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A Correlation for Flame Length of Oxygen-
Assisted, Swirled, Coal and Biomass Flames
David Ashworth, John Tobiasson, Dale Tree
Bhupesh Dhungel
Air Liquide, USA
Clearwater Clean Coal Conference
June 7th, 2016
1
Introduction
• Biomass has been investigated for use in coal-fired power plants as a CO2-
neutral fuel
• Longer biomass flames become an issue in fixed volume boilers designed
to burnout coal
• The effects of oxygen enrichment and swirl on biomass flames were
explored
• Trends in NOx formation and burnout associated with flame length are
apparent as burner geometry, swirl, and O2 flow rates change
• A model to predict such trends could aid in the design of optimal burner
geometries
• Efforts have been made to model flame length for gaseous flames
• An initial, low-fidelity mathematical model for solid fuel flames with curve-fit
constants was created
2
Experimental Setup
Burner Flow Reactor (BFR) 2.4 m length
0.75 m diameter
150 kWth
3
Background - Visual Model
Enlarged View
1
2 2
3 3
1 – Center flow (Oxygen Enrichment)
4
2 – Primary flow (Solid Fuel in Air)
3 – Secondary flow (Air and Oxygen)
Background - Volatiles Flame
Determine axial location where fuel and
air mix to a stoichiometric composition
𝐶𝑠
𝐿 𝑓
5
𝑐 𝑠 =
𝑚 𝑓𝑢𝑒𝑙
𝑚 𝑜𝑥 𝑠
Background - Flame Length Model
𝑐 𝑠 =
𝑚 𝑓𝑢𝑒𝑙
𝑚 𝑜𝑥 𝑠
=
𝜌 𝑚𝑖𝑥 𝑉𝑝
𝜋
4
𝑑 𝑝
2
− 𝑑 𝑐
2
∗ 𝑌𝑓𝑢𝑒𝑙,𝑝
𝑌𝑂2,𝑠𝑒𝑐 𝜌𝑠𝑒𝑐 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝜋𝑑 𝑝 𝐿 𝑓 𝑐1 + 𝜌𝑠𝑒𝑐 𝑈 𝑅𝑍 𝜋𝑏𝐿 𝑓 𝑐2 + 𝑚 𝑂2,𝑐 + 𝑚 𝑂2,𝑝
𝑈 𝑅𝑍 =
0.2 ∗ 𝑆 ∗ 𝑉𝑠𝑒𝑐
0.2 + 𝑆
Recirculation term including
swirl and velocity
Mixing due to
Recirculation
Mixing due to shearing
between streams
𝑑 𝑐
𝑑 𝑝
𝑏
𝐿 𝑓
𝑚 = 𝜌𝑉𝐴
6
Background - Flame Length Model
𝐿 𝑓 =
𝑚 𝑓𝑢𝑒𝑙
𝑐 𝑠
− 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐
𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐
Factor out Lf (flame length) and rearrange terms
7
Total Fuel
Empirical Constants
Objectives
1. Refine the flame length model by:
– Using volatiles fraction from ASTM Proximate Analysis
– Predicting empirical constants
2. Compare modeled results to experimental data
8
Straw Medium Fine Switchgrass PRB Coal
Wood Wood
0.7381 0.7906 0.7642 0.6778 0.3376
Results - Volatiles Fraction
For total fuel mass flow:
• Correlation is good for biomass
• Coal data is more horizontally oriented
9
0.0
0.5
1.0
1.5
2.0
2.5
0.0 0.5 1.0 1.5 2.0 2.5
TheoreticalCalculatedLength(m)
Visual Length (m)
Med. Wood
Fine Wood
Straw
Coal
Switchgrass
0.0
0.5
1.0
1.5
2.0
2.5
0.0 0.5 1.0 1.5 2.0 2.5
TheoreticalCalculatedLength(m)
Visual Length (m)
Med. Wood
Fine Wood
Straw
Switchgrass
Coal
Results - Volatiles Fraction
10
For volatiles mass flow:
• Scatter increases slightly for all fuels
• Coal data correlates better
Straw Medium Fine Switchgrass PRB Coal
Wood Wood
0.7381 0.7906 0.7642 0.6778 0.3376
Results - Empirical Constants
11
0.0000
0.0005
0.0010
0.0015
0.0020
0.0025
0.0030
0.0035
0.0040
0 100 200 300 400 500
C1Value
Mean Particle Size (μm)
Fuel c1 c2
Coal 0.00000 0.02156
Fine Wood 0.00000 0.04915
Straw 0.00000 0.02675
Med Wood 0.00352 0.02823
Switchgrass 0.00326 0.02362
y = -3E-05x + 0.0374
R² = 0.141
0.00
0.01
0.02
0.03
0.04
0.05
0.06
0 100 200 300 400 500
C2Value
Mean Particle Size (μm)
𝐿 𝑓 =
𝑚 𝑓𝑢𝑒𝑙
𝑐 𝑠
