Schlieren

Schlieren (from German; singular "schliere") are optical inhomogeneities in transparent material not visible to the human eye. Schlieren physics developed out of the need to produce high-quality lenses void of these inhomogeneities. These inhomogeneities are localized differences in optical path length that cause light deviation. This light deviation is converted to shadow in a schlieren system.

History

Schlieren were first observed by Robert HookeHooke, R., "Of a New Property in the Air," "Micrographia", Observation LVIII,217-219, London(1665).] in 1665 using a large convex lens and two candles. One candle served as a light source. The warm air rising from the second candle provided the schliere.The conventional schlieren system is credited mostly to German physicist August Toepler. Toepler's original system Toepler, A., "Beobachtungen nach einer neuen optischen Methode", Maximillan Cohen und Sohn, Bonn (1864).] was designed to detect schlieren in glass used to make lenses. In the conventional schlieren system Rienitz, J., "Schlieren Experiments 300 years ago," Nature [London] 254, 293-295 (March 27, 1975).] , a point source is used to illuminate the test section containing the schliere. An image of this light is formed using a converging lens (also called a schlieren lens). This image is located at the conjugate distance to the lens according to the thin lens equation:$frac\{1\}\{f\}=frac\{1\}\{d\_o\}+frac\{1\}\{d\_i\}$where $f$ is the focal length of the lens, $d\_o$ is the distance from the object to the lens and $d\_i$ is the distance from the image of the object to the lens. A knife edge at the point source-image location is positioned as to partially block some light from reaching the viewing screen. The illumination of the image is reduced uniformly. A second lens is used to image the test section to the viewing screen. The viewing screen is located a conjugate distance from the plane of the schliere.

Schlieren Flow Visualization

Schlieren flow visualization is based on the deflection of light by a refractive index gradient. The index gradient is directly related to flow density gradient. The deflected light is compared to undeflected light at a viewing screen. The undisturbed light is partially blocked by a knife edge. The light that is deflected toward or away from the knife edge produces a shadow pattern depending upon whether it was previously blocked or unblocked. This shadow pattern is a light-intensity representation of the expansions (low density regions) and compressions (high density regions) which characterize flow.

See also

* Mach-Zehnder interferometer
* Schlieren photography
* Shadowgraph
* Background Oriented Schlieren technique

References

External links

* [http://www.ingentaconnect.com/content/els/00457906/2000/00000026/00000001/art00023 Non-intrusive optical diagnostic experiments for high-speed flow generator flowfield characterization]
* [http://www.seattleu.edu/scieng/engpc/stdntprj/mme011/MME01.1web%20Proposal.doc Flow Visualization System for a Pulse Detonation Engine]
* [http://www.mne.psu.edu/PSGDL The Penn State University Gas Dynamics Lab, where schlieren imaging is done in all its forms]
* [http://www.springerlink.com/content/2529612236q71278/ Background Oriented schlieren for flow visualisation in hypersonic impulse facilities]
* [http://espace.library.uq.edu.au/eserv.php?pid=UQ:8810&dsID=SreekanthRughuna.pdf Visualisation of supersonic flows in shock tunnels using Background Oriented Schlieren (BOS) technique]