Abstract:
The present invention is a method for improving the estimation of physical properties of a material based on the infrared spectrum of the material and the correlation between directly-measured properties of interest and the infrared spectra of a representative set of calibration specimens of the material. By intentionally introducing spectral distortion such as transmittance shifts, wavelength shifts, absorbance-baseline shifts and absorbance-baseline tilts into the infrared spectra of the representative specimens and then determining the correlation between the distorted spectra and the directly-measured properties before applying the correlation to the infrared spectrum of the sample being analyzed, the correlation is self-compensating for the types of distortion introduced.
Abstract:
A portable spectrophotometer includes a small-diameter optical sphere as well as optical detectors and signal processing and display circuitry which allows the instrument to be taken to an object to be measured and which provides a readout of color values at the portable instrument. The instrument is capable of providing specular-included and specular-excluded color readings simultaneously. The interior of the integrating sphere is coated with a highly reflective, color-absorbing material, and light from an incandescent lamp is diffused within the sphere prior to reaching the object to be measured. The sphere is provided with a first aperture which receives spectrally-included light and which is positioned to absorb a spectral component of the diffused source light. A second aperture positioned at a corresponding angular position with respect to the object measures specular-excluded light, excluding the specular component absorbed by the first aperture. Light detected from the first aperture is analyzed at a plurality of wavelengths obtained by the use of interference filters, and the light obtained from the second aperture is analyzed at one of the plurality of wavelengths. By appropriately combining the specular-included and specular-excluded at one wavelength, a value for the specular component is derived. Since this value is a theoretical constant, it is used to derive a specular-excluded reading from each of the specular-included readings at the different wavelengths.
Abstract:
In addition to obtaining a spectrum of a measuring spot of an object, a spectrum measuring apparatus comprises a TV camera for picking-up a total image of the object. Signals corresponding to the spectrum and the total image are superposed so that the spectrum and the total image are displayed on a screen of a TV monitor at the same time.
Abstract:
To reduce the data rate of a digitalized measuring signal produced in Fourier spectroscopy, the analog signal representing the interferogram is mixed with a second electrical signal whