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TECHNICAL FOUNDATIONS TO ESTABLISH NEW
CRITERIA FOR EFFICIENT OPERATION OF INDUSTRIAL
          STEAM-ASSISTED GAS FLARES




 L. Douglas Smoot, Ph.D., Combustion Resources, Inc.
   Joseph D. Smith, Ph.D., Idaho National Laboratory
      Robert E. Jackson, Combustion Resources

               IFRF 16th International Members’ Conference
Combustion and Sustainability: New Technologies, New Fuels, New Challenges

              8-10 June, 2009 – Boston Massachusetts, USA
Slide 2



Discussion Outline
•   Basic Flare Operation and Control
    – Operating/design issues for Pipe Flares and Ground Flares
•   Historical Performance Analysis
    – EPA and CMA Data
    – API Guidelines
•   Proposed Metrics for Flare Operation
    – Adiabatic Temperature vs. LHV
    – Combustion Efficiency vs. Steam Ratio
•   BAT for Flare Performance Analysis
•   Conclusions and Recommendations




                                                               IFRF 16th International Members’ Conference:
                               Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 3

 Flares in Recent News!

Decades of contamination of the water and soil from oil and gas operations mean most food
must now be imported, says JNN, and the practice of "gas flaring" has put a toxic
pall over many villages.




WILLEMSTAD (Reuters) - A refinery on Curacao operated by
Venezuela's state oil company is damaging people's health
and must cut emissions or face multi-million dollar fines, a
court on the Caribbean island ruled on Thursday.                         Industrial flares burn off pressurized
                                                                         gases but also can shoot out massive
In 2007, a Curacao court threatened to close Isla if it cannot           amounts of noxious emissions. The
meet emissions standards, citing a study estimating that 18              Houston area has about 400 flare
people die prematurely every year from contaminant                       stacks, and they are among the largest
exposure.                                                                and least- understood sources of pollution
                                                                         in the region, researchers said.
Van Unen also took into account excessive flaring that
sometimes runs for days and weeks. The amounts to be
paid were decided with the serious health consequences and
the earnings of PDVSA in mind, the judge stated.


                                                                                     IFRF 16th International Members’ Conference:
                                                     Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 4



   Operating/Design Issues for Pipe Flares



                                                                                   Wind shortens Flame and
                                                                                   causes soot formation on
                                                                                          back side of flame

                                                                               Flame bends over in wind
                                                                              and licks downwind side of
                                                                                             flare stack


                             Air egression into
                             stack tip can lead
                             to internal burning
                                and possible
                                  explosive
                                  conditions


 Cross winds cause air                                                    P. Gogolek, CANMET Energy
egression into flare stack                                                Technology Centre – Ottawa Natural
                                                                          Resources Canada

                                                                 IFRF 16th International Members’ Conference:
                                 Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 5
Operating/Design Issues for Low Profile Flares
  High tip velocity increases air
  entrainment
  o   Tip design controls air entrainment
      (fuel/air mixing)
  o   High jet velocities = High Jet Noise
  Pressure Assist improves
  mixing and combustion
  o   Smoke below certain tip pressure
      (D-stage pressure) = ambient air
      entrainment
  Tip spacing critical
  o   Tips must cross light
  o   Individual tip flames can merge and
      lengthen overall flare flame
  o   Adjacent rows compete for ambient
      air (longer flames near flare center)

                                                                    IFRF 16th International Members’ Conference:
                                    Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 6

What is a Flare or Why is there a
flame on top of that stack?
Flares are Safety Devices used to prevent catastrophic events in
systems with highly flammable gases
Flares provide safe discharge point for relief devices or in case of loss
of containment
API RP-521† describes proper flare design and operation but does not
define them as “combustors with routine emissions” (e.g., incinerators
or process heaters)
Plants required to have “Flare minimization plan” as part of air permit –
recovery devices operate with quasi-steady flows but can’t operate over
large flow ranges possible in hydrocarbon refineries or chemical plants
Pollution control devices (i.e., incinerators) combust process emissions
Safe and efficient flare design must handle very low hydrocarbon flows
(due to fuel cost) and high hydrocarbon flows (due to safety constraints)
under variable ambient conditions (i.e., wind and rain) for non-uniform
gas compositions
†API   RP-521, 4th ed., American Petroleum Institute, Washington D.C., March (1997).


                                                                           IFRF 16th International Members’ Conference:
                                           Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 7

 Flare Efficiency Studies (EER)
     Flare Screening Facility and Flare Test Facility used to analyze
     flame stability and combustion/destruction efficiency for
     different fuels and different flare tips (captured/analyzed flare
     plume)
     Used 3”, 6”, and 12” Open Pipe Flares plus Air-assisted,
     Pressure- assisted and Steam-assisted Flares
     Considered Pilot vs non-pilot operation
     Considered saturated/unsaturated hydrocarbon, H2S, and NH3
     Correlated Flame stability vs Gas heating value and Tip exit
     velocity
        o   Flame stability defined as Tip velocity > Flame velocity
        o   Assisted flares more stable, Piloted flares more stable,
            unsaturated fuels more stable (but require more air)
Pohl, J.H. & N.R. Soelberg, Evaluation of the Efficiency of Industrial Flares: Flare Head
Design and Gas Composition, EPA-600/2-85-106, September (1985)
Pohl, J.H. & N.R. Soelberg, Evaluation of the Efficiency of Industrial Flares: H2S Gas
Mixtures and Pilot Assisted Flares, EPA-600/2-86-080 September (1986)


                                                                           IFRF 16th International Members’ Conference:
                                           Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 8

Testing on Flame Stability and Heating Value
       Identified Min HV for Gas where Flame Speed equal Exit Velocity
       Characterized flows for different fuels and tip sizes
       Pilot and Assist media Improved Flame Stability




 Pohl, J.H. & N.R. Soelberg, Evaluation of the Efficiency of Industrial Flares: H2S Gas Mixtures and Pilot Assisted
 Flares, EPA-600/2-86-080 September (1986)




