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Stanford University Thermosciences Flow Reactor Study of Controlled Combustion Kinetics GCEP Global Climate and Energy Project C. T. Bowman K. Walters Mechanical Engineering Department

Flow Reactor Study of Controlled Combustion Kinetics GCEP Global

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Page 1: Flow Reactor Study of Controlled Combustion Kinetics GCEP Global

Stanford University Thermosciences

Flow Reactor Study of Controlled Combustion Kinetics

GCEP Global Climate and Energy Project

C. T. BowmanK. Walters

Mechanical EngineeringDepartment

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Stanford University Thermosciences

Outline

• Background

- Motivation

- Objectives

• Approach

• Experimental Setup

• Results

• Future work

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Stanford University Thermosciences

Why Controlled Combustion?

• In conventional combustion devices, the chemical conversion offuel and oxidizer to products occurs rapidly in an uncontrolledand highly irreversible process (flame) and prior to work extraction,leading to a loss in cycle efficiency.

10

20

30

40

50

0 5 10 15 20 25Cycle Pressure Ratio

y

Second Law Cycle Efficiency - %

Fuel Exergy Loss in Combustion - %

Simple Brayton Cycle

T04 = 1200K

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Stanford University Thermosciences

Why Controlled Combustion?

• Modification of work producing cycles to match work extractionand heat release rates can lead to increased cycle efficiencyand, hence, reduced greenhouse gas emissions.

Cycle OPR nth Gain

Simple 20 41.2%

Reheat 92.6 48.0%13.8%

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Stanford University Thermosciences

What is Controlled Combustion?

• In controlled combustion, the rateof the fuel conversion process isvaried by imposing prescribedconditions (temperature and massfractions of the oxidizer/diluents),leading to potential reductions inirreversibilities in energy conversion(improved efficiency) and reducedemissions of pollutants andgreenhouse gases.

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Stanford University Thermosciences

Controlled Combustion

The Challenge to Implementation:

• A new regime of combustion that is poorly understood at thefundamental level needed for design optimization, especiallyfor high-pressure combustion systems, such as gas turbinesand diesel engines (HCCI).

The Objective of this Study:

• To investigate the combustion mechanisms of fuels in theintermediate preheat temperature range (1000-1300K) forpressures up to 50 bar with dilution by inert and chemicallyactive species.

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Stanford University Thermosciences

Controlled Combustion – Expected Outcomes

• Understanding of the effects of inert and chemically activeadditives on combustion rates at intermediate temperaturesand high pressures.

• Detailed and reduced mechanisms for controlled flamelessoxidation of model fuels for use in modeling and designinglow-irreversibility combustion engines, including HCCI andmulti-stage turbine burners.

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Stanford University Thermosciences

Range of Conditions Investigated

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Stanford University Thermosciences

Approach

• Flow Reactor Experiments– Measure the spatial evolution of temperature and composition– Experimental parameters:

• Temperature• Pressure• Oxygen concentration• Fuel concentration• Fuel composition: C2H6, C2H6/CH4 mixtures, surrogates, and

oxygenated fuels• Bath gas composition

• Compare the experimental data to the model results using adetailed reaction mechanism

• Optimize and validate the reaction mechanism• Model reduction by principal component analysis

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Stanford University Thermosciences

High-Pressure Flow Reactor

Gas Analyzers

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Stanford University Thermosciences

High-Pressure Flow Reactor

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Stanford University Thermosciences

Modeling Approach

• Initial studies have been conducted using CH4, C2H6and CH4-C2H6 mixtures to simulate natural gas.

• The starting reaction mechanism is GRI-Mech 3.0.

• The Chemkin and Senkin computer codes are used tomodel the reaction progress and to conduct sensitivityand reaction path analysis.

• Future studies will focus on surrogate andoxygenated fuels.

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Stanford University Thermosciences

1500 ppm C2H6: 0.5% O2

P = 1 bar

Experimental and Model Results

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Stanford University Thermosciences

1500 ppm C2H6: 3.0% O2

T0 = 1170K P = 1 bar

Experimental and Model Results

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Stanford University Thermosciences

Sensitivity Analysis Results

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Stanford University Thermosciences

1050 ppm C2H6: 0.5% O2

T0 = 1250K P = 2 bar

Experimental and Model Results

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Stanford University Thermosciences

Sensitivity Analysis Results

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Stanford University Thermosciences

Sensitivity Analysis Results

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Experimental and Model Results

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Stanford University Thermosciences

Conclusions

• Combustion times can be varied from 10 ms – 100 msec by varying initial O2concentration and diluents.

• For the fuels considered, combustion times increase with increasing pressure.

• Existing detailed reaction mechanisms capture some of the featuresof combustion of methane and ethane in the controlled combustionregime.

• The model consistently under predicts the initial rate of CO formation.

• In the controlled combustion regime, RO2 chemistry becomes increasingly important as the initial O2 concentration decreases and pressure increases.

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Stanford University Thermosciences

Future Work

• Additional experiments– Vary fuel composition and concentration– Vary O2 concentration– Vary pressure

• Measurements of stable intermediates– Aldehydes (CH2O, CH3CHO)– Alcohols (CH3OH, C2H5OH, C3H3OH )

• Update the mechanism• Mechanism reduction