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Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL 3. Results and Validation 1 Simcha Singer, William Green Dept. of Chemical Engineering, MIT

Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

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Page 1: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

Numerical Simulation of Forward and Static Smoldering Combustion

Outline

1. Introduction

2. Numerical Implementation in COMSOL

3. Results and Validation

1

Simcha Singer, William Green

Dept. of Chemical Engineering, MIT

Page 2: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

Physics and Chemistry of Smoldering Combustion in a Cigarette

• Simulation domain encompasses tobacco rod, filter, paper and surrounding air

• Evaporation and pyrolysis zone exist ahead of oxidation zone due to pre-heating

• Transient problem due to alternation between natural smoldering and puffing

• Most air enters at paper burn line, radial advection and diffusion occur

• Local thermal equilibrium between gas and solid does not always hold

• Effective transport and thermo-physical properties depend on structure and change markedly with conversion (e.g. permeability, conductivity, diffusivities, etc.)

Porous Tobacco Filter

Wrapping paper

Adapted from Baker, R R, PECS, 7, (1981), 135-153

Air

Pyrolysis

Oxidation

Condensation and

Filtration

Paper

Burn Line

Page 3: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

3

Numerical Implementation in COMSOL

2-D axisymmetric domain employed

Physics interfaces used:

• (Reaction Engineering, synced with: )

• Free and Porous Media Flow: Regions 1,2,3,4 (Source term in Region 2 accounts for solid-to-gas reaction)

• Transport of Concentrated Species: Regions 1,2,3,4 (Source terms in Region 2 account for reactions)

• Heat Transfer in Fluids: Regions 1,2,3,4 (Source terms account for interphase heat transfer in Regions 2,3,4)

and

• Heat Transfer in Solids: Regions 2,3,4 (Source terms account for heats of reaction and interphase heat transfer)

• Domain ODEs: Region 2 (for tobacco, char and moisture densities)

• Domain ODE: Region 4 (for paper permeability)

Ignition Tsolid

70 mm

12 mm

20 mm

109 mm

50 μm 4 mm

Free Flow

Porous Tobacco

28 mm

Filter

Porous Paper

Region #1

Region #2

Region #3

Region #4

r

Page 4: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

4

Numerical Implementation: Volume Averaged Conservation Equations

,

j

j j j k k j

k

ww w Q

t

u J

,( ) ( ) ( ) ( )g

p eff eff g j p j g g s g s s g

j

Tc k T N c T h A T T

t

,( ) j k k

j k

Qt

u

,

,

solid i

i k k

k

d

dt

Gas Species Eq:

Mass Conservation:

Thermal Energy (Gas):

Solid Species (char, volatile precursors):

Momentum (porous rod):

2

1 2( ) ( )

3

TQp

t

u uu u u u u I F

2

( ) ( )3

Tpt

uu u u u u I F

Thermal Energy (Solid):

( ) ( ) ( ) ( )sp eff eff s r k g s g s g s

k

Tc k T h h A T T

t

6 Major Gas Species included (O2, CO, CO2, N2, H2O and “Volatiles”)

Momentum (free flow):

Page 5: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

Numerical Implementation in COMSOL

5

Mesh and Elements Details:

• Non-uniform mapped mesh (thin paper!) elements for porous regions

• Free quad elements in free flow region

• Most elements linear, although 2nd order shape functions used for some variables

Normal Stress = 0

Ignition Tsolid

Solver Settings:

• Time dependent BDF solver

• Newton’s Method at each time step

• Employed either Direct MUMPS solver or Iterative GMRES with Multigrid Preconditioner and Vanka pre- and post-smoothers

Initial and Boundary Conditions

• Atmospheric initial conditions with zero initial velocity are employed

• Puffing/smoldering transition via application of prescribed flow rate at outlet

Symmetry BCs (no flux)

Tg=Tamb

Tg=Tamb

wi=wi,amb

wi=wi,amb

Outflow BCs

Normal Stress = 0

Ignition Tsolid

Surface to Ambient Radiation BCs for Tsolid

Open boundary

Open boundary

Ignition BC

Page 6: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

6

Numerical Implementation in COMSOL: Sub-models

• Properties calculated dynamically as function of temperature, porosity, etc.

