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Laser Induced Fluorescence – LIF/PLIF

It is a powerful diagnostic tool for the investigation of nonreacting as well as reacting gas and liquid flows.

LaVision was founded in 1989 as a spin-off from Max Planck Institute and Laser Laboratory in Goettingen, Germany.

LaVision offers standard and dedicated customer designed Laser Imaging Systems for reactive and non-reactive flow field analysis and fluid mechanics applications, Intelligent Imaging Systems for non-destructive material testing, a range of high-performance cameras (CCDs and intensified CCDs) and smart optical sensor systems.

The LaVision team has extensive professional experience in Laser Imaging Spectroscopy and optical techniques such as Laser Induced Fluorescence (LIF), Absorption and Emission Spectroscopy, Raman, Rayleigh and Mie Scattering, Particle Image Velocimetry (PIV), Spray Analysis, Digital Image Correlation (DIC) techniques as well as ultra-fast time-resolved imaging and high-speed image recording.


Planar Laser Induced Fluorescence (PLIF = LIF Imaging) is a very sensitive laser imaging technique for species concentration, mixture fraction and temperature measurements in fluid mechanical processes, sprays and combustion systems. 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).


Imaging of flame structure (also in 3D) of excited flame species

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.



High-speed OH-LIF imaging

LIF Imaging Setup:

A laser beam is formed to a light sheet (or volume) and intersects the fluid area of interest, e.g. in flames, sprays or thermal flows. The resulting fluorescence light from excited molecules in the light sheet is imaged through a selective filter onto a time-gated digital camera. For pulsed UV LIF applications usually an image intensifier amplifies the LIF signal. The conversion of LIF images into meaningful concentration or temperature fields is based on calibration measurements.


LIF Advantages:

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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