                                                                                      IFRF 16th International Members’ Conference:
                                                      Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 9
Flare Efficiency Studies by CMA/EPA/JZ (1983)Ŧ

   Tested Air-Assisted and Steam-Assisted Flares with emphasis on
   determination of combustion efficiency and factors that affect it
   Utilized commercial scale steam and air-assisted flares while burning
   propylene and nitrogen in varying compositions. Factors considered:
    o Flow rate of the relief gas,
    o Heating value of the relief gas, and
    o Steam/relief gas ratio
   Showed flares achieve >98% destruction efficiency if properly
   operated
   Optimal Combustion efficiency with steam to relief gas mass ratio of
   0.4 – 1.5 lbm/lbm
   Over-steaming appeared to occur for steam/relief gas ratio greater
   than 4x recommended steam rates

Ŧ McDaniel, M., Flare Efficiency Study, EPA-600/2-83-052, July (1983)




                                                                      IFRF 16th International Members’ Conference:
                                      Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 10

Factors Important in Flare
Performance

  Smokeless operation¥
  o   Black Smoke = Soot (fv< 10-5 Vol Frac, dprim< 40 nm)
  o   Smoke burns up in high temperature region (smokes if
      soot exits this region before being consumed)
  o   Smoke forms when C-C bonds in hydrocarbons crack and
      aromatic structures grow into multi-ring molecules (>3 ring
      = primary soot particle)
  o   Other Poly-aromatic hydrocarbons (PAH) form along
      reaction route to soot
¥ Moss, J.B., Stewart, C.D., and Young, K.J., “Modeling Soot Formation and Burnout
in a High Temperature Laminar Diffusion Flame Burning under Oxygen-Enriched
Conditions,” Combustion and Flame, 101: 491-500 (1995)

Gollahalli and Parthasaronthy, R.P., "Turbulent Smoke Points in a Cross-Wind,"
Research Testing Services Agreement No. RTSA 3-1-98, University of Oklahoma,
Norman, OK, August (1999).



                                                                     IFRF 16th International Members’ Conference:
                                     Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 11

Factors Important in Flare
Performance
High Exit velocity: use
“momentum ratio” to account
for cross wind effect
  o      Flare gas entrains surrounding air to
         enhance mixing/combustion efficiency
  o      Assist media (steam/air) enhances entrainment
  o      Purge conditions (low momentum ratio) results in flame
         deflection and poor mixing
  o      Flare gas momentum < 10% wind momentum allows flame
         stabilization downwind of tip‡
‡Pohl, J., Gogolek, P., Schwartz, R., and Seebold, J., “The effect of Waste Gas Flow & Composition Steam Assist &
Waste Gas Mass Ratio Wind & Waste Gas Momentum Flux Ratio Wind Turbulence Structure on the Combustion
Efficiency of Flare Flames”

Gogolek, P.E.G., and A.C.S. Hayden, “Efficiency of Flare Flames in Turbulent Crosswind,” Advanced Combustion
Technologies, Natural Resources Canada, American Flare Research Committee, Spring Meeting, May (2002).



                                                                                  IFRF 16th International Members’ Conference:
                                                  Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 12
   Factors Important in Flare Performance
         Flare Gas Heat Content > Minimum Heating Value for
         Stability
          o   Lower Heat value provides less energy to local reaction zone
          o   Combustion at lower flame temperature
          o   Reaction zone more susceptible to flame shearing (quenching)




Pohl, J.H., R. Payne & J. Lee, Evaluation of the Efficiency of Industrial Flares: Test Results, EPA-600/2-84-095, May (1984)


                                                                                          IFRF 16th International Members’ Conference:
                                                          Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Factors Important in Flare Performance                                                              Slide 13



Flare Gas Heat Content > Minimum Heating Value for
Stability
 o   Saturated HC’s: stable flame at
     increasing exit velocities for higher
     gas HV (increased mixing dilutes
     reactants before combusted –
     requires more fuel to compensate)
 o   Unsaturated HC’s: stable flame at
     increasing exit velocities for constant/
     decreasing gas HV (increased mixing
     with fast kinetics and reduced O2 demand for unsaturated HC)
 o   Assist media increases stability (enhanced mixing for flare gas
     with pilots)
 o   Practical operation: increasing C/H ratio (unsaturation) requires
     more assist media


                                                                  IFRF 16th International Members’ Conference:
                                  Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 14
Quantifying Flare Performance Using Flammability Ratio
              and Steam/Fuel Mass Ratio

    General Straight Chain Saturated (Aliphatic) Hydrocarbons
    have Heating Values ~20,000 Btu/lbm
    Flammability Limit represents “mixture” that has sufficient
    oxidant and fuel to react
    Other factors affecting “reaction” include:
     o   Fuel/Oxidant Mixing (turbulent versus laminar)
     o Ignition source (create radicals to promote reaction)
     o “Stability” (radicals to propagate reaction)

    Example Calculation:
     o   Propylene (fuel), Nitrogen (purge), Natural Gas (pilots and
         supplemental fuel), and Steam




                                                                   IFRF 16th International Members’ Conference:
                                   Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 15
Definitions Used in Proposed Performance
Metrics:¥
m = molar, st = stoichiometric, F = Fuel, M = mixture of fuel plus air

o   Vent gas = Waste Fuel Gas + Supplemental Fuel Gas + Purge gas
o   Flare gas = Vent gas + Pilot fuel gas + Steam

o   (FR)m     = (F/CZG) / (F/M)st
o   CZG       = Combustion Zone Gas
              = Flare gas plus added Combustion Air to reach
                Stoichiometric Oxygen
o   (F/M)st   = Fuel / (Fuel + Stoichiometric Air) (molar basis)
o   (FR)m     = Flammability Ratio (molar basis)
              ~ % Lean Flammability Limit / % Stoichiometry

