Abstract:
A particle counter uses optical scattering with heterodyne detection to lower the particle size detection limit imposed by background scattering from the fluid carrier in which the particles are immersed. In one embodiment, particle counter (10) includes a diode laser-pumped, high intracavity power solid-state laser. Intracavity radiation scatters from particles injected into flow (14) by nozzle (16) and from background gases in laser resonator (20). Scattered light (24), including the Doppler broadened Rayleigh background, is collected by optics (26), transmitted via beam combiner (28), and imaged by condenser lens (30) onto a linear photodiode array (32). Each photodiode (40) detects scattered light from a small length (42) along intracavity beam (40) in view-volume (18). A small amount of light simultaneously exits left-hand resonator mirror (48), is collected by beam expander (50), and redirected by mirrors (58, 60) to beam combiner (28), whence it copropagates collinearly to lens (30), which focuses it onto the photodiode array.
Abstract:
A system and method are provided for the characterization of a sample containing a macromolecule in solution. A light source illuminates the sample, generally in the ultraviolet-visible wavelength range, and a plurality of sensors that are radially disposed about the sample at a plurality of observation angles simultaneously sense the light energy emerging from the sample. An intensity spectrum is calculated as a function of wavelength for each observation angle, from which is calculated a particle characteristic such as shape, conformational change, composition, and particle size distribution. Both scattering and absorption data are utilized to provide complementary information.
Abstract:
The present invention comprises method and apparatus for the quantitative determination of particles in fluid. Apparatus of the invention comprises an emitter set of one or more light emitters, in combination with a detector set of one or more light detectors sensitive to the output of the emitters; during analysis of the sample, data from a plurality of signal paths between the emitter and detector sets are gathered. This information is subsequently evaluated by comparison with known data for different fluid particle contents. Some differentiation between different particles in a fluid sample are possible in many embodiments. Typical uses include analysis of milk and dairy fluids, blood samples, lubricants, suspensions of pigments, etc.
Abstract:
Methods and apparatus are provided for detecting analyte in a sample using diffraction patterns. In the subject method, sample suspected of comprising analyte and particles if the analyte is not the particle, as well specific binding pair members, are combined in an assay medium with a solid surface transparent to a wavelength range of interest. In one embodiment, a cross-linking agent is included in the assay medium, where the particles cross-link in an amount proportional to the amount of analyte in the sample. As the particles interact with analyte and specific binding pair members, larger diffraction particles are formed which are randomly distributed in a single plane in the assay medium. The diffraction particles may remain mobile in solution or may settle on the solid surface. In an alternative embodiment, the solid surface comprises members of a specific binding pair which are randomly distributed, providing for specific binding of the diffraction particles to the surface. The diffraction particles are then irradiated with coherent light, where the light is diffracted into a diffraction pattern by the diffraction particles. The spacing and amplitude of the diffraction pattern is detected and measured. A logic means is used to relate the spacing and amplitude of the diffraction pattern to the presence of analyte in the sample.
Abstract:
A laser (1) is applied on the side of a channel which is traversed by a medium. The light beam from the laser (1) passes across the channel. Particles (5) in the medium within the measuring volume are hit by light and deflect this, thus creating forwardly-directed light cones. These light cones are refracted outside the channel by a lens (6) and thereafter hit a detector plate (8). The light which hits the detector plate (8) occurs in the form of light rings which have arisen by light diffraction. On the detector plate (8) at least two detector rings are arranged, consisting of light-sensitive elements adapted to measure the light power in those light rings which fall onto the light-sensitive elements. In an electronic differentiating unit (9) a difference is created between the measured light power values from two of these detector rings. This results in a difference signal which can be related to the size distribution of particles occurring in the flowing medium.
Abstract:
In a particle size measuring system, particles suspended in a sample cell (8') are illuminated by interrogating light beams (212) including a first interrogating component having a polarization parallel to a scattering plane, and a second interrogating component having a polarization perpendicular to the scattering plane. A photodetector (214) generates first and second intensity signals representative of the intensity, at various scattering angles, of scattered light corresponding to the first and second interrogating components. A processor (126) generates a difference signal representative of the difference between the first and second intensity signals, and calculates a resultant signal representative of particle size, based on a selected arithmetic transformation of the difference signal.
