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Frontiers in Spectroscopy. Ohio State University, March 2004. Nonlinear Spectroscopy:. From quantum mechanics to auto-mechanics. Lecture Outline. Lecture 1: Linear and Nonlinear Optics Nonlinear spectroscopic techniques Lasers for nonlinear spectroscopy
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Frontiers in Spectroscopy. Ohio State University, March 2004 Nonlinear Spectroscopy: From quantum mechanics to auto-mechanics Paul Ewart
Lecture Outline • Lecture 1: Linear and Nonlinear Optics Nonlinear spectroscopic techniques Lasers for nonlinear spectroscopy • Lecture 2: Basic theory of wave mixing Coherent signal generation Spectral simulation • Lecture 3: Spectroscopy and diagnostics High resolution spectroscopy Combustion diagnostics
DFWM spectrum of C2 in oxy-acetylene flame Note: High spectral resolution High signal-to-noise in luminous environment
DFWM Spectra of C2 in oxy-acetylene flame • Swan band (0,0) Band head • Corrected line positions • Coherent addition
Multiplex DFWM spectroscopy in flames 1 3 2 • Broad laser spectrum overlaps • molecular resonances • 2. Broadband FWM spectrum • recorded on CCD camera • 3. Theoretical spectrum fitted to • find temperature. • C2 spectrum in oxy-acetylene flame
Multiplex FWM thermometry in flames • Time resolved measurement of temperature by single laser shot of broadband modeless laser • Single shot precision of ~4%
1-D line imaging by FWM Line imaged on Spectrograph slit
Multiplex FWM along a line • Line formed by intersecting planar laser beams • FWM signal is induced by broadband laser • Signal line is mapped onto spectrograph slit • Spatially resolved spectra recorded on CCD camera
Simultaneous measurement of Temperature and Concentration of C2 along a line Spectrum at each position yields temperature T(x) Spectral intensity along line yields concentration
Simultaneous measurement of C2concentration and temperature along 1-D line
Detection of combustion generated NO in s.i.engine using DFWM • BOXCARS plates: • simple, stable, reproducible • alignment of input laser beams. • Collimated beams in interaction • region minimizes noise from • windows etc.
DFWM spectrum of NO in firing s.i. engine (methane/air) Skip fire 1 in 9 Speed 1200 rpm Ignition timing: 40o BTDC Laser timing: BDC Upper trace: NO absorption (line of sight) Lower trace: DFWM spectrum (space resolved)
LITGS in OH in high pressure CH4/air flame Recorded using cw Ar-ion Laser: 1 Watt in ~ 1 ms
Flashlamp pumped dye Laser: 106 Watt in ~ 1 ms
LITGS using long pulse probe NO2:N2 5 bar 300K Temperature precision + 0.1% Pressure precision + 2 %
Simultaneous measurement of Temperature and Pressure along a line using LITGS
Streak image of LITGS signal from line: NO2 in N2 at 2.5 bar 5 mm Position x 0 120 Time nsec Oscillation frequency yields Temperature, T(x) Decay function in time yields Pressure, P(x)
TGV in NO2 seeded air flow • Thermal grating written by two beams at 532 nm • Signal read by delayed pulses at 1064 nm from SLM laser • Forward and Back scattered signals are Doppler shifted up and down in frequency by Dn
Conclusions • Laser Induced Grating techniques: • Temperature CARS • Minor Species, Temperature DFWM • 1-D Concentration and Temp. DFWM • Velocity LITGS • Pressure and Temperature LITGS • 1-D Pressure and Temperature LITGS
Acknowledgements • Karen Bultitude • Rob Stevens • Geraint Lloyd • Radu Bratfalean • Andrew Grant • Duncan Walker • University of Heidelberg PCI • University of Stuttgart, ITV and DLR • EPSRC, British Gas, Rover plc
Potential of LITGS diagnostics • Non-invasive temperature and pressure measurement • Time and space resolved data • Detection of local temperature and pressure • Diagnostics of auto-ignition and engine “knock” Schlieren film of autoignition Courtesy of Prof CWG Sheppard University of Leeds