¥ Proposed Metrics by Mr. Brian Dickins, EPA Engineer, Chicago, Illinois




                                                                                   IFRF 16th International Members’ Conference:
                                                   Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 16
    Proposed Performance Metrics for Steam Flares:
    Standard 1 - Steam/Vent Gas Mass Ratio Limit:
    •    Optimum = manufacturer’s recommendation or constant
    •    Maximum ≤ 4 times manufacturer’s recommended value
    •    All flows defined by operating conditions – need Purge Gas
         flow
    •    Purge gas flow rate can be set based on manufacturer value
         or estimated by Husa criteria:
            Purge Gas (scfh)‡ = 0.0035 D3.46K                                                                   (1)
             where: D = flare stack diameter (inches)
                    K = Purge gas constant for specific gases
                      = 2.33 for methane;
                      = 1.71 for N2 with wind
                      = 1.07 for N2 without wind

    Standard 2 – Minimum Gas Heat Content Limit:
    •    If Flare Gas, then LHV ≥ 200 BTU/scf                                                                   (2A)
‡
    •    If Vent Gas, then LHV ≥ 300 BTU/scf                                                                    (2B)
 Berg, L.D., Smith, J.D., Suo-Anttila, A., Price, R., Modi, J., Smith, S., “Flare Purge Rates: Comparison of CFD and
Husa”, AFRC Symposium, Houston, TX (2006)

                                                                                       IFRF 16th International Members’ Conference:
                                                       Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 17

Application of Metrics: Required Information

Input Parameters:
•   Flare diameter (ft) and tip design
•   Waste fuel to be flared, including moisture
•   Wind velocity (ft/hr)
•   Pilot Gas flow rate (scfh)
•   Combustion Air flow into tip zone (lb/hr)

Operational Parameters (to be Specified)
• Purge gas flow rate (lb/hr)
• Supplemental fuel flow rate (lb/hr)
• Steam flow rate to tip for air entrainment/mixing (lb/hr)


                                                              IFRF 16th International Members’ Conference:
                              Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 18


         Example: Calculated Adiabatic Flame Temperature for
           Selected Steam Flow at constant LHV


                                                       Vent              Steam/Flare
            Purge     Steam       Fuel       Vent      Gas Flare Gas Gas Mass          Tip Exit    Adiabatic            Reynolds Froude
          Flow (N2)    Flow       Flow       Flow      LHV       LHV         ratio     Velocity   Flame Temp    FRm       No.      No.
                                                            3         3
Case #     (lbm/hr)   (lbm/hr)   (lbm/hr)   (lbm/hr) (BTU/ft ) (BTU/ft )   (lbm/lbm)   (ft/min)       (ºF)       (-)       (-)       (-)
    1       28          43        14.9       43       552       200        1.00          6.3         2893       0.702     1005      0.016
    2       28         208        55.2       83       1199      200        2.50          10.8        2856       0.702     1716      0.028
    3       28         5554      1360.6     1389      2050      200        4.00         156.0        2843       0.702     24760     0.397
    4       74         113        39.3       113      552       200        1.00          16.7        2893       0.702     2656      0.043
    5       74         549        145.8      220      1199      200        2.50          28.6        2856       0.702     4536      0.073
    6       74        14679      3595.9     3670      2050      200        4.00         412.3        2843       0.702     65438     1.049
    7       148        227        78.6       227      552       200        1.00          33.5        2893       0.702     5311      0.085
    8       148        1099       291.5      440      1199      200        2.50          57.1        2856       0.702     9071      0.145
    9       148       29359      7191.7     7340      2050      200        4.00         824.5        2843       0.702    130876     2.098

 CMA52      2.14       201       0.452      2.592      251      112                                  2330       0.576
 CMA53      1.41       201       0.226      1.636      197      112                                  2323       0.575


 Notes:
 • Flare Gas LHV = (Fuel / Combustion Zone Gas) / (Molar Stoichiometric Ratio Based on Air)
 • Steam and Fuel Flows adjusted to achieve Desired Steam/Flare Gas Mass Ratio and Adiabatic Flame
    Temp calculated for mixture


                                                                                                IFRF 16th International Members’ Conference:
                                                                Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 19

Correlation of Steam to Hydrocarbon Flow vs
Adiabatic Flame Temp (Tad) at constant LHV
    Computed Adiabatic Flame Temperature, F
   o


                                              3000
                                                                                                                       Propylene


                                              2900



                                              2800



                                              2700



                                              2600



                                              2500
                                                     0   0.5   1   1.5         2        2.5         3        3.5         4        4.5

                                                                   Steam to Vent Gas Ratio


                                                                                                         IFRF 16th International Members’ Conference:
                                                                         Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 20


   Example: Calculated Adiabatic Flame Temperature for
     Selected LHV at different Flare Operating Conditions

                                                      Vent                           Steam/Flare
           Purge     Steam       Fuel       Vent      Gas Flare Gas       Tip Exit    Gas Mass    Adiabatic             Reynolds Froude
         Flow (N2)    Flow       Flow       Flow      LHV       LHV       Velocity       ratio   Flame Temp      FRm      No.      No.
                                                           3         3
Case #    (lbm/hr)   (lbm/hr)   (lbm/hr)   (lbm/hr) (BTU/ft ) (BTU/ft )   (ft/min)     (lbm/lbm)     (ºF)         (-)      (-)       (-)
  10        74        81         7.3        81       130        50         13.2          1.00         1619      0.353      2091     0.034
  11        74        223        15.3       89        256       50         14.1          2.50         1586      0.353      2233     0.036
  12        74        397        25.1       99        390       50         15.2          4.00         1574      0.353      2406     0.039
  13        74         90        16.0       90        265       100        14.1          1.00         2283      0.528      2244     0.036
  14        74        280        38.0       112       539       100        16.6          2.50         2243      0.528      2633     0.042
  15        74        594        74.4       148       847       100        20.6          4.00         2229      0.528      3275     0.053
  16        74        151        76.6       151       862       300        20.9          1.00         3165      0.789      3314     0.053
  17        74        330       145.8       220      1199       300        28.6          1.50         3150      0.789      4536     0.073
  18        74        814       332.8       407      1584       300        49.4          2.00         3140      0.789      7838     0.126
  19        74         69        63.4       137       768       400        19.4          0.50         3339      0.841      3082     0.049
 CMA52     2.14       201       0.452      2.592      251       112                                   2330      0.576
 CMA53     1.41       201       0.226      1.636      197       112                                   2323      0.575