− 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐
𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐
Results - Empirical Constants
12
𝐿 𝑓 =
𝑚 𝑓𝑢𝑒𝑙
𝑐 𝑠
− 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐
𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐
-0.0005
0.0000
0.0005
0.0010
0.0015
0.0020
0.0025
0.0030
0.0035
0.0040
0 100 200 300 400 500
C1Value
Mean Particle Size (μm)
0.0000
0.0005
0.0010
0.0015
0.0020
0.0025
0.0030
0.0035
0.0040
0 100 200 300 400 500
C1Value
Mean Particle Size (μm)
𝑐1 =
0.1854
𝐷 − 443
− 7.147 ∗ 10−4
Results - Empirical Constants
13
𝐿 𝑓 =
𝑚 𝑓𝑢𝑒𝑙
𝑐 𝑠
− 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐
𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐
𝑐2 = (−9.677 ∗ 10−5
𝐷 + 7.482 ∗ 10−2
) ∗ 𝑓𝑣
y = -3E-05x + 0.0374
R² = 0.141
0.00
0.01
0.02
0.03
0.04
0.05
0.06
0 100 200 300 400 500
C2Value
Mean Particle Size (μm)
y = -0.0000968x + 0.0748245
R² = 0.9582012
0.00
0.01
0.02
0.03
0.04
0.05
0.06
0.07
0 100 200 300 400 500
C2/VolatilesFraction
Mean Particle Size (μm)
Results - Refined Model
14
𝐿 𝑓 =
𝑚 𝑓𝑢𝑒𝑙 ∗ 𝑓𝑣
𝑐 𝑠
− 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐
𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐
𝑐1 =
0.1854
𝐷 − 443
− 7.147 ∗ 10−4
𝑐2 = (−9.677 ∗ 10−5
𝐷 + 7.482 ∗ 10−2
) ∗ 𝑓𝑣
Results - Comparison
15
• Overall scatter has increased but not within a specific fuel
0.0
0.5
1.0
1.5
2.0
2.5
0.0 0.5 1.0 1.5 2.0 2.5
TheoreticalCalculatedLength(m)
Visual Length (m)
Med. Wood
Fine Wood
Straw
Switchgrass
Coal
Conclusions
• A model has been created which predicts volatiles flame
length for solid fuel as a function of burner geometry, flow
rates, and fuel properties
• Two constants which were previously determined empirically
were found to be predicted well by particle size and volatiles
fraction making the model fully predictive
• The model enables an understanding of how the following
parameters impact flame length:
– Volatiles fraction
– Oxygen addition, location and flow rates
– Swirl
– Primary and secondary velocities
– Burner diameters
– Particle Size
16
Thank You
Questions
17
Results
18
0.0
0.5
1.0
1.5
2.0
2.5
0.0 0.5 1.0 1.5 2.0 2.5
TheoreticalCalculatedLength(m)
Visual Length (m)
Med. Wood
Fine Wood
Straw
Coal
Switchgrass
0.0
0.5
1.0
1.5
2.0
2.5
0.0 0.5 1.0 1.5 2.0 2.5
TheoreticalCalculatedLength(m)
Visual Length (m)
Med. Wood
Fine Wood
Straw
Switchgrass
Coal
Initial Final
CO Mapping
19
Coal Wood
• Visual and CO flame lengths follow similar trends

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Clearwater 2016

  • 1. A Correlation for Flame Length of Oxygen- Assisted, Swirled, Coal and Biomass Flames David Ashworth, John Tobiasson, Dale Tree Bhupesh Dhungel Air Liquide, USA Clearwater Clean Coal Conference June 7th, 2016 1
  • 2. Introduction • Biomass has been investigated for use in coal-fired power plants as a CO2- neutral fuel • Longer biomass flames become an issue in fixed volume boilers designed to burnout coal • The effects of oxygen enrichment and swirl on biomass flames were explored • Trends in NOx formation and burnout associated with flame length are apparent as burner geometry, swirl, and O2 flow rates change • A model to predict such trends could aid in the design of optimal burner geometries • Efforts have been made to model flame length for gaseous flames • An initial, low-fidelity mathematical model for solid fuel flames with curve-fit constants was created 2
