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Modeling of Strata Gas Liberation into the Mine Drifts with Time-Dependent Ventilation George Danko, Davood Bahrami, and Jon Fox University of Nevada, Reno, Reno, NV Date: February 26, 2013 Location: Denver, CO SME Annual Meeting
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Modeling of Strata Gas Liberation into the Mine Drifts with Time-Dependent Ventilation

George Danko, Davood Bahrami, and Jon Fox University of Nevada, Reno, Reno, NV

Date: February 26, 2013

Location: Denver, CO SME Annual Meeting

Outline

• Introduction • Coupled transient transport processes • Response changes in ventilation to flow

control in a large-scale mine • Response to barometric pressure variation • Conclusions

2

Introduction Coupled transient transport processes

3

TOUGH2, TOUGHREACT, and TOUGH-FLAC domain

Near-field stresses

Opening/closing fractures

Drift cavity

Drift wall

Air, heat, and mass flow

Pw, Tw, Cw

Assume that the air flow is modified according to VOD control: P, Qa change

Fan start, stop, or partial change of RPM: P, Qa change

Air regulator adjustment: P, Qa change

∆Qa modifies concentration ∆P modifies qm, qc, and qh

4

qh(Pa) qm(Pa) qc(Pa) Rock strata flows and transport model:

T(Qa, qm, …), RH(Qa, qm, …), C(Qa, qc, …)

Introduction Coupled transient transport processes

PMC domain

TOUGH2, NUFT for heat and moisture TOUGHREACT for heat, moisture and chemical reaction TOUGH-FLAC for heat, moisture and mechanical (stress) interaction

CFD domain: Fine-scale Integrated-parameter MULTIFLUX or a simple flow and transport numerical model

Air flow

Time dependent 2-D or 3-D sub-models domains for poro-elastic conduction-advection (TOUGH2, TOUGHREACT, or TOUGH-FLAC)

Time-dependent MULTIFLUX Convection-advection-flow and heat transport CFD model in the drift cavity

. . . .

. . . . i

j

k

drift cavity

5

. . . .

. . . . i

j

k

qh, qm, qc

qh, qm, qc

qh, qm, qc

[qh]=[[ht]](Tw-T0)+[[hp]](Pw-P0) +[[hc]](Cw-P0) [qm]=[[mt]](Tw-T0)+[[mp]](Pw-P0) +[[mc]](Cw-P0) [qc]=[[ct]](Tw-T0)+[[cp]](Pw-P0) +[[cc]](Cw-P0) Where, [[ht]], [[hp]], [[hc]], [[ht]], [[mp]], [[mc]], [[ct]], [[cp]], and [[cc]] are system-response NTCF matrices for time-dependent flux exchanges with the rockmass

drift cavity

US Patent: US7610183, 2009 for Numerical Transport Code Funcionalization in MULTIFLUX

Introduction Coupled transient transport processes

Air flow network model

Heat flow network model

Moisture flow network model

Rhtqh ∆

=

Rmqm ω∆

=

RaPbqa ∆

=

( )qaRaRa = NTCF

NTCF NTCF NTCF

NTCF

NTCF

NTCF NTCF

NTCF

NTCF

NTCF NTCF NTCF

NTCF

NTCF

NTCF NTCF

NTCF

Species flow network model

NTCF

NTCF NTCF NTCF

NTCF

NTCF

NTCF NTCF

NTCF

RcCqc ∆

=6

Introduction Coupled transient transport processes in MULTIFLUX

• Twin Joy M84 booster fans are modulated at 1450 level – Variable frequency modeled @ 50%

Real Mine Example Change in Airflow Directions due to Fan RPM Modulation

7

Change in Airway Velocities Due to Fan RPM Modulation

A twin Joy M84 booster fans is modulated at 1450 level Variable frequency control modeled at 50% pressure

Airways where the flow direction reversed

8

Dominantly Affected Airways - Percentage Change in Airflow Rate Start End ΔQab % Δ Previous New Start End ΔQab % Δ Previous New

280 286 -26.622 -101% 26.412 -0.20943 475 478 -6.721 -192% 3.4943 -3.2267 286 296 -26.622 -101% 26.412 -0.20943 1062 1061 -3.9417 -129% 3.0483 -0.89347 411 410 -33.943 -157% 21.575 -12.368 1061 1056 -3.9167 -130% 3.0056 -0.91109 418 411 -33.943 -157% 21.575 -12.368 1056 1057 -3.9167 -130% 3.0056 -0.91109 410 412 -33.943 -157% 21.575 -12.368 1421 1455 -12.983 -592% 2.1931 -10.789 412 415 -33.943 -157% 21.575 -12.368 1342 1209 -11.912 -819% 1.454 -10.458 415 417 -33.943 -157% 21.575 -12.368 1902 1867 -0.22717 -122% 0.18642 -0.04075