 Notes:
 • Vent Gas adjusted to achieve desired (LHV)f level and Adiabatic Flame Temp calculated for mixture
 • Flare Gas LHV = (Fuel/Combustion Zone Gas) / (Molar Stoichiometric Ratio Based on Air)
 • (LHV)f includes Fuel + Steam + Purge
 • CMA data with Low LHV included for comparison purposes



                                                                                                IFRF 16th International Members’ Conference:
                                                                Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 21

Correlation of Vent Gas LHV versus Adiabatic Flame
Temp (Tad ) for Selected Flare Operating Conditions
                                   5000
                                                                                                     Propylene
 Adiabatic Flame Temperature (F)

                                   4500
 o




                                   4000
                                   3500
                                   3000
                                   2500
                                   2000
                                   1500
                                   1000
                                    500
                                          0   500       1000             1500               2000              2500
                                              Vent Gas Lower Heating Value (BTU/scf)




                                                                                          IFRF 16th International Members’ Conference:
                                                          Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 22

                Correlation of Flare Gas LHV versus Adiabatic Flame
                 Temp (Tad ) for Select Flare Operating Conditions
                                  5000
Adiabatic Flame Temperature (F)


                                                                                                      "Propylene"
o




                                  4500                                                                Log. ("Propylene")

                                  4000
                                                                                                         R2 = 0.9941
                                  3500
                                  3000
                                  2500
                                  2000
                                  1500
                                  1000
                                  500
                                         0   50   100   150     200         250        300         350         400         450
                                                  Flare Gas Lower Heating Value (BTU/scf)



                                                                                              IFRF 16th International Members’ Conference:
                                                              Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 23


Correlation of Flammability Ratio (~%FL/%SR) versus
     Adiabatic Flame Temp (Tad ) for Propylene
                                   4000
                                                                                                                (LHV)f = 400
                                   3500                                                                (LHV)f = 300
 Adiabatic Flame Temperature (F)
o




                                                                                             (LHV)f = 200
                                   3000         Inflammable
                                                                                (LHV) f = 100
                                   2500
                                                                                                          Flammable
                                   2000                   (LHV)f = 50
                                                                                   R2 = 0.9963
                                   1500
                                                                                                                         .4
                                                                                                                 Propylene
                                                                                                                 Linear (Propylene)
                                   1000

                                   500

                                     0
                                          0   0.1   0.2       0.3       0.4         0.5          0.6       0.7        0.8         0.9
                                                               FRm (%Flammability/%SR)



                                                                                                    IFRF 16th International Members’ Conference:
                                                                    Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 24



Deficiencies and Limitations
 Need to account for wind effects (i.e., wake stabilized mixing
 versus momentum mixing)
  o   If wind effects added, need good wind data to facilitate
      incorporation into metrics
 Additional testing useful in understanding previous data that
 show low LHV and high combustion efficiency
  o   CMA data indicates “stable” combustion at low heat
      values?
  o   Calculation basis, definition of LHV, etc.
 Metrics do not account for tip geometry effects (i.e., internal
 burning, flame stabilizer rings, etc.)
  o   Impossible in simplified approach to account – CFD useful
      for detailed analysis



                                                               IFRF 16th International Members’ Conference:
                               Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 25
LES Based CFD Represents “BAT” for
Flare Flame Analysis
   CFD captures dynamics of flare flame
   o   Momentum vs. Buoyancy
   o   Wind Effect on Flame Structure
   o   Chemical Reactions
   o   Radiation to/from flame
   Approaches
   o   Eddy Breakup (EBU) Chemistry in Reynold’s Averaged
       Navier-Stokes (RANDS) Formulation (averaged flame
       structure)
   o   Large-Eddy Simulation (LES) with Detailed Chemistry
       and Radiation (accurate flame structure)
   o   LES with EBU Chemistry and Diffuse Radiation




                                                                 IFRF 16th International Members’ Conference:
                                 Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 26



Isis-3D Flare Model:
• Provide reasonably accurate estimates of the total
  heat transfer to objects from large fires
• Predict general characteristics of temperature
  distribution in surrounding objects (i.e., Fence)
• Accurately assess impact of flare operations in
  given ambient conditions (effect of wind speed, fuel
  flow, fuel composition, surrounding equipment for
  given flare geometry)
• Reasonable CPU time requirements using
  “standard” desktop LINUX workstations (i.e., P4
  processor, 1 GByte RAM)



                                                        IFRF 16th International Members’ Conference:
                        Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 27
ISIS-3D Simulation of Multi-Tip Ground Flare (no wind)


                                                                                                                         ~16 m (52 ft)




                                                     Flame height ~11 m (~36’)




                                                                                                                                             12 m (39 ft)
                                                    Non-luminous region ~1 m (3’)

                                                    Tip Height~3 m (10’)


Smith, J.D., Suo-Ahttila, A., Smith, S., and Modi, J., “Estimation of the Air-Demand, Flame Height, and Radiation Load from Low-Profile Flare using ISIS-
3D,” American – Japanese Flame Research Committees International Symposium, Advances in Combustion Technology: Improving the Environment
and Energy Efficiency, Marriott Waikoloa, Hawaii - Oct. 22 –24 (2007)


                                                                                                                 IFRF 16th International Members’ Conference:
                                                                                 Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 28