• Diffusion is calculated using the Maxwell-Stefan approach for multi-component diffusion, accounts for porous medium

• Temperature dependent thermal conductivities and viscosity of gas mixture are incorporated, effective thermal conductivities for each phase

• Pyrolysis reactions: 4-precursor model

• Solid conductivity accounts for contribution of shred-to-shred radiation

• Solid-to-gas heat transfer coefficient

• Tobacco permeability increases 3 orders of magnitude with conversion

• Paper burns @ 723 K and permeability increases by 20 orders of magnitude

Riley D, et al., PhysicoChemical Hydrodynamics, 7, (1986), 255-279

Muramatsu M et al., Beitr. Tabakforsch, 11, (1981), 79-86 Saidi et al., App. Math. Mod., 31 (2007) 1970-1996

Log10(κ) [m2])

Time = 30 [s]

0.5 [s] into Puff

[m] [m]

2 [s] into Puff

Page 7: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

7

Numerical Implementation in COMSOL: Validation

• In order to validate simulation, we must use identical conditions and properties as experiments…

• Employed full-size cigarette and extended domain radially to twice the cigarette radius

• Incorporated paper permeability used in experiments and used paper’s O2 diffusivity given by Riley 1986

• Employed full Puff/Smolder cycles for ISO Regime:

-Puff volume: 35 cc/ 2 sec -Smoldering interval: 58 sec

• Similar to experiment, 9 mm of cigarette is covered by smoking machine

• Still some unknown parameters, use same sub-models as literature (Saidi et al. 2007)

Baker, R R, High Temp. Science, 7 (1975) 236-247 Baker, R R, Beitr. Tabakforsch, 11, (1981), 1-17 Riley D, et al., PhysicoChemical Hydrodynamics, 7, (1986), 255-279

Mesh Consists of 8341 elements

[m]

Page 8: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

Mesh Refinement

Solid Temperature at z=55 mm

Oxygen Mass Fraction at z=55 mm

Gas Temperature at z=55 mm

Page 9: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

[K]

Tgas Tgas Tsolid Tsolid

[m]

Full Temperature Profiles

Smoldering Puffing

Page 10: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

[m] [m]

Smoldering Smoldering Puffing Puffing wO2 wO2 wCO wCO

Mass Fraction Profiles

Page 11: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

11

Char and Volatile-Precursor Density Profiles

Beginning of smolder

End of a 2 [s] puff (2nd puff)

End of 58 [s] smolder

[m]

[kg/m3]

[kg/m3]

Char Density Volatile Density

Middle of smolder

Page 12: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

Experimental and Simulated Solid Temperatures (˚C)

Middle of a 2[s] Puff End of 58 [s] Smolder

Baker, R R, High Temp. Science, 7 (1975) 236-247 12

600

700 750

775 700

750

800

>850

800

600

>900

PBL

PBL

PBL = paper burn line location at start of 3rd Puff

[m] [m]

Porous region Porous

region

Page 13: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

Experimental and Simulated Gas Temperatures (˚C)

300

400

500

700 750

800

>850 600

Middle of a 2[s] Puff End of 58 [s] Smolder

Baker, R R, High Temp. Science, 7 (1975) 236-247 13

750

775

700

600

500

400

PBL

PBL

[m] [m]

Free Flow

Porous region

Porous region

Free Flow

Page 14: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

Experimental and Simulated Oxygen Mass Fraction

Middle of a 2[s] Puff End of 58 [s] Smolder

Baker, R R, Beitr. Tabakforsch, 11, (1981), 1-17

14

0.0

0.02

0.04

0.06

[m] [m]

0.0

0.02 0.04 0.06 0.08 0.10

0.12

0.14

Porous region

Porous region Free

Flow

Free Flow

Page 15: Numerical Simulation of Forward and Static Smoldering ...Numerical Simulation of Forward and Static Smoldering Combustion Outline 1. Introduction 2. Numerical Implementation in COMSOL

15

Conclusions and Directions for Further Work

[m/s]

Cold Flow, Velocity Magnitude

• Simulation for full puffing/smoldering cycle on entire domain has been constructed in 2-D

• Model agrees reasonably well with experimental data

• Discrepancies may be due to unknown sub-model parameters, questionable applicability of sub-models or REV assumption

• Future work could attempt to resolve smaller scales, since separation of scales is questionable

Acknowledgments

• Prof. William H. Green (MIT)

• Dr. Fabrice Schlegel (COMSOL, MIT)

• Dr. Ray Speth

• Philip Morris International for funding