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Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jerse Piscataway, New Jersey Steven Summer Federal Aviation Administration Atlantic City Airport, New Jersey

Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

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Page 1: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Modeling Wing Tank Flammability

Dhaval D. Dadia

Dr. Tobias RossmannRutgers, The State University of New JerseyPiscataway, New Jersey

Steven SummerFederal Aviation Administration

Atlantic City Airport, New Jersey

Page 2: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Motivation

Numerous accounts of wing tank explosions across the world

Current flammability models are for center wing tanks

The proposed regulation for wing tank safety are mostly based on center wing tank models

Models will predict ullage concentrations existing during typical ground and flight operations

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Page 3: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Current Work

Flammable mixtures can be achieved in the wing tank

Experiments are being conducted to build flammability models for wing tanks

Current work involves Predicting the influence of the surrounding temperatures on the

characteristic fuel surface temperature Creating a model that will predict flammability in wing tanks

using heat transfer correlations

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Page 4: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Overview

Single Thermocouple Method (STM)

Difference between Center Wing Tank and Wing Tank

Center Wing Tank Flammability Model

Heat and Mass Transfer Correlations

Experimental Results

Computational Results

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Page 5: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Distillation Curve Jet fuel is a mixture of many different

hydrocarbons

Fuel composition is characterized by the number of alkane reference hydrocarbons

The approach reduces the number of components from over 300 down to 16 species (C5-C20 alkanes)

Liquid compositions of different JP-8 samples with varying flashpoints are presented in terms of the mole fractions of C5-C20 alkanes

ASTM D2887 Distillation Curve

100

150

200

250

300

350

400

450

500

550

600

0.0 0.2 0.4 0.6 0.8 1.0

Fraction Distilled

Tem

per

atu

re D

eg F

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Page 6: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Single Thermocouple Method

Uses Fuel Air Ratio (FAR) calculator by Ivor Thomas

Calculates fuel air ratio over a range of altitudes and temperatures

All compounds with same carbon number were assigned together

Fuel is segregated based on boiling points of alkane species respective of their carbon number

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Page 7: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Single Thermocouple Method

At constant temperature the THC increases as the pressure decreases

Polynomial correlation between Scaled THC and temperature

Film temperature is calculated at a given pressure and THC

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Page 8: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Center Wing Tank (CWT)

The CWT has thin layer of fuel at the bottom of the tank

30% Mass Loading

The tank is heated from the bottom due to heat released from underneath the tank

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Page 9: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Wing Tank (WT)

The WT is mostly filled with fuel

80 % Mass Loading

The tank is heated from the top from an ambient heat source such as the Sun

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Page 10: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Sorting Data

The data is sorted because of the difference in the driving force

The data is sorted into Ascending Profile

The top surface is hotter than the fuel surface

The ullage temperature governs the film temperature

Descending Profile The fuel is hotter than the top

surface The fuel temperature governs the

film temperature

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Page 11: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Correlations

Ascending profile

Correlations between ullage temperature and fuel temperature

Ullage temperature is greater than liquid fuel temperature

Correlation coefficient 0.89

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Page 12: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Correlations

Ascending profile

Correlating ullage temperature with film temperature

Liquid fuel temperature is greater than ullage temperature

Correlation coefficient 0.976

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Page 13: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Correlations

Descending profile

Correlations between ullage temperature and fuel temperature

Ullage temperature is greater than liquid fuel temperature

Correlation coefficient 0.41

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Page 14: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Correlations

Descending profile

Correlations between ullage temperature and fuel temperature

Liquid fuel temperature is greater than ullage temperature

Correlation coefficient 0.93

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Page 15: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Summary of STM

Correlation works best when: Liquid fuel temperature is larger than the

ullage temperature Fuel temperature is the driving force

During Ascending pressure profile Vapor pressure remains constant

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Page 16: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Base Model

Current CWT Model (Polymeropoulos 2004)*

Natural convection flow field between the heated floor and the unheated ceiling and sidewalls

Ullage gases are well mixed due to natural convection and mass transfer

Liquid vaporization Vapor Condensation

Natural convection flow is in the turbulent regime

* JET A VAPORIZATION IN A SIMULATED AIRCRAFT FUEL TANK, Polymeropoulos and Ochs 2004

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Page 17: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Principal Assumptions