ISIS-3D Validation: Radiation Predictions
Compared to Experimental Data




Smith, J.D., Suo-Ahttila, A., Smith, S., and Modi, J., “Estimation of the Air-Demand, Flame Height, and Radiation Load from Low-Profile Flare using
ISIS-3D,” American – Japanese Flame Research Committees International Symposium, Advances in Combustion Technology: Improving the
Environment and Energy Efficiency, Marriott Waikoloa, Hawaii - Oct. 22 –24 (2007)


                                                                                                   IFRF 16th International Members’ Conference:
                                                                   Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 29

Wind Effect on Radiative Flux




 Smith, J.D., Suo-Ahttila, A., Smith, S., and Modi, J., “Estimation of the Air-Demand, Flame Height, and Radiation Load from Low-Profile Flare using
 ISIS-3D,” American – Japanese Flame Research Committees International Symposium, Advances in Combustion Technology: Improving the
 Environment and Energy Efficiency, Marriott Waikoloa, Hawaii - Oct. 22 –24 (2007)


                                                                                                    IFRF 16th International Members’ Conference:
                                                                    Combustion and Sustainability: New Technologies, New Fuels, New Challenges
Slide 30

    Conclusions and Recommendations
•   Flare performance effected by cross winds
     –   ratio of flare gas to wind momentum
     –   combining oxidant with fuel
     –   shearing reaction zone
     –   Cooling reaction zone
•   Flare performance effected by steam rate
     – steaming adds additional air to combustion zone
     – over steaming quenches (cools) reaction zone
     – over steaming dilutes reaction zone
•   Flare performance effected by flare gas heating value
     – flare gas (vent + purge + pilots + steam) must be flammable when mixed
       with air to burn
     – Flammability ratio (fuel/flare gas) / (fuel/fuel+air)stio captures
       “combustibility” of flare gas with steam addition to combustion zone
•   LES based CFD represents BAT for Flare Performance analysis
     – includes combustion/soot reactions plus detailed radiation
     – results compare well to test data


                                                                      IFRF 16th International Members’ Conference:
                                      Combustion and Sustainability: New Technologies, New Fuels, New Challenges

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Flare Performance And Analysis Smoot Smith Jackson

