Abstract:
A light source for examining sites in heating, ventilating, and air conditioning systems for leaks using a fluorescent dye is described. The light source can include a low voltage lamp or a low heat generating lamp.
Abstract:
An optical configuration and related analysis techniques are presented that provide a practical method for determining the Rytov parameter based on the difference of variances for the differential image motion (average wavefront gradient or wavefront tilt) between two receiving apertures. The Rytov parameter is the log-amplitude variance predicted by an approximate solution to Maxwell's equations for propagation through media with random index of refraction (Rytov theory). It is a useful metric of the optical effects for extended turbulence propagation and is a leading indicator of the performance limitations of adaptive optical compensation devices not related to the transverse coherence diameter. A time-duplex alternative apparatus and a single source alternative apparatus are also disclosed.
Abstract:
A method for determining the time curve of the intensity of radiation present at the location of at least one sample which is being examined. The sample follows a circular path of movement in a sealed sample chamber of a weathering testing device, around a stationary radiation device for producing UW and global radiation. At least one sensor which detects the momentary radiation intensity of the radiation device is provided. The sensor moves together with the at least one sample, and is displaced in relation thereto in relation to the radiation device, for example in the peripheral direction of the path of movement. An electrical signal corresponding to the momentary intensity of the radiation is derived by the sensor at set intervals.
Abstract:
A method and apparatus for detecting for detecting an object within a radiating beam of a radiating source. The method receives reflected and radiated radiation directly from the object to provide a radiation signal. The method then processes the radiation signal to provide a control to the radiating source. A concomitant apparatus comprising a detector and a control circuit is provided. The detector receives reflected and radiated radiation directly from the object and provides a radiation signal indicative of the reflected and radiated radiation received from the object. The control circuit, coupled to the detector, processes the provided radiation signal to provide a control signal to the radiating source.
Abstract:
A modulated infrared source is disclosed in which spatial modulation is accomplished by the rotation of beam forming optics about an infrared source in which a portion of the energy in the beam produced includes energy coming directly from the IR source without being reflected. Close to 100% of the energy from the infrared source is focused by rotating parabolically shaped elements, such that energy losses due to the modulation technique are minimized. The speed of the rotation of the reflective optics is minimized while maintaining sufficiently high modulation frequencies by the provision of four beams from a single source.
Abstract:
Apparatus for efficiently modulating the output from an infrared radiation source is provided by a collector/collimator for collecting and collimating the output of the radiation source and a modulator including a stator and at least one rotor. The stator includes a disc of alternating opaque and transparent radial segments having means associated therewith for gathering the radiation from the source and passing substantially all of it to the transparent segments including optical wedges arranged on the opaque segments and a central reflector/collector. The rotor includes a disc of alternating transparent and opaque radial segments. A second rotor may be provided for adding a second modulation and comprises a disc of alternating opaque and transparent radial segments also having optical wedges arranged on the opaque segments and a central reflector.
Abstract:
A photometering apparatus has a photometering apparatus having a plurality of photometering systems for measuring the brightness of an object. photometering system includes:a light receiving device in which different parts of an object are detected by a plurality of split photodetectors whose light receivers each comprise a detection area which is made separate by at least one insensitive area; a photometering optical system for projecting the image of the object onto the light receiving device; wherein the image of the object formed on the at least one insensitive area of one of the plurality of split photodetectors of one of the plurality of photometering systems is formed on the plurality of detection areas of another of the plurality of split photodetectors of another of the plurality of photometering systems.
Abstract:
An array for projecting thermal images and a method of making same. The array of the present invention combines a two-tier architecture created with special processing whereby each pixel member resides on an elevated platform directly over discrete pixel control electronics and electrically conducting traces couple a plurality of pixels so that they can be controlled to project thermal images at equal to or faster than video frame rates. Microlens assemblies coupled to each discrete pixel improves the thermal efficiency of the array for certain applications. In the method of fabrication, a semiconductor microbridge-type structure obtains with the use of sacrificial layers under deposited pixel members in a compact array so that the pixel electronics reside beneath their associated pixel and the array electronics inhabit the same chip as the array thereby improving fill factor and time constant of the resulting array.
Abstract:
Electron-optical rotationally symmetrical lenses inevitably suffer from chromatic aberration which often determines the resolution limit at low acceleration voltages. This lens defect cannot be eliminated by compensation by means of rotationally symmetrical fields. In order to improve the resolution nevertheless, it has already been proposed to correct the chromatic aberration by means of a corrector (28) provided with two correction elements (34, 40). Each correction element consists of a number of quadrupole fields. Using the known corrector, it has been found that the chromatic magnification error is inadmissibly high. In order to solve this problem, the correction elements in the corrector according to the invention are provided with at least five layers of electrodes (60-a, 60-b, 60-c, 60-d) which produce quadrupole fields. Because of the strong periodicity of the electron paths in the correcting quadrupole fields, the chromatic magnification error is limited sufficiently (or even reduced to zero) so as to allow the use of the corrector for practical purposes.
Abstract:
A method for adjusting an optical system of an energy beam apparatus by using a mark signal that is obtained by one-dimensionally or two-dimensionally scanning a mark on a sample with an energy beam. The mark has a one-dimensional or two-dimensional periodic structure. A first mark signal is detected by scanning the mark with a beam. The mark is set on the optical axis of the optical system. A second mark signal is detected by scanning the mark with a beam. The mark is located at a position that is deviated from the optical axis. A deviation of a deflection position is determined based on a phase difference between the first and second mark signals.