Well mixed gas and liquid phases Buoyancy induced mixing

Quasi-steady transport using heat transfer correlations

The analogy between heat and mass transfer for estimating film coefficients for heat and mass transfer

The liquid fuel and wall temperatures are known from experiments

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Page 18: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Computational Method

Inputs The tank geometry Fuel loading Liquid fuel composition Tank pressure Liquid fuel, and tank wall temperatures as functions of time

Computes Equilibrium species concentrations of Jet A in a uniform

temperature, constant pressure tank Temporal variation of vapor temperature and species

concentration

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Page 19: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

CWT Model

Simulation using center wing tank flight test data

The calculated THC is in good agreement with the measured THC

0

0.5

1

1.5

2

2.5

3

0 2000 4000 6000 8000 10000 12000

Time, Seconds

% P

ropa

ne E

quiv

alen

t

Measured THCCalculated THC, 115 FPCalculated THC, 120 FP

FID Error

*Vaporization of JP-8 Jet Fuel in a Simulated Aircraft Fuel Tank under varying ambient conditions –

Ochs 2006

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Page 20: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

CWT Correlations

Heat & Mass Transfer Correlations Horizontal surface:

Top surface: Lower surface of cooled plate

Top of Fuel Layer: Upper Surface of heated plate

Vertical Surface: Laminar Forced Convection on a flat

plate

Horizontal Surface

Vertical Surfaces

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Page 21: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Difference in Model Correlations

The CWT model differs from the WT model in the ascending and cruise conditions due to: Percent load Ullage height Heat and mass transfer correlations Heat source Surface being heated

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Page 22: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Experiments

Experiments were conducted

For 60% and 80% mass loadings

For equilibrium temperatures from 80°F to 100°F

For cruising altitudes of 25000 feet and 34000 feet

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Page 23: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Experimental Equipment

Experiments conducted in an altitude chamber

Designed to simulate temperature and pressure similar to a flight profile Can simulate altitudes from sea

level to 100,000 feet Can simulate temperatures from

-100˚F to +250˚F

NDIR gas analyzer used to measure the total hydrocarbon concentration

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Page 24: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Experimental Setup

An aluminum fuel tank of dimensions 24”w x 24” d x 36” h was used

Access panels on top for thermocouple penetration, ullage sampling, vent, and the fill tube

Thermocouples measured surface, ullage, fuel surface and bulk fuel temperatures

The vent was equipped with a mass flow meter

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Page 25: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Flight Profile

The following flight profile will be used in the altitude chamber

Cruise at 35000 feet

Total flight time is 2.5 hours

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Page 26: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Combination of Models

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Simulation using flight test data

Using wing tank dimensions on a CWT flammability model

Shows that the CWT model works for wing tanks in descending pressure profiles

Page 27: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Wing Tank Correlations

Heat & Mass Transfer correlations Horizontal surface: (Ascending)

Top surface: Laminar Forced Convection on a flat plate

Top of Fuel Layer: Laminar Forced Convection on a flat plate

Horizontal Surface (Cruise and Descending)

Top surface: Turbulent Forced Convection on a flat plate

Top of Fuel Layer: Laminar Forced Convection on a flat plate

Vertical Surface: Laminar Forced Convection on a flat

plate

Horizontal Surface

Vertical Surface

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Page 28: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Test Results

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Ascending Top Surface Heat Transfer Correlations

Page 29: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Test Results

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Cruise and Descending Top Surface Heat Transfer Correlations

Page 30: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Summary of Experimental Results

Laminar Forced Convection during ascent

Turbulent Forced Convection the rest of the flight

Shows ullage gases are well mixed in the ullage

High Reynolds number in the heat transfer cells in the ullage

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Page 31: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Conclusion

Single Thermocouple method can calculate THC using data from a single thermocouple in the tank

The differences between the WT model and the CWT model: Percent Load Ullage Height Heat and mass transfer correlations Heat Source Surface being heated

The CWT model cannot be applied in the ascending and cruise profiles, but can be applied in the descending profiles

Experiments will be conducted To confirm the state of the ullage To compare computed data to experimental data

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Page 32: Modeling Wing Tank Flammability Dhaval D. Dadia Dr. Tobias Rossmann Rutgers, The State University of New Jersey Piscataway, New Jersey Steven Summer Federal

Questions?

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