  • 1. TECHNICAL FOUNDATIONS TO ESTABLISH NEW CRITERIA FOR EFFICIENT OPERATION OF INDUSTRIAL STEAM-ASSISTED GAS FLARES L. Douglas Smoot, Ph.D., Combustion Resources, Inc. Joseph D. Smith, Ph.D., Idaho National Laboratory Robert E. Jackson, Combustion Resources IFRF 16th International Members’ Conference Combustion and Sustainability: New Technologies, New Fuels, New Challenges 8-10 June, 2009 – Boston Massachusetts, USA
  • 2. Slide 2 Discussion Outline • Basic Flare Operation and Control – Operating/design issues for Pipe Flares and Ground Flares • Historical Performance Analysis – EPA and CMA Data – API Guidelines • Proposed Metrics for Flare Operation – Adiabatic Temperature vs. LHV – Combustion Efficiency vs. Steam Ratio • BAT for Flare Performance Analysis • Conclusions and Recommendations IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 3. Slide 3 Flares in Recent News! Decades of contamination of the water and soil from oil and gas operations mean most food must now be imported, says JNN, and the practice of "gas flaring" has put a toxic pall over many villages. WILLEMSTAD (Reuters) - A refinery on Curacao operated by Venezuela's state oil company is damaging people's health and must cut emissions or face multi-million dollar fines, a court on the Caribbean island ruled on Thursday. Industrial flares burn off pressurized gases but also can shoot out massive In 2007, a Curacao court threatened to close Isla if it cannot amounts of noxious emissions. The meet emissions standards, citing a study estimating that 18 Houston area has about 400 flare people die prematurely every year from contaminant stacks, and they are among the largest exposure. and least- understood sources of pollution in the region, researchers said. Van Unen also took into account excessive flaring that sometimes runs for days and weeks. The amounts to be paid were decided with the serious health consequences and the earnings of PDVSA in mind, the judge stated. IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 4. Slide 4 Operating/Design Issues for Pipe Flares Wind shortens Flame and causes soot formation on back side of flame Flame bends over in wind and licks downwind side of flare stack Air egression into stack tip can lead to internal burning and possible explosive conditions Cross winds cause air P. Gogolek, CANMET Energy egression into flare stack Technology Centre – Ottawa Natural Resources Canada IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 5. Slide 5 Operating/Design Issues for Low Profile Flares High tip velocity increases air entrainment o Tip design controls air entrainment (fuel/air mixing) o High jet velocities = High Jet Noise Pressure Assist improves mixing and combustion o Smoke below certain tip pressure (D-stage pressure) = ambient air entrainment Tip spacing critical o Tips must cross light o Individual tip flames can merge and lengthen overall flare flame o Adjacent rows compete for ambient air (longer flames near flare center) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 6. Slide 6 What is a Flare or Why is there a flame on top of that stack? Flares are Safety Devices used to prevent catastrophic events in systems with highly flammable gases Flares provide safe discharge point for relief devices or in case of loss of containment API RP-521† describes proper flare design and operation but does not define them as “combustors with routine emissions” (e.g., incinerators or process heaters) Plants required to have “Flare minimization plan” as part of air permit – recovery devices operate with quasi-steady flows but can’t operate over large flow ranges possible in hydrocarbon refineries or chemical plants Pollution control devices (i.e., incinerators) combust process emissions Safe and efficient flare design must handle very low hydrocarbon flows (due to fuel cost) and high hydrocarbon flows (due to safety constraints) under variable ambient conditions (i.e., wind and rain) for non-uniform gas compositions †API RP-521, 4th ed., American Petroleum Institute, Washington D.C., March (1997). IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 7. Slide 7 Flare Efficiency Studies (EER) Flare Screening Facility and Flare Test Facility used to analyze flame stability and combustion/destruction efficiency for different fuels and different flare tips (captured/analyzed flare plume) Used 3”, 6”, and 12” Open Pipe Flares plus Air-assisted, Pressure- assisted and Steam-assisted Flares Considered Pilot vs non-pilot operation Considered saturated/unsaturated hydrocarbon, H2S, and NH3 Correlated Flame stability vs Gas heating value and Tip exit velocity o Flame stability defined as Tip velocity > Flame velocity o Assisted flares more stable, Piloted flares more stable, unsaturated fuels more stable (but require more air) Pohl, J.H. & N.R. Soelberg, Evaluation of the Efficiency of Industrial Flares: Flare Head Design and Gas Composition, EPA-600/2-85-106, September (1985) Pohl, J.H. & N.R. Soelberg, Evaluation of the Efficiency of Industrial Flares: H2S Gas Mixtures and Pilot Assisted Flares, EPA-600/2-86-080 September (1986) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 8. Slide 8 Testing on Flame Stability and Heating Value Identified Min HV for Gas where Flame Speed equal Exit Velocity Characterized flows for different fuels and tip sizes Pilot and Assist media Improved Flame Stability Pohl, J.H. & N.R. Soelberg, Evaluation of the Efficiency of Industrial Flares: H2S Gas Mixtures and Pilot Assisted Flares, EPA-600/2-86-080 September (1986) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 9. Slide 9 Flare Efficiency Studies by CMA/EPA/JZ (1983)Ŧ Tested Air-Assisted and Steam-Assisted Flares with emphasis on determination of combustion efficiency and factors that affect it Utilized commercial scale steam and air-assisted flares while burning propylene and nitrogen in varying compositions. Factors considered: o Flow rate of the relief gas, o Heating value of the relief gas, and o Steam/relief gas ratio Showed flares achieve >98% destruction efficiency if properly operated Optimal Combustion efficiency with steam to relief gas mass ratio of 0.4 – 1.5 lbm/lbm Over-steaming appeared to occur for steam/relief gas ratio greater than 4x recommended steam rates Ŧ McDaniel, M., Flare Efficiency Study, EPA-600/2-83-052, July (1983) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 10. Slide 10 Factors Important in Flare Performance Smokeless operation¥ o Black Smoke = Soot (fv< 10-5 Vol Frac, dprim< 40 nm) o Smoke burns up in high temperature region (smokes if soot exits this region before being consumed) o Smoke forms when C-C bonds in hydrocarbons crack and aromatic structures grow into multi-ring molecules (>3 ring = primary soot particle) o Other Poly-aromatic hydrocarbons (PAH) form