Abstract:
A particle characterisation instrument (200), comprising a light source (201), a sample cell (202), an optical element (204) between the light source (201) and sample cell (202) and a detector (203). The optical element (204) is configured to modify light from the light source (201) to create a modified beam (207), the modified beam (207): a) interfering with itself to create an effective beam (208) in the sample cell (202) along an illumination axis (206) and b) diverging in the far field to produce a dark region (209) along the illumination axis (206) that is substantially not illuminated at a distance from the sample cell (202). The detector (203) is at the distance from the sample cell (202), and is configured to detect light scattered from the effective beam (208) by a sample in the sample cell (202), the detector (203) positioned to detect forward or back scattered light along a scattering axis (306) that is at an angle of 0° to 10° from the illumination axis (206).
Abstract:
Measurement device for the detection and/or analysis of fluid-borne particles, the measurement device comprising means (1, 1') for producing a flow of fluid along a fluid flow path, a laser (2) positioned for emitting a beam (20) of laser light in a measurement volume of the fluid flow path; a lens set (3) for collecting laser light (23) scattered in the measurement volume by fluid-borne particles (9) contained in the flow of fluid, a photo-detector (4) positioned for the detection of scattered laser light (23) collected by the lens set (3), wherein the lens set (3) is configured for focusing the scattered light (23) in a line at a focal distance (f2) of the lens set (3), said line being perpendicular to a flow direction (y) of the flow of fluid in said measurement volume; and wherein the photo-detector (4) is a linear multipixel detector for capturing the laser light focused by the lens set (3), wherein said linear multipixel detector (4) is positioned at a distance from the focal distance (f2) of the lens set (3) and oriented with its longitudinal axis parallel to said line. Measurement method for the detection and/or analysis of fluid-borne particles, comprising the steps of producing a flow of fluid along a fluid flow path, said flow of fluid potentially containing fluid-borne particles (9) to be detected; emitting a beam (20) of laser light in a measurement volume of the fluid flow path; collecting laser light (23) scattered in the measurement volume by fluid-borne particles (9) contained in the flow of fluid and focusing said scattered light in a line at a focal distance (f2), said line being perpendicular to a flow direction (y) of the flow of fluid in said measurement volume; capturing the collected and focused scattered laser light (23) with a linear multipixel photo-detector (4) positioned at a distance from the focal distance (f2) and oriented with its longitudinal axis parallel to said line; repeating the steps of emitting, collecting and capturing a plurality of times during the time of crossing the measurement volume by an individual fluid-borne particle (9) of the smallest size measured by the measurement method.
Abstract:
A system for determining the growth/dissolution rate of colloidal particles is disclosed and includes multiple light sources and multiple sensors. A light source is constructed to emit a beam of electromagnetic radiation at a specimen chamber that holds the colloidal particles. The chamber allows a portion of the combined beam to scatter perpendicularly or at some other angle to the combined beam. The scattered portion of the beam is directed to a sensor that detects electromagnetic radiation. The sensor is connected to processor that activates the light source and obtains an image from the sensor. Multiple images are taken at a time interval and for each image taken, and a total image intensity level is calculated and normalized. A formula is then calculated that fits the normalized values over time and a slope is determined from the formula.
Abstract:
Systems and techniques are disclosed for flat-top intensity laser sheet beam generation. The system includes a source of light directed at a first optical component arranged to receive the light and generate spherical aberration (e.g., third order positive aberration) in the light rays. The spherical aberration results in positive aberrations in the light in a first plane and also results in the light being substantially collimated in a second plane perpendicular to the first plane. In some cases, the source of light is provided from a laser diode and the first optical component is one of an aspherical lens and a spherical lens. The system also includes a second optical component for focusing the light in the second plane. In some cases, the second optical component is a cylindrical lens.