  • 3. Experimental Setup Burner Flow Reactor (BFR) 2.4 m length 0.75 m diameter 150 kWth 3
  • 4. Background - Visual Model Enlarged View 1 2 2 3 3 1 – Center flow (Oxygen Enrichment) 4 2 – Primary flow (Solid Fuel in Air) 3 – Secondary flow (Air and Oxygen)
  • 5. Background - Volatiles Flame Determine axial location where fuel and air mix to a stoichiometric composition 𝐶𝑠 𝐿 𝑓 5 𝑐 𝑠 = 𝑚 𝑓𝑢𝑒𝑙 𝑚 𝑜𝑥 𝑠
  • 6. Background - Flame Length Model 𝑐 𝑠 = 𝑚 𝑓𝑢𝑒𝑙 𝑚 𝑜𝑥 𝑠 = 𝜌 𝑚𝑖𝑥 𝑉𝑝 𝜋 4 𝑑 𝑝 2 − 𝑑 𝑐 2 ∗ 𝑌𝑓𝑢𝑒𝑙,𝑝 𝑌𝑂2,𝑠𝑒𝑐 𝜌𝑠𝑒𝑐 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝜋𝑑 𝑝 𝐿 𝑓 𝑐1 + 𝜌𝑠𝑒𝑐 𝑈 𝑅𝑍 𝜋𝑏𝐿 𝑓 𝑐2 + 𝑚 𝑂2,𝑐 + 𝑚 𝑂2,𝑝 𝑈 𝑅𝑍 = 0.2 ∗ 𝑆 ∗ 𝑉𝑠𝑒𝑐 0.2 + 𝑆 Recirculation term including swirl and velocity Mixing due to Recirculation Mixing due to shearing between streams 𝑑 𝑐 𝑑 𝑝 𝑏 𝐿 𝑓 𝑚 = 𝜌𝑉𝐴 6
  • 7. Background - Flame Length Model 𝐿 𝑓 = 𝑚 𝑓𝑢𝑒𝑙 𝑐 𝑠 − 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐 𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐 Factor out Lf (flame length) and rearrange terms 7 Total Fuel Empirical Constants
  • 8. Objectives 1. Refine the flame length model by: – Using volatiles fraction from ASTM Proximate Analysis – Predicting empirical constants 2. Compare modeled results to experimental data 8
  • 9. Straw Medium Fine Switchgrass PRB Coal Wood Wood 0.7381 0.7906 0.7642 0.6778 0.3376 Results - Volatiles Fraction For total fuel mass flow: • Correlation is good for biomass • Coal data is more horizontally oriented 9 0.0 0.5 1.0 1.5 2.0 2.5 0.0 0.5 1.0 1.5 2.0 2.5 TheoreticalCalculatedLength(m) Visual Length (m) Med. Wood Fine Wood Straw Coal Switchgrass
  • 10. 0.0 0.5 1.0 1.5 2.0 2.5 0.0 0.5 1.0 1.5 2.0 2.5 TheoreticalCalculatedLength(m) Visual Length (m) Med. Wood Fine Wood Straw Switchgrass Coal Results - Volatiles Fraction 10 For volatiles mass flow: • Scatter increases slightly for all fuels • Coal data correlates better Straw Medium Fine Switchgrass PRB Coal Wood Wood 0.7381 0.7906 0.7642 0.6778 0.3376
  • 11. Results - Empirical Constants 11 0.0000 0.0005 0.0010 0.0015 0.0020 0.0025 0.0030 0.0035 0.0040 0 100 200 300 400 500 C1Value Mean Particle Size (μm) Fuel c1 c2 Coal 0.00000 0.02156 Fine Wood 0.00000 0.04915 Straw 0.00000 0.02675 Med Wood 0.00352 0.02823 Switchgrass 0.00326 0.02362 y = -3E-05x + 0.0374 R² = 0.141 0.00 0.01 0.02 0.03 0.04 0.05 0.06 0 100 200 300 400 500 C2Value Mean Particle Size (μm) 𝐿 𝑓 = 𝑚 𝑓𝑢𝑒𝑙 𝑐 𝑠 − 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐 𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐
  • 12. Results - Empirical Constants 12 𝐿 𝑓 = 𝑚 𝑓𝑢𝑒𝑙 𝑐 𝑠 − 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐 𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐 -0.0005 0.0000 0.0005 0.0010 0.0015 0.0020 0.0025 0.0030 0.0035 0.0040 0 100 200 300 400 500 C1Value Mean Particle Size (μm) 0.0000 0.0005 0.0010 0.0015 0.0020 0.0025 0.0030 0.0035 0.0040 0 100 200 300 400 500 C1Value Mean Particle Size (μm) 𝑐1 = 0.1854 𝐷 − 443 − 7.147 ∗ 10−4