along reaction route to soot ¥ Moss, J.B., Stewart, C.D., and Young, K.J., “Modeling Soot Formation and Burnout in a High Temperature Laminar Diffusion Flame Burning under Oxygen-Enriched Conditions,” Combustion and Flame, 101: 491-500 (1995) Gollahalli and Parthasaronthy, R.P., "Turbulent Smoke Points in a Cross-Wind," Research Testing Services Agreement No. RTSA 3-1-98, University of Oklahoma, Norman, OK, August (1999). IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 11. Slide 11 Factors Important in Flare Performance High Exit velocity: use “momentum ratio” to account for cross wind effect o Flare gas entrains surrounding air to enhance mixing/combustion efficiency o Assist media (steam/air) enhances entrainment o Purge conditions (low momentum ratio) results in flame deflection and poor mixing o Flare gas momentum < 10% wind momentum allows flame stabilization downwind of tip‡ ‡Pohl, J., Gogolek, P., Schwartz, R., and Seebold, J., “The effect of Waste Gas Flow & Composition Steam Assist & Waste Gas Mass Ratio Wind & Waste Gas Momentum Flux Ratio Wind Turbulence Structure on the Combustion Efficiency of Flare Flames” Gogolek, P.E.G., and A.C.S. Hayden, “Efficiency of Flare Flames in Turbulent Crosswind,” Advanced Combustion Technologies, Natural Resources Canada, American Flare Research Committee, Spring Meeting, May (2002). IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 12. Slide 12 Factors Important in Flare Performance Flare Gas Heat Content > Minimum Heating Value for Stability o Lower Heat value provides less energy to local reaction zone o Combustion at lower flame temperature o Reaction zone more susceptible to flame shearing (quenching) Pohl, J.H., R. Payne & J. Lee, Evaluation of the Efficiency of Industrial Flares: Test Results, EPA-600/2-84-095, May (1984) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 13. Factors Important in Flare Performance Slide 13 Flare Gas Heat Content > Minimum Heating Value for Stability o Saturated HC’s: stable flame at increasing exit velocities for higher gas HV (increased mixing dilutes reactants before combusted – requires more fuel to compensate) o Unsaturated HC’s: stable flame at increasing exit velocities for constant/ decreasing gas HV (increased mixing with fast kinetics and reduced O2 demand for unsaturated HC) o Assist media increases stability (enhanced mixing for flare gas with pilots) o Practical operation: increasing C/H ratio (unsaturation) requires more assist media IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 14. Slide 14 Quantifying Flare Performance Using Flammability Ratio and Steam/Fuel Mass Ratio General Straight Chain Saturated (Aliphatic) Hydrocarbons have Heating Values ~20,000 Btu/lbm Flammability Limit represents “mixture” that has sufficient oxidant and fuel to react Other factors affecting “reaction” include: o Fuel/Oxidant Mixing (turbulent versus laminar) o Ignition source (create radicals to promote reaction) o “Stability” (radicals to propagate reaction) Example Calculation: o Propylene (fuel), Nitrogen (purge), Natural Gas (pilots and supplemental fuel), and Steam IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 15. Slide 15 Definitions Used in Proposed Performance Metrics:¥ m = molar, st = stoichiometric, F = Fuel, M = mixture of fuel plus air o Vent gas = Waste Fuel Gas + Supplemental Fuel Gas + Purge gas o Flare gas = Vent gas + Pilot fuel gas + Steam o (FR)m = (F/CZG) / (F/M)st o CZG = Combustion Zone Gas = Flare gas plus added Combustion Air to reach Stoichiometric Oxygen o (F/M)st = Fuel / (Fuel + Stoichiometric Air) (molar basis) o (FR)m = Flammability Ratio (molar basis) ~ % Lean Flammability Limit / % Stoichiometry ¥ Proposed Metrics by Mr. Brian Dickins, EPA Engineer, Chicago, Illinois IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 16. Slide 16 Proposed Performance Metrics for Steam Flares: Standard 1 - Steam/Vent Gas Mass Ratio Limit: • Optimum = manufacturer’s recommendation or constant • Maximum ≤ 4 times manufacturer’s recommended value • All flows defined by operating conditions – need Purge Gas flow • Purge gas flow rate can be set based on manufacturer value or estimated by Husa criteria: Purge Gas (scfh)‡ = 0.0035 D3.46K (1) where: D = flare stack diameter (inches) K = Purge gas constant for specific gases = 2.33 for methane; = 1.71 for N2 with wind = 1.07 for N2 without wind Standard 2 – Minimum Gas Heat Content Limit: • If Flare Gas, then LHV ≥ 200 BTU/scf (2A) ‡ • If Vent Gas, then LHV ≥ 300 BTU/scf (2B) Berg, L.D., Smith, J.D., Suo-Anttila, A., Price, R., Modi, J., Smith, S., “Flare Purge Rates: Comparison of CFD and Husa”, AFRC Symposium, Houston, TX (2006) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 17. Slide 17 Application of Metrics: Required Information Input Parameters: • Flare diameter (ft) and tip design • Waste fuel to be flared, including moisture • Wind velocity (ft/hr) • Pilot Gas flow rate (scfh) • Combustion Air flow into tip zone (lb/hr) Operational Parameters (to be Specified) • Purge gas flow rate (lb/hr) • Supplemental fuel flow rate (lb/hr) • Steam flow rate to tip for air entrainment/mixing (lb/hr) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 18. Slide 18 Example: Calculated Adiabatic Flame Temperature for Selected Steam Flow at constant LHV Vent Steam/Flare Purge Steam Fuel Vent Gas Flare Gas Gas Mass Tip Exit Adiabatic Reynolds Froude Flow (N2) Flow Flow Flow LHV LHV ratio Velocity Flame Temp FRm No. No. 3 3 Case # (lbm/hr) (lbm/hr) (lbm/hr) (lbm/hr) (BTU/ft ) (BTU/ft ) (lbm/lbm) (ft/min) (ºF) (-) (-) (-) 1 28 43 14.9 43 552 200 1.00 6.3 2893 0.702 1005 0.016 2 28 208 55.2 83 1199 200 2.50 10.8 2856 0.702 1716 0.028 3 28 5554 1360.6 1389 2050 200 4.00 156.0 2843 0.702 24760 0.397 4 74 113 39.3 113 552 200 1.00 16.7 2893 0.702 2656 0.043 5 74 549 145.8 220 1199 200 2.50 28.6 2856 0.702 4536 0.073 6 74 14679 3595.9 3670 2050 200 4.00 412.3 2843 0.702 65438 1.049 7 148 227 78.6 227 552 200 1.00 33.5 2893 0.702 5311 0.085 8 148 1099 291.5 440 1199 200 2.50 57.1 2856 0.702 9071 0.145 9 148 29359 7191.7 7340 2050 200 4.00 824.5 2843 0.702 130876 2.098 CMA52 2.14 201 0.452 2.592 251 112 2330 0.576 CMA53 1.41 201 0.226 1.636 197 112 2323 0.575 Notes: • Flare Gas LHV = (Fuel / Combustion Zone Gas) / (Molar Stoichiometric Ratio Based on Air) • Steam and Fuel Flows adjusted to achieve Desired Steam/Flare Gas Mass Ratio and Adiabatic Flame Temp calculated for mixture IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 19. Slide 19 Correlation of Steam to Hydrocarbon Flow vs Adiabatic Flame Temp (Tad) at constant LHV Computed Adiabatic Flame Temperature, F o 3000 Propylene 2900 2800 2700 2600 2500 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 Steam to Vent Gas Ratio IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 