LIF imaging is a molecule specific visualization method with high spatial and temporal resolution. If the fluid itself contains no LIF-active species (like N2, CH4 or water), flow seeding with fluorescent markers (tracers) is used for scalar flow field imaging (Tracer-LIF).Laser imaging applications in fluid dynamics are numerous and cover high resolution imaging in microfluidics to large scale flow visualization in wind tunnels, fluid mixing and thermometry as well as the validation of CFD models.
For scalar laser imaging in fluids, Laser Induced Fluorescence (LIF) is the very sensitive, versatile and practical measurement technique featuring high signal levels and spectral selectivity. This technique is used across multiple LaVision’s imaging systems (i.e. FlameMaster (system measuring flames), FluidMaster (system measuring fluid).
LIF Principle LIF is a two step process: absorption of a laser photon followed by emission of a fluorescence photon from the excited state. For absorption the laser wavelength λL must match an allowed energy transition of the LIF-active molecule (atom).
Only a fraction ΦLIF of these excited molecules fluoresces, the rest relaxes without light emission. An optical filter selects the usually red-shifted fluorescence light at the emission wavelength λLIF. Only the fraction η of all emitted LIF-photons is detected and converted to the camera signal SF.
LIF IMAGING SETUP
LIF imaging monitors in-situ the process of fluid mixing on micro and macro scales with high spatio-temporal resolution. 1-color LIF imaging as well as 2-color LIF ratio imaging are applied in LaVision’s FluidMaster systems for scalar flow imaging.
For scalar flow imaging the ratiometric 2-color LIF method is best practice, because its LIF signal ratio is independent of local laser energy and tracer concentration variations and laser beam absorption effects, thus leaving the LIF signal ratio only dependent of the measured flow parameter.
TOMO IN FLUID IMAGING
The turbulent flow field of a liquid jet is 3D in nature and requires for a complete understanding a 3D imaging approach, for time-resolved measurements a 4D imaging technique.
Volumetric flame imaging based on tomographic reconstruction gives insights into the complex 3D-distribution of flame species. While multi-cameras are used in parallel to reconstruct the instantaneous 3D flame structure, time-averaged 3D flame imaging is possible with only one camera collecting consecutively the (laser induced) flame emission from multiple views.
TUNABLE LIF IMAGING SYSTEM
Laser imaging in engines investigates all stages of internal combustion engines (i.e. charge motion, in-cylinder laser imaging, mixture preparation, fuel injection, pre-combustion, etc)
For all laser imaging applications a pulsed multi-wavelength Nd:YAG laser is the standard light source. Upgraded with a T-YAG module (intra-cavity etalon) the laser also allows OH-LIF imaging. Only by changing the emission filter in front of the camera the desired in-cylinder process can be investigated. The crank angle resolved measurements are synchronized with the encoder signal of the engine supporting all engine operation modes such as cold start, skip-fired and acceleration modes.
Laser Imaging enables instantaneous detection for important species in reaction kinetics like CH & OH, and is able to resolve the distribution of prominent pollutants like NO.
Structured Laser Illumination Planar Imaging (SLIPI) reduces multiple light scattering applying laser imaging in dense sprays.
SLIPI is based on spatially modulated laser light sheets for Mie or LIF imaging.
While multiply scattered light loses the modulation information, it is maintained for singly scattered light. When the stripe-like phase shifted images are combined correctly, the resulting SLIPI image shows higher image contrast and reveals inner spray structures, which are hidden when using conventional planar laser imaging.
LIF is a technique with high selectivity. It is possible to selectively address species to emit light even in combustion environments where hundreds of different species are present. For small, typically diatomic molecules single quantum states can be detected which allow to determine gas temperatures even under non-equilibrium conditions.
Due to the spectral shift of the LIF emission unwanted interferences from stray light or Mie scattering can be effectively suppressed.
LIF imaging is particularly attractive due to the strength of the resonant absorption process compared with the non-resonant Rayleigh and Raman techniques Due to this sensitivity, techniques like LIF has the capability to detect flame radicals and other species at the ppm or even sub-ppm level. Sensitivity and selectivity are the two main advantages of the LIF technique.
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