Pilot-Scale Investigation of Heat Flux, Radiation and CO - - PowerPoint PPT Presentation

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Pilot-Scale Investigation of Heat Flux, Radiation and CO - - PowerPoint PPT Presentation

Pilot-Scale Investigation of Heat Flux, Radiation and CO Distribution from an OxyCoal Flame Andrew Fry, Jennifer Spinti, Oscar Diaz-Ibarra, Ignacio Preciado, Teri Draper, Eric Eddings, Terry Ring University of Utah, Institute for Clean and


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SLIDE 1

Pilot-Scale Investigation of Heat Flux, Radiation and CO Distribution from an OxyCoal Flame

Andrew Fry, Jennifer Spinti, Oscar Diaz-Ibarra, Ignacio Preciado, Teri Draper, Eric Eddings, Terry Ring University of Utah, Institute for Clean and Secure Energy U.S. Department of Energy, Agreement # DE-NA0002375 2015 AIChE Annual Meeting

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SLIDE 2
  • Project Overview
  • Experimental Setup
  • Initial Modeling Efforts
  • Heat Removal and Radiation Data
  • Summary & Conclusions
  • Questions

Presentation Road Map

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SLIDE 3
  • Project Overview
  • Experimental Setup
  • Initial Modeling Efforts
  • Heat Removal and Radiation Data
  • Summary & Conclusions
  • Questions

Presentation Road Map

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SLIDE 4

Project Objective

Implementation of exascale computing with V&V/UQ to more rapidly deploy a new technology for providing low cost, low emission electric power generation V&V/UQ – Verification & Validation with Uncertainty Quantification

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SLIDE 5

Project Objective

  • V/UQ performed on data produced at 4 scales

– Bench-scale, Lab-scale (~100 kWth), Large-scale (~1-5 MWth), Pilot-scale (~15 MWth)

  • Ultimate goal to design a next-generation 350 MWe oxy-coal

boiler

  • Year 1 of a 5 year program is complete
  • Focus here will be on a 1.5 MWth data set
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SLIDE 6
  • Project Overview
  • Experimental Setup
  • Initial Modeling Efforts
  • Heat Removal and Radiation Data
  • Summary & Conclusions
  • Questions

Presentation Road Map

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SLIDE 7

5.0 MBtu/hr Pilot-Scale Furnace (L1500)

Unique L1500 Capabilities:

  • Realistic Burner Turbulent Mixing Scale
  • Realistic Radiative Conditions
  • Realistic Time – Temperature Profile

FD and Recycle Fan Convective Section Baghouse Air/FGR/O2 Control Radiative Section Burner Sample Ports

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SLIDE 8

Bluff Body (Not installed in these tests) Primary (Coal carrier) Natural Gas (For heat up) Inner Secondary Air or O2/FGR Mixture Outer Secondary Air or O2/FGR Mixture

Dual Register Low-NOx Burner (LNB)

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SLIDE 9

Furnace Cooling Coils and Plates

Cooling Coils (8 installed) Cooling Plates (3 installed) Heat removal by cooling surfaces is determined by measuring cooling water flow and temperature in and out

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SLIDE 10

α field of view = 2 * Tan -1 ((D2/2)/Lp2) = 2.74

Sensing thermistors Focusing lens Water-cooled jacket Field of view Lp1 Lp2 D2 D1

Radiometer Configuration

Three radiometers are installed opposite the cooling plates. Angle of view Includes only the cooling plate surface Black body radiator was used to calibrate these devices

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SLIDE 11

Radiometer Configuration

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SLIDE 12

Infrared Heat Flux Measurement

FLIR infrared camera in the wavelength range of 3825–3975 nm. The camera was calibrated with a blackbody generator, which is a source of known emission, in order to obtain infrared heat flux data.

At times placed in one of the first three sections Across from the cooling plates

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SLIDE 13

Units Target 0% Swirl 100% Swirl Firing Rate Btu/hr 3.5 Coal Rate lb/hr 297.0 297.0 296.9 Primary FGR lb/hr 450.2 461.9 461.7 Primary O2 lb/hr 85.3 86.4 86.3 Inner Secondary FGR lb/hr 361.9 362.0 362.0 Inner Secondary O2 lb/hr 105.9 114.0 106.3 Inner Secondary Temp ˚F 500.0 496.2 502.3 Outer Secondary FGR lb/hr 1448.6 1440.3 1449.2 Outer Secondary O2 lb/hr 422.6 418.2 418.4 Outer Secondary Temp ˚F 500.0 498.6 501.9 O2 % 3.0 2.6 2.9 CO2 % 96.1 85.7 88.2 C 66.9 H 4.5 N 1.2 S 0.4 O 13.6 Ash 7.9 Moisture 5.6 Volatile Matter 40.4 Fixed Carbon 46.1 HHV, Btu/lb 11,765 * all values in mass % unless otherwise specified

Targeted and Actual Conditions Utah Sufco Coal Composition

Difference in CO2 concentration due to air leakage, which occurs mainly through the FGR recycle fan and is a function of back pressure through the burner. More leakage occurs at 0% swirl condition

Experimental Conditions

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SLIDE 14
  • Project Overview
  • Experimental Setup
  • Initial Modeling Efforts
  • Heat Removal and Radiation Data
  • Summary & Conclusions
  • Questions

Presentation Road Map

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SLIDE 15

Experimental and Predicted Values

model experiment

Gas temperature profile predictions using LES model Prediction and measurement of cooling coil heat flux We have high confidence in our ability to accurately represent gas-phase and entrained particle properties (emissivity, heat capacity)

Why then the disconnect between model and experiment?