20. Slide 20 Example: Calculated Adiabatic Flame Temperature for Selected LHV at different Flare Operating Conditions Vent Steam/Flare Purge Steam Fuel Vent Gas Flare Gas Tip Exit Gas Mass Adiabatic Reynolds Froude Flow (N2) Flow Flow Flow LHV LHV Velocity ratio Flame Temp FRm No. No. 3 3 Case # (lbm/hr) (lbm/hr) (lbm/hr) (lbm/hr) (BTU/ft ) (BTU/ft ) (ft/min) (lbm/lbm) (ºF) (-) (-) (-) 10 74 81 7.3 81 130 50 13.2 1.00 1619 0.353 2091 0.034 11 74 223 15.3 89 256 50 14.1 2.50 1586 0.353 2233 0.036 12 74 397 25.1 99 390 50 15.2 4.00 1574 0.353 2406 0.039 13 74 90 16.0 90 265 100 14.1 1.00 2283 0.528 2244 0.036 14 74 280 38.0 112 539 100 16.6 2.50 2243 0.528 2633 0.042 15 74 594 74.4 148 847 100 20.6 4.00 2229 0.528 3275 0.053 16 74 151 76.6 151 862 300 20.9 1.00 3165 0.789 3314 0.053 17 74 330 145.8 220 1199 300 28.6 1.50 3150 0.789 4536 0.073 18 74 814 332.8 407 1584 300 49.4 2.00 3140 0.789 7838 0.126 19 74 69 63.4 137 768 400 19.4 0.50 3339 0.841 3082 0.049 CMA52 2.14 201 0.452 2.592 251 112 2330 0.576 CMA53 1.41 201 0.226 1.636 197 112 2323 0.575 Notes: • Vent Gas adjusted to achieve desired (LHV)f level and Adiabatic Flame Temp calculated for mixture • Flare Gas LHV = (Fuel/Combustion Zone Gas) / (Molar Stoichiometric Ratio Based on Air) • (LHV)f includes Fuel + Steam + Purge • CMA data with Low LHV included for comparison purposes IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 21. Slide 21 Correlation of Vent Gas LHV versus Adiabatic Flame Temp (Tad ) for Selected Flare Operating Conditions 5000 Propylene Adiabatic Flame Temperature (F) 4500 o 4000 3500 3000 2500 2000 1500 1000 500 0 500 1000 1500 2000 2500 Vent Gas Lower Heating Value (BTU/scf) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 22. Slide 22 Correlation of Flare Gas LHV versus Adiabatic Flame Temp (Tad ) for Select Flare Operating Conditions 5000 Adiabatic Flame Temperature (F) "Propylene" o 4500 Log. ("Propylene") 4000 R2 = 0.9941 3500 3000 2500 2000 1500 1000 500 0 50 100 150 200 250 300 350 400 450 Flare Gas Lower Heating Value (BTU/scf) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 23. Slide 23 Correlation of Flammability Ratio (~%FL/%SR) versus Adiabatic Flame Temp (Tad ) for Propylene 4000 (LHV)f = 400 3500 (LHV)f = 300 Adiabatic Flame Temperature (F) o (LHV)f = 200 3000 Inflammable (LHV) f = 100 2500 Flammable 2000 (LHV)f = 50 R2 = 0.9963 1500 .4 Propylene Linear (Propylene) 1000 500 0 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 FRm (%Flammability/%SR) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 24. Slide 24 Deficiencies and Limitations Need to account for wind effects (i.e., wake stabilized mixing versus momentum mixing) o If wind effects added, need good wind data to facilitate incorporation into metrics Additional testing useful in understanding previous data that show low LHV and high combustion efficiency o CMA data indicates “stable” combustion at low heat values? o Calculation basis, definition of LHV, etc. Metrics do not account for tip geometry effects (i.e., internal burning, flame stabilizer rings, etc.) o Impossible in simplified approach to account – CFD useful for detailed analysis IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 25. Slide 25 LES Based CFD Represents “BAT” for Flare Flame Analysis CFD captures dynamics of flare flame o Momentum vs. Buoyancy o Wind Effect on Flame Structure o Chemical Reactions o Radiation to/from flame Approaches o Eddy Breakup (EBU) Chemistry in Reynold’s Averaged Navier-Stokes (RANDS) Formulation (averaged flame structure) o Large-Eddy Simulation (LES) with Detailed Chemistry and Radiation (accurate flame structure) o LES with EBU Chemistry and Diffuse Radiation IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 26. Slide 26 Isis-3D Flare Model: • Provide reasonably accurate estimates of the total heat transfer to objects from large fires • Predict general characteristics of temperature distribution in surrounding objects (i.e., Fence) • Accurately assess impact of flare operations in given ambient conditions (effect of wind speed, fuel flow, fuel composition, surrounding equipment for given flare geometry) • Reasonable CPU time requirements using “standard” desktop LINUX workstations (i.e., P4 processor, 1 GByte RAM) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 27. Slide 27 ISIS-3D Simulation of Multi-Tip Ground Flare (no wind) ~16 m (52 ft) Flame height ~11 m (~36’) 12 m (39 ft) Non-luminous region ~1 m (3’) Tip Height~3 m (10’) Smith, J.D., Suo-Ahttila, A., Smith, S., and Modi, J., “Estimation of the Air-Demand, Flame Height, and Radiation Load from Low-Profile Flare using ISIS- 3D,” American – Japanese Flame Research Committees International Symposium, Advances in Combustion Technology: Improving the Environment and Energy Efficiency, Marriott Waikoloa, Hawaii - Oct. 22 –24 (2007) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 28. Slide 28 ISIS-3D Validation: Radiation Predictions Compared to Experimental Data Smith, J.D., Suo-Ahttila, A., Smith, S., and Modi, J., “Estimation of the Air-Demand, Flame Height, and Radiation Load from Low-Profile Flare using ISIS-3D,” American – Japanese Flame Research Committees International Symposium, Advances in Combustion Technology: Improving the Environment and Energy Efficiency, Marriott Waikoloa, Hawaii - Oct. 22 –24 (2007) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 29. Slide 29 Wind Effect on Radiative Flux Smith, J.D., Suo-Ahttila, A., Smith, S., and Modi, J., “Estimation of the Air-Demand, Flame Height, and Radiation Load from Low-Profile Flare using ISIS-3D,” American – Japanese Flame Research Committees International Symposium, Advances in Combustion Technology: Improving the Environment and Energy Efficiency, Marriott Waikoloa, Hawaii - Oct. 22 –24 (2007) IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges
  • 30. Slide 30 Conclusions and Recommendations • Flare performance effected by cross winds – ratio of flare gas to wind momentum – combining oxidant with fuel – shearing reaction zone – Cooling reaction zone • Flare performance effected by steam rate – steaming adds additional air to combustion zone – over steaming quenches (cools) reaction zone – over steaming dilutes reaction zone • Flare performance effected by flare gas heating value – flare gas (vent + purge + pilots + steam) must be flammable when mixed with air to burn – Flammability ratio (fuel/flare gas) / (fuel/fuel+air)stio captures “combustibility” of flare gas with steam addition to combustion zone • LES based CFD represents BAT for Flare Performance analysis – includes combustion/soot reactions plus detailed radiation – results compare well to test data IFRF 16th International Members’ Conference: Combustion and Sustainability: New Technologies, New Fuels, New Challenges