1270 1258 -23.28 -147% 15.831 -7.4483 1043 1042 -3.0427 -1676% 0.18154 -2.8611 1280 1270 -23.28 -147% 15.831 -7.4483 1044 1043 -3.0427 -1676% 0.18154 -2.8611 1286 1280 -23.28 -147% 15.831 -7.4483 1046 1044 -3.0427 -1676% 0.18154 -2.8611 1287 1286 -23.28 -147% 15.831 -7.4483 1047 1045 -3.0427 -1676% 0.18154 -2.8611 1288 1287 -23.28 -147% 15.831 -7.4483 1045 1046 -3.0427 -1676% 0.18154 -2.8611 1289 1288 -23.28 -147% 15.831 -7.4483 1051 1047 -3.0427 -1676% 0.18154 -2.8611 1291 1289 -23.28 -147% 15.831 -7.4483 1057 1051 -3.0427 -1676% 0.18154 -2.8611 1197 1196 -23.263 -147% 15.793 -7.4704 658 757 -0.17297 -114% 0.1514 -0.02156 1198 1197 -23.263 -147% 15.793 -7.4704 429 425 0.32736 157% -0.20841 0.11896 1201 1198 -23.263 -147% 15.793 -7.4704 1342 1244 11.912 819% -1.454 10.458 1206 1201 -23.263 -147% 15.793 -7.4704 400 398 4.6321 218% -2.1234 2.5087 1208 1206 -23.263 -147% 15.793 -7.4704 324 226 6.0118 175% -3.4439 2.5678 1248 1208 -23.263 -147% 15.793 -7.4704 226 227 6.0118 175% -3.4439 2.5678 1196 1291 -23.263 -147% 15.793 -7.4704 329 323 6.0118 175% -3.4439 2.5678

811 808 -29.569 -207% 14.304 -15.265 325 324 6.0118 175% -3.4439 2.5678 989 988 -12.632 -138% 9.1362 -3.4963 323 325 6.0118 175% -3.4439 2.5678 991 989 -12.632 -138% 9.1362 -3.4963 332 329 6.0118 175% -3.4439 2.5678

1462 1502 -10.644 -174% 6.1307 -4.5137 336 332 6.0118 175% -3.4439 2.5678 1012 1015 -10.377 -195% 5.3298 -5.0474 1462 1458 10.644 174% -6.1307 4.5137

399 1492 -4.7941 -137% 3.5036 -1.2906 305 277 15.675 179% -8.7679 6.9068

Negative sign in the change means change in air flow direction

Start End Qprevious (kg/s)

Qnew (kg/s)

280 286 26.41 -0.21 1012 1015 5.33 -5.05

399 1492 3.50 -1.29

0

1

2

3

4

5

6

0 100 200 300

Pres

sure

kPa

Flow Rate m3/sec

Joy M84-50-1180

Jair 78301200 -200hp

Jetair_60-26-1170

JAir78-30-1200-200hp

JOY108"-65-1200

Joy M84

0

0.5

1

1.5

2

2.5

3

3.5

0 20 40 60 80

Pres

sure

kPa

Flow Rate m3/sec

Joy 60-26-1170

48-26-1800RPM-Jetair

2-stage48"-30-1800

Joy 1000 54-26-1770

joy 54-26-1170

0 1 2 3 4 5 6 7 8 9

0 100 200 300

Pres

sure

kPa

Flow Rate m^3/sec

54-26-1170

Spendrup-140-80-1760

Robin_700hp_76"fan

Howden Sirocco

0

0.5

1

1.5

2

2.5

3

0 50 100

Pres

sure

kPa

Flow Rate m^3/sec

JOY2000_48-26-1770

Combo 48-150 n 45-10

Combo 54-100 n48-150

54-30-1800RPM-Jetair

Change in Pressure Due to Fan RPM Modulation

9

Change of Dynamic Variations

• Air pressure variations: – Atmospheric pressure (Pb) variation – VOD-related pressure changes caused by variable fan operation – Dynamic airway resistance changes, e.g., door opening or

closing – Blasting operation, underground or surface – Fire/explosion in a different section of the mine

• Flow rate (Qa) variations: – VOD-related pressure difference changes caused by variable fan

operations (booster or main) – Dynamic airway resistance changes, e.g., door opening or

closing.