  • 13. Results - Empirical Constants 13 𝐿 𝑓 = 𝑚 𝑓𝑢𝑒𝑙 𝑐 𝑠 − 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐 𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐 𝑐2 = (−9.677 ∗ 10−5 𝐷 + 7.482 ∗ 10−2 ) ∗ 𝑓𝑣 y = -3E-05x + 0.0374 R² = 0.141 0.00 0.01 0.02 0.03 0.04 0.05 0.06 0 100 200 300 400 500 C2Value Mean Particle Size (μm) y = -0.0000968x + 0.0748245 R² = 0.9582012 0.00 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0 100 200 300 400 500 C2/VolatilesFraction Mean Particle Size (μm)
  • 14. Results - Refined Model 14 𝐿 𝑓 = 𝑚 𝑓𝑢𝑒𝑙 ∗ 𝑓𝑣 𝑐 𝑠 − 𝑚 𝑂2,𝑝 − 𝑚 𝑂2,𝑐 𝜌 𝑉𝑝 − 𝑉𝑠𝑒𝑐 𝑑 𝑝 𝜋𝑐1 + 𝜌𝑠𝑒𝑐 𝜋𝑏𝑈 𝑅𝑍 𝑐2 𝑌𝑂2,𝑠𝑒𝑐 𝑐1 = 0.1854 𝐷 − 443 − 7.147 ∗ 10−4 𝑐2 = (−9.677 ∗ 10−5 𝐷 + 7.482 ∗ 10−2 ) ∗ 𝑓𝑣
  • 15. Results - Comparison 15 • Overall scatter has increased but not within a specific fuel 0.0 0.5 1.0 1.5 2.0 2.5 0.0 0.5 1.0 1.5 2.0 2.5 TheoreticalCalculatedLength(m) Visual Length (m) Med. Wood Fine Wood Straw Switchgrass Coal
  • 16. Conclusions • A model has been created which predicts volatiles flame length for solid fuel as a function of burner geometry, flow rates, and fuel properties • Two constants which were previously determined empirically were found to be predicted well by particle size and volatiles fraction making the model fully predictive • The model enables an understanding of how the following parameters impact flame length: – Volatiles fraction – Oxygen addition, location and flow rates – Swirl – Primary and secondary velocities – Burner diameters – Particle Size 16
  • 18. Results 18 0.0 0.5 1.0 1.5 2.0 2.5 0.0 0.5 1.0 1.5 2.0 2.5 TheoreticalCalculatedLength(m) Visual Length (m) Med. Wood Fine Wood Straw Coal Switchgrass 0.0 0.5 1.0 1.5 2.0 2.5 0.0 0.5 1.0 1.5 2.0 2.5 TheoreticalCalculatedLength(m) Visual Length (m) Med. Wood Fine Wood Straw Switchgrass Coal Initial Final
  • 19. CO Mapping 19 Coal Wood • Visual and CO flame lengths follow similar trends

Editor's Notes

  1. Flame length affects NOx, burnout, heat transfer, deposition, and corrosion, which all can become an issue for biomass in coal boilers.
  2. Variable diameter tubes.
  3. This is for a volatiles flame. The classical method found in many textbooks to determine flame length is to find the boundary where the mixture fraction is stoichiometric along the centerline. We thought to apply this to turbulent flames as an average.
  4. Recirculation and shearing terms are ideas borrowed from Chen and Driscoll. Urz is a term we created as a parameter to fit our model to Chen and Driscoll’s swirl data. Vr,shearing=|Vp-Vsec|C1 Vr,recirculation=UrzC2 Constants are proportionality constants for radial velocity terms Use the term FUEL RICH REGION.
  5. Again this fuel mass flow is the total solid fuel flow (moisture + volatiles + carbon + ash). C1 and C2 are constants determined by a curve-fit to empirical data.
  6. Dry, ash-free volatiles fractions. We recognize our low fidelity measurements. Visual lengths varied on the order of 20 cm between individuals. We visually measured flame length (very low fidelity) over MANY data points (high fidelity). We could have measured with a camera and a photo processing program to get higher fidelity measurements, but then we could not have taken measurements at nearly as many data points.
  7. Groups of coal data are various oxygen flows. Upper group is No oxygen and Secondary; Middle group is 4 kg/hr O2 (at 0, 6, 6, and 9 turns of swirl); Lower group is 8 kg/hr O2 (at 0, 6, 6, 9 turns of swirl as well)