Schlieren imaging

 

The optical setup of a schlieren imaging system may comprise the following main sections:^{[citation needed]} Parallel beam, focusing element, stop (sharp edge) and a camera. The parallel beam may be achieved by a point-like light source (a laser focused into a pinhole is sometimes used) placed in the focal point of a collimating optical element. The collimating element may be a lens or a mirror. The optical stop may be realized by a razor placed horizontally or vertically in the focal point of the focusing element, carefully positioned to block the light spot image on its edge. The camera is positioned behind the stop and may be equipped with a suitable lens.^{[citation needed]}

A parallel beam is described as a group of straight and parallel 'rays'.^{[citation needed]} The rays cross through the transparent medium while potentially interacting with the contained acoustic field, and finally reach the focusing element.^{[citation needed]} Note that the principle of a focusing element is directing (i.e. focusing) rays that are parallel - into a single point on the focal plane of the element. Thus, the population of rays crossing the focal plane of the focusing element can be divided into two groups: those that interacted with the acoustic field and those that didn't. The latter group is undisturbed by the acoustic field, so it remains parallel and forms a point in a well-defined position in the focal plane. The optical stop is positioned exactly at that point, so as to prevent all corresponding rays from further propagating through the system and to the camera.^{[citation needed]} Thus we get rid of the portion of light that crossed the acoustic field without interaction. However, there are also rays that did interact with the acoustic field in the following manner: If a ray travels through a region of nonuniform density whose spatial gradient has a component orthogonal to the ray, that ray is deflected from its original orientation, as if it were passing through a prism. This ray is no longer parallel, so it doesn't intersect the focal point of the focusing element and is not blocked by the knife. In some circumstances the deflected ray escapes the knife-blade and reaches the camera to create a point-like image on the camera-sensor, with a position and intensity related to the inhomogeneity experienced by the ray. An image is formed in this way, exclusively by rays that interacted with the acoustic field, providing a mapping of the acoustic field.^{[citation needed]}

The acousto-optic effect couples the optical refractive index of the medium with its density and pressure. Thus, spatial and temporal variations in pressure (e.g., due to ultrasound radiation) induces corresponding variations in refractive index. Optical wavelength and wavenumber in medium depend on refractive index. The phase acquired by electromagnetic wave traveling through the medium is related to the line-integral of the wavenumber along the propagation line.^{[citation needed]}

For a plane-wave electromagnetic radiation traveling parallel to the Z-axis, the XY planes are iso-phase manifolds (regions of constant phase; the phase does not depend on coordinates (x,y)). However, when the wave emerges from the acoustic field, XY planes are not iso-phase manifolds anymore; the information about the accumulated pressure along each (x,y) line resides in the phase of the emerging radiation, forming a phase image (phasor) in the XY plane. The phase information is given by the Raman-Nath parameter:^[3]

${\displaystyle v(x,y)={\frac {2\pi \kappa }{\lambda }}\int {p(x,y,z)}\,dz}$ 

with ${\displaystyle \kappa }$  - the piezooptic coefficient, ${\displaystyle \lambda }$  the optical wavelength and ${\displaystyle p(x,y,z)}$  the three-dimensional pressure field.^[4] The schlieren technique converts the phase information into an intensity image, detectable by a camera or a screen.

The accepted gold-standard for quantitative acoustic measurement is the hydrophone. However, scanning the acoustic field with a hydrophone suffers from several limitations, giving rise to supplementary evaluation methods such as the schlieren imaging. The importance of the schlieren imaging technique is prominent in HIFU research and development. ^[5] Advantages of schlieren imaging include:

• Free field: the investigated acoustic field is not distorted by the measuring probe.
• High intensity measurements: the method is compatible with high acoustic intensities.
• Real time: Schlieren imaging system provides on-line, live video of the acoustic field.

• Hargather, Michael John; Settles, Gary S. (9 July 2009). "Natural-background-oriented schlieren imaging". Experiments in Fluids. 48 (1): 59–68. doi:10.1007/s00348-009-0709-3. S2CID 53590637.
• Atcheson, Bradley; Heidrich, Wolfgang; Ihrke, Ivo (5 October 2008). "An evaluation of optical flow algorithms for background oriented schlieren imaging". Experiments in Fluids. 46 (3): 467–476. doi:10.1007/s00348-008-0572-7. S2CID 17713504.
• Skeen, Scott A.; Manin, Julien; Pickett, Lyle M. (2015). "Simultaneous formaldehyde PLIF and high-speed schlieren imaging for ignition visualization in high-pressure spray flames". Proceedings of the Combustion Institute. 35 (3): 3167–3174. doi:10.1016/j.proci.2014.06.040.
• Willert, Christian E.; Mitchell, Daniel M.; Soria, Julio (5 April 2012). "An assessment of high-power light-emitting diodes for high frame rate schlieren imaging". Experiments in Fluids. 53 (2): 413–421. Bibcode:2012ExFl...53..413W. doi:10.1007/s00348-012-1297-1. S2CID 120726611.

• A presentation of schlieren imaging on YouTube
• Acoustic Field Characteriztation with Schlieren System - a short presentation