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Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION WORKING GROUP MEETING November 1-2, 2005 Atlantic City, New Jersey USA

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Page 1: Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION

Fuel Tank Protection Research at NASA GRC

Clarence T. ChangNASA Glenn Research Center

Cleveland, Ohio 44135USA

INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION WORKING GROUP MEETING

November 1-2, 2005Atlantic City, New Jersey

USA

Page 2: Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION

Adaptive OBIGGS

Inert gas

Inert gasgeneration

Ullageignitionmodel

Ullageflammability

sensors

O2 sensor

Correctiveresponses Ignitable

fuel tankullage

mixture

Detonationtransition

Ignitionsources

Fuel tankconstraints

The Problem

CTC 9-15-2005

Outside air

No ignition

Ullage detonation

Tank over-pressure

Limitedignition

MostlyFATALMay be

survivable

SurvivableDamage

NoProblem

AlwaysFATAL

The OutcomesThe Inputs

Fuel

Page 3: Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION

Fuel Modification Reduces Ignition Overpressure

0

25

50

75

100

125

150

175

200

-10 0 10 20 30 40 50 60

Temperature/ oC

Vap

or P

ress

ure/

mm

Hg

iso-Octane (2,2,4-trimethyl Pentane)2,2,3-trimethyl Pentane2,2,3,3-tetramethyl Butanen-Octanen-Heptane

Isomeric forms of Octane

MIE = 1.5 mJ

MIE = 0.25 mJ

n-Octane

iso-Octane

MTBE

Linear Species (n-Octane) Form Reactive Ethylene While Branched Species (iso-Octane, MTBE) Form Reaction Quenching Isobutylene

Vapor Pressure Increases With Branching

Ignition Energy Increases with Branching

Energy Density Increases with Branching

Vapor Phase iso-Octane Concentration is 3 Times That of n-Octane at 40oC, MIE is a Factor of 6 Higher

Substitution of Branched for Linear Alkanes Reduces Pressure Impulse Thus Reducing Structural Failure

Branched Alkanes Increase Ignition Delay That Decreases Reaction Rates and Leads to Flame Extinction

Combustion Pressure Impulse

0

1000

2000

3000

4000

5000

6000

7000

0 500 1000 1500 2000 2500 3000 3500 4000

Time (ms)

dP/d

T (A

tm/s)

Linear AlkanesBranched Alkanes

Page 4: Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION

Ignition Sensitization: Minimum Ignition Energy Dependent on Spark Duration!

n-Octane MIE vs. Spark Duration

10-1

100

101

102

103

100 101 102 103 104

Spark Duration, μs

Sp

ark

En

erg

y ,

mJ

n-Octane, 35.9 ºC, Φ =2

n-Octane, 18.3 ºC, Φ =1

n-Octane, 17 ºC, Φ =0.95

n-Octane, 19.8 ºC, Φ =1.06

n-Octane, 19.8 ºC (no spark)

Page 5: Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION

Fuel tank Protection -Deflagration-to-Detonation Transition

1. Ignition in compartment A results in constant-volume combustion2. Constant volume combustion results in over-pressure in A maximum 8x3. Pressurized gas jets into compartment B at sonic speed.4. Jet poses 4-10 order of magnitude stronger ignition energy than the MIE5. Jet ignites ullage gas in B, transition from deflagration to detonation wave.

Some deflagration over-pressure may be survivable.Detonation is not survivable.

AC B

Ullage gas

Liquid fuel at bottom

UnspecifiedIgnition Source

DeflagrationDetonation

Page 6: Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION

Improved Inert-Gas Recovery from Combustion Derived Inerting

Φ = 0.70 Dry Combustion Products and Air at 150 ºF and 180 ºF at 40 psig

80

82

84

86

88

90

92

94

96

98

100

0 10 20 30 40 50 60 70 80 90 100

Inert-Gas Recovery Fraction, %

Iner

t-G

as P

uri

ty, %

  CDI, Φ = 0.70,

N2+CO2

  CDI, Φ = 0.70,

N2 only

  ASM, N2 only

180 ºF150 ºF 

1/3 More N2 Recovery or ¼ less Bleed Air Needed

Page 7: Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION

In-Tank Real-Time Multi-Species Fiber Optic Flammability Sensor

• Real-Time: 5 second update interval for feedback control, and critical time-dependent process monitoring

• Multi-Species Analysis: N2, O2, CO2, H2O, CO, CH4, other HC’s, H2, H2S, NO, SO2,…

• Precise: currently has 1% precision in 5 seconds for N2; future versions will require < 1 second for same precision

• Rugged and Reliable: system has no moving parts to go out of alignment or consumables to wear out

• Intrinsically-Safe: No electrical penetration into measurement volume

• Cost-Effective: Monitor multiple locations simultaneously with multiple fiber sensors and one base unit

0

0.05

0.10

0.15

0.20

0.25

30 60 90 120 150 180 210 240 270 3000

0.2

0.4

0.6

0.8

H2O

CO2

O2

N2

Time (seconds)

O2

, C

O2

, H

2O

[M

ole

Fra

ctio

n]

N2

[M

ole

Fra

ctio

n]

Real-Time FiberOptic Gas Analyzer

Gas Inlet

Gas Outlet

Respiration Gas Monitoring Example

Low-VolumeGas SamplingChamber(or Fuel Tank Ullage)

Advantages

Fiber OpticSensor Probe

Page 8: Fuel Tank Protection Research at NASA GRC Clarence T. Chang NASA Glenn Research Center Cleveland, Ohio 44135 USA INTERNATIONAL AIRCRAFT SYSTEMS FIRE PROTECTION

Contact Information at NASA Glenn Research Center

CDI-OBIGGS & Ignition MitigationClarence Chang, Ph.D.

[email protected]

Deflagration-to-Detonation Transition ScienceNan-Suey Liu, Dr.-Ing.

[email protected]

In-Tank Real-Time Flammability SensorQuang-Viet Nguyen, Ph.D.

[email protected]

Fuel & Ignition ScienceMarty Rabinowitz, Ph.D.

[email protected]