dependence Minimum Oxygen Concentration Minimum Ignition Energy Adiabatic Compression Ignition Sources
  • 32. Adiabatic Compression  When gases are compressed they heat up and can ignite (this is how a diesel engine works, also the cause of “knocking” in gasoline engines) The adiabatic temperature rise is: 1 and absolute f f i i P T T P T P          
  • 33. Fires and Explosions Definitions Flammability Flash Points Flammability limits Mixtures Temperature Dependence Pressure Dependence Minimum Oxygen Concentration Minimum Ignition Energy Adiabatic Compression Ignition Sources
  • 34. Ignition Sources Ignition sources are free!!! Table 6-3 gives the results of a study by Factory Mutual Engineering Corporation who studied over 25,000 industrial fires to determine the source of ignition.
  • 35. In Class Problem What is the UFL of a gas mixture composed of 1% methane, 2% ethane and 3% propane by volume at 50°C and 2 atmospheres: Data: Component MW Heat of Combustion (kcal/mol) Methane 16.04 212.79 Ethane 30.07 372.81 Propane 44.09 526.74
  • 36. Solution Procedure: Correct for temperature Correct for pressure (only for UFL) Find for mixture.
  • 37. Solution  Correction for Temperature : UFL from Table 6- 1         25 50 50 50 Eq. 6-4 1 0.75( 25)/ Methane 15 1 0.75(25) / 212.79 16.32 Ethane 12.5 1 0.75(25)/372.81 13.13 Propane 9.5 1 0.75(25)/526.74 9.84 T c UFL UFL T H UFL UFL UFL              
  • 38. Solution cont. Correction for Pressure (UFL only)   10 2 1 10 2 1 Propane Eq. 6-5 20.6(log 1) 101 2 0.202 1000 20.6(log (0.202 ) 1) 6.290 22.61 19.40 16.13 P atm atm atm atm Methane Ethane UFL UFL P kPa MPa P atm MPa atm kPa UFL UFL MPa UFL UFL UFL UFL UFL                          
  • 39. Solution cont. Mixture calculation Equation 6-2 for mixtures Mixture Vol% Mol frac Comb Methane 1 0.1667 Ethane 2 0.3333 Propane 3 0.5000 Combustibles 6 1 1 mix n i i i UFL y UFL   
  • 40. Solution Continued Since total combustibles in air 1+2+3=6 < 18 then the system is in the combustible range (below UFL) 1 18.0 % 0.1667 0.3333 0.5 22.61 19.40 16.13 Mixture UFL vol    