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SLIDE 16
  • Project Overview
  • Experimental Setup
  • Initial Modeling Efforts
  • Heat Removal and Radiation Data
  • Summary & Conclusions
  • Questions

Presentation Road Map

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SLIDE 17

100000 120000 140000 160000 180000 200000 220000 12:50:01 12:51:27 12:52:54 12:54:20 12:55:47 12:57:13 12:58:39 13:00:06 Heat Removal (Btu/hr) Section 1 Section 2 Section 3 Section 4 100000 120000 140000 160000 180000 200000 220000 12:50:01 12:51:27 12:52:54 12:54:20 12:55:47 12:57:13 12:58:39 13:00:06 Heat Removal (Btu/hr) Section 1 Section 2 Section 3 Section 4

Change from 0% to 100% Swirl Change from 0% to 100% Swirl

100000 120000 140000 160000 180000 200000 220000 Sec 1 Sec 2 Sec 3 Sec 4

Heat Removal (Btu/hr)

South Cooling Coils

0 Swirl 100 Swirl 100000 120000 140000 160000 180000 200000 220000 Sec 1 Sec 2 Sec 3 Sec 4

Heat Removal (Btu/hr)

North Cooling Coils

0 Swirl 100 Swirl

Cooling Coil Data (Change from 0 to 100% Swirl)

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SLIDE 18

100000 120000 140000 160000 180000 200000 220000 10:48:00 12:00:00 13:12:00 14:24:00 Heat Removal (Btu/hr) Section 1 Section 2 Section 3 Section 4 100000 120000 140000 160000 180000 200000 220000 10:48:00 12:00:00 13:12:00 14:24:00 Heat Removal (Btu/hr) Section 1 Section 2 Section 3 Section 4

Change from 0% to 100% Swirl Change from 0% to 100% Swirl

South Cooling Coils North Cooling Coils

Cooling Coil Data (Long Times)

Heat removal through the cooling tubes steadily decreases This is consistent with increasing insulating layer thickness due to deposition

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SLIDE 19

100 % swirl 0 % swirl

Time

Radiometer 1 Radiometer 2 Radiometer 3 100 % swirl 0 % swirl

Time

Section 1 Section 2 Section 3

15848 53884 22188 28527 34866 41206 47545 60224 66563 Heat Flux (Btu/ft2 hr)

Radiometer Data (Long Times)

Heat flux to radiometers increases steadily over time Wall temperatures are stable Why?

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SLIDE 20

Infrared Heat Flux Data

FLAME NO FLAME

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SLIDE 21

Ash Deposits

Probably peeled off during shut down Deposit is extensive For 1 week of testing

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CO Distribution

0 % Swirl 100 % Swirl

CO (ppmv) CO (ppmv)

Distance from Burner (m) 4.3 5.5 6.7 7.9 9.1 10.4 11.6 0.0 0.3 0.6 Distance from Center (m) 4.3 5.5 6.7 7.9 9.1 10.4 11.6 0.0 0.3 0.6 Distance from Center (m) Distance from Burner (m)

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SLIDE 23

Observations

  • An accurate prediction of heat flux through heat

exchange surfaces requires:

– Accurate representation of surface properties which are dominated by deposited mineral mater – Emissivity, thermal conductivity and deposit thickness must be known accurately

  • Predictive tool must include accurate representation
  • f deposit rate and mineral composition
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SLIDE 24
  • Project Overview
  • Experimental Setup
  • Initial Modeling Efforts
  • Heat Removal and Radiation Data
  • Summary & Conclusions
  • Questions

Presentation Road Map

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SLIDE 25

Summary & Conclusions

  • An oxy-coal combustion data set was produced to be

used for V&V/UQ

  • Air Leakage was higher than desired and occurs

primarily in the recycle fan

  • Heat removal through the coils is sensitive to burner

changes and consistent with expected flame behavior

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SLIDE 26

Summary & Conclusions

  • Heat removal through the coils decreases

continuously due to ash deposition on heat transfer surface

  • Radiometer data increases continuously due to ash

buildup and change in surface emissivity

  • CFD Modeling is Underway

– Trends in heat flux and temperature are well represented – Magnitude is not exact – Most likely due to assignment of surface boundary conditions (emissivity, conductivity, etc.)

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SLIDE 27

Summary & Conclusions

  • Current efforts include:

– Measurement of the physical properties of the ash containing surfaces

  • For the next round of testing the following

modifications will be made:

– Upgrade of recycle fan to reduce air inleakage – Addition of soot blowing for cooling tubes and plates

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SLIDE 28
  • Project Overview
  • Experimental Setup
  • Initial Modeling Efforts
  • Heat Removal and Radiation Data
  • Summary & Conclusions
  • Questions

Presentation Road Map