10

Typical Barometric Pressure, Pb, Variation in Nevada

11

12

Typical Barometric Pressure, Pb, variation in Nevada

Criticality More gas inflow

from strata or gob Less gas dilution by air flow

Summary of changes

13

Pressure, Pb Air flow

(related to ∆P=Pbin-Pbout)

1

2

3

4

Qa

Pb

Qa

Pb

Pb

Pb Qa

Qa

Pb Qa

Example Application

Model input • Flow cross section, A: 23m2

• Flow wetted perimeter, Per: 19m • Rockmass porosity: 15% • Rockmass liquid saturation: 0 • Rockmass permeability: 2.4x10-12 m2

(~2.4 Darcy) • Far-field barometric pressure: 87.3 Kpa • In-drift barometric pressure: 87 KPa

Gas flow toward drift airway

100m thick rockmass around the drift

Fixed pressure boundary at 87.3 KPa

87 Kpa

14

Initial rate changing with time

NTCF model Preparation

0 500 1000 1500 2000 2500 3000 3500 4000-2

-1.5

-1

-0.5

0

0.5

1

1.5

2x 10

-5

Time ( Sec )

Stra

ta G

as li

bera

tion

Rat

e ( k

g/s-

m2

)

drift pressure: Pb-1000 Padrift pressure: Pb+1000 Pa

0

10

20

30

0

10

20

30-6

-4

-2

0

2

4

6

x 10-9

0 500 1000 1500 2000 2500 3000 3500 40000

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

2x 10

-5

Time (sec)

Gas

Lib

erat

ion

Rat

e (k

g/s-

m2 )

NUFTNTCF

1000 Pa or -1000 Pa step change in drift air pressure

NUFT

NTCF verification

15

NTCF code was used with a cylindrical mesh around the opening. A 1-hr transient model was prepared in 2-min ∆t.

NTCF matrix, [[CC (NxN)]] where N=30

Gas Liberation and Concentration Example Darcy, background gas flow

16

0 10 20 30 40 50 60-1

-0.5

0

0.5

1

1.5

Time (minute)

Gas

Lib

erat

ion

Flux

(kg/

s)

0200

400600

8001000

0

20

40

600

0.1

0.2

0.3

0.4

Distance (m)Time (minute)

Gas

Con

cent

ratio

n (%

)

Gas concentration variation in time at 1000m distance. Steady state gas flow

Gas concentration variation in time and space due to 87kPa in-drift air pressure. V= 1 m/s

qm

Gas Liberation and Concentration Example 1000 Pa in-drift pressure change

17

Gas concentration variation in time for Darcy flow condition 1000m drift section, 86 kPa in-drift air pressure.

0 10 20 30 40 50 600.2

0.4

0.6

0.8

1

1.2

1.4

1.6

Time (minute)

Gas

Lib

erat

ion

Flux

(kg/

s)

0 10 20 30 40 50 6085

85.2

85.4

85.6

85.8

86

86.2

86.4

86.6

86.8

87

Time (minute)

Bar

omet

ric P

ress

ure

(kP

a)

Sudden drop (∆Pb) in pressure

qm

18

0200

400600

8001000

0

20

40

600

0.5

1

1.5

2

2.5

3

Distance (m)Time (minute)G

as C

once

ntra

tion

(%)

Gas concentration variation in time at 1000m distance. V=1 m/s

Gas concentration variation in time and space due to 86kPa in-drift air pressure.

Gas Liberation and Concentration Example 1000 Pa in-drift pressure change

C%

0 10 20 30 40 50 600

0.5

1

1.5

2

2.5

3

Time (minute)

Gas

Con

cent

ratio

n (%

)

C% Initial

19

0 10 20 30 40 50 6085.5

86

86.5

87

Time (minute)

Bar

omet

ric P

ress

ure

(kP

a)

0 10 20 30 40 50 60-0.2

0

0.2

0.4

0.6

0.8

1

1.2

Time (minute)

Gas

Lib

erat

ion

Flux

(kg/

s)

Gas Liberation and Concentration Example Variable in-drift pressure, and lowered air flow velocity from 5 to 1 m/s

Initial Pbar

qm Pb

20

0 10 20 30 40 50 600

0.5

1

1.5

2

2.5

3

3.5

Time (minute)

Gas

Con

cent

ratio

n (%

)

0

200

400

600

800

1000

010

2030

4050

60-1

0

1

2

3

4

Distance (m)Time (minute)

Gas

Con

cent

ratio

n (%

)

Gas concentration variation in time at 1000m distance. V=1 m/s.

Gas concentration variation in time and space due to variable in-drift air pressure.

Gas Liberation and Concentration Example Variable in-drift pressure

C%

C% Initial

21

Gas Liberation and Concentration Example Variable in-drift pressure

0 10 20 30 40 50 6086.5

86.6

86.7

86.8

86.9

87

87.1

87.2

87.3

87.4

87.5

Time (minute)

Bar

omet

ric P

ress

ure

(kP

a)

0 10 20 30 40 50 600

0.05

0.1

0.15

0.2

0.25

0.3

0.35

0.4

0.45

0.5

Time (minute)

Gas

Lib

erat

ion

Flux

(kg/

s)

qm Pb

Initial Pbar

22

Gas concentration variation in time at 1000m distance. V=1 m/s • We cannot say with confidence that a time-

averaged solution is safely equivalent with the short-time-averaged of a transient

0 10 20 30 40 50 600

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

Time (minute)

Gas

Con

cent

ratio

n (%

)

0

500

1000

01020304050600

0.2

0.4

0.6

0.8

1

Distance (m)

Time (minute)

Gas

Con

cent

ratio

n (%

)

Gas concentration variation in time and space due to variable in-drift air pressure.

Steady state, from Darcy gas flow

Gas liberation and concentration example Variable in-drift pressure

C%

Conclusions

23

Acknowledgement

24

Thank You

Questions?

25

support

• 30 CFR § 77.201-2 Methane accumulations; change in ventilation. If, at any time, the air in any structure, enclosure or other facility contains 1.0 volume per centum or more of methane changes or adjustments in the ventilation of such installation shall be made at once so that the air shall contain less than 1.0 volume per centum of methane.

26

support • 30 CFR § 75.323

Actions for excessive methane. (a)Location of tests. Tests for methane concentrations under this section shall be made at least 12 inches from the roof, face, ribs, and floor. (b)Working places and intake air courses. (1) When 1.0 percent or more methane is present in a working place or an intake air course, including an air course in which a belt conveyor is located, or in an area where mechanized mining equipment is being installed or removed-- (i) Except intrinsically safe atmospheric monitoring systems (AMS), electrically powered equipment in the affected area shall be deenergized, and other mechanized equipment shall be shut off; (ii) Changes or adjustments shall be made at once to the ventilation system to reduce the concentration of methane to less than 1.0 percent; and (iii) No other work shall be permitted in the affected area until the methane concentration is less than 1.0 percent. (2) When 1.5 percent or more methane is present in a working place or an intake air course, including an air course in which a belt conveyor is located, or in an area where mechanized mining equipment is being installed or removed-- (i) Everyone except those persons referred to in §104(c) of the Act shall be withdrawn from the affected area; and (ii) Except for intrinsically safe AMS, electrically powered equipment in the affected area shall be disconnected at the power source. (c)Return air split. (1) When 1.0 percent or more methane is present in a return air split between the last working place on a working section and where that split of air meets another split of air, or the location at which the split is used to ventilate seals or worked-out areas changes or adjustments shall be made at once to the ventilation system to reduce the concentration of methane in the return air to less than 1.0 percent.

27

support • 30 CFR § 75.323

Actions for excessive methane. (2) When 1.5 percent or more methane is present in a return air split between the last working place on a working section and where that split of air meets another split of air, or the location where the split is used to ventilate seals or worked-out areas-- (i) Everyone except those persons referred to in §104(c) of the Act shall be withdrawn from the affected area; (ii) Other than intrinsically safe AMS, equipment in the affected area shall be deenergized, electric power shall be disconnected at the power source, and other mechanized equipment shall be shut off; and (iii) No other work shall be permitted in the affected area until the methane concentration in the return air is less than 1.0 percent.

• (d)Return air split alternative. (1) The provisions of this paragraph apply if-- (i) The quantity of air in the split ventilating the active workings is at least 27,000 cubic feet per minute in the last open crosscut or the quantity specified in the approved ventilation plan, whichever is greater; (ii) The methane content of the air in the split is continuously monitored during mining operations by an AMS that gives a visual and audible signal on the working section when the methane in the return air reaches 1.5 percent, and the methane content is monitored as specified in §75.351; and (iii) Rock dust is continuously applied with a mechanical duster to the return air course during coal production at a location in the air course immediately outby the most inby monitoring point. (2) When 1.5 percent or more methane is present in a return air split between a point in the return opposite the section loading point and where that split of air meets another split of air or where the split of air is used to ventilate seals or worked-out areas-- (i) Changes or adjustments shall be made at once to the ventilation system to reduce the concentration of methane in the return air below 1.5 percent; (ii) Everyone except those persons referred to in §104(c) of the Act shall be withdrawn from the affected area; (iii) Except for intrinsically safe AMS, equipment in the affected area shall be deenergized, electric power shall be disconnected at the power source, and other mechanized equipment shall be shut off; and (iv) No other work shall be permitted in the affected area until the methane concentration in the return air is less than 1.5 percent. (e)Bleeders and other return air courses. The concentration of methane in a bleeder split of air immediately before the air in the split joins another split of air, or in a return air course other than as described in paragraphs (c) and (d) of this section, shall not exceed 2.0 percent.

28


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