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EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman, and Albert Ratner Department of Mechanical and Industrial Engineering The University of Iowa June 2014
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EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Dec 17, 2015

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Page 1: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A

LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH

Jianan Zhang, Kelsey Kaufman, and

Albert Ratner

Department of Mechanical and Industrial Engineering

The University of Iowa

June 2014

Page 2: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Outline

Motivation

Combustion Heat Release Measurement

Methods

Experimental System

Results and Discussion

Acknowledgements

Page 3: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Outline

Motivation

Combustion Heat Release Measurement

Methods

Experimental System

Results and Discussion

Acknowledgements

Page 4: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Motivation

In the real system, the flame is highly turbulent and the flame structure is complicated.

Proper measurement of heat release of combustion is critical for understanding the feature of a burner used in the real energy system.

Page 5: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Motivation

The low swirl burner is a newly designed burner that operates under lean regime to ensure low NOx production.

In the real lean combustion system, thermoacoustic instability is a common combustion instability form.

Thermoacoustic instability results from coupling between combustion heat release and pressure oscillation in the system.

Page 6: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Outline

Motivation

Combustion Heat Release Measurement

Methods

Experimental System

Results and Discussion

Acknowledgements

Page 7: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Chemiluminescence Measurement

Chemiluminescence spectra of OH*(508 nm), CH*(431 nm), and C2*(513 nm) in laminar flame (J. Kojima. 2013)

CH+O2 OH*+CO

Chemiluminescence of OH*(508 nm) of a swirling flame

Chemiluminescence results can show the heat release information globally.

It is easy to record with photomultiplier or ICCD camera equipped with filter.

Line of sight method, which has low space resolution and lose the detail information about the flame structure

Page 8: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Planar Laser Induced Fluorescence of OH

PLIF can get cross-section view of the flame, good spatial resolution

Two-dimensional result OH exists in both of the flame front and burnt gas

OH spectrum (Hult, 2005)

PLIF setup

OH PLIF

Page 9: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Combination of OH and CH2O PLIF

CH2O+OH HCO + H2O

Can get local heat release rate accurately

Measurement system is more complicated

Two Dimensional resultImages of OH PLIF and CH2O PLIF(B.O. Ayoola, 2006)

Page 10: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Outline

Motivation

Combustion Heat Release Measurement

Methods

Experimental System

Results and Discussion

Acknowledgements

Page 11: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Experimental System

Low swirl burner: flow divergence for stabilization provided by Dr. Robert Cheng of LBNL

1 inch burner and swirler with low swirl number (0.5)

Flame shapeVelocity vectors and shear stresses (background contours) obtained in R= 2.54 cm LSB. Adapted from Chen [1]

[1] Cheng, Robert K. "Low swirl combustion." DOE Gas Turbine Handbook (2006).

Page 12: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

A: Acoustic Chamber; B: Air compressor; C: Fuel cylinder; D: Premixer; E: Burner; F: Quartz window; G: ICCD camera; H: Signal generator; I: Power amplifier; J: Signal transducer; K:

Signal transducer; L: computer; P: Pressure sensor; S: Speaker; T: Thermocouple

Experimental System

Page 13: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Experimental System

Laser system

Final laser beam with power of 27 mJ/Pulse

Page 14: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Outline

Motivation

Combustion Heat Release Measurement

Methods

Experimental System

Results and Discussion

Acknowledgements

Page 15: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Result (Analytical Method)

∑𝑖=1

𝑛 𝑞′𝑝′

𝑞𝑝𝑟𝑚𝑠

𝒒 ′

𝒑 ′Rayleigh Index map

Rayleigh Index based on Rayleigh Criteria is used in current research.

R =

Instability is damped

Instability is encouraged

Page 16: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Results(Rayleigh Index Map)

Rayleigh Index map of 5 m/s flame with perturbation frequency of 125 Hz

Results with OH-PLIF clearly show the coupling structure and location.

Coupling strength increases with the forcing level and then becomes stable.

Along the flame edge, the coupling trend is also clearly illustrated. Response of Rayleigh Index

Distribution to Perturbation Amplitude

Page 17: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Results(Weighted RRMS)

Original Rayleigh Index Map

The general trend can be divided into two regions, which include a linear and nonlinear region.

The maximum uncertainty is 10.89%

Global RMS Rayleigh Index

Rayleigh Index considering oscillation level

Page 18: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

Acknowledgement

Lawrence Berkeley National Laboratory for

providing the low swirl burner

The University of Iowa for financial support

and facilities

Page 19: EXPERIMENTAL EXAMINATION OF THE THERMOACOUSTIC INSTABILITY OF A LOW SWIRL FLAME WITH PLANAR LASER INDUCED FLUORESCENCE OF OH Jianan Zhang, Kelsey Kaufman,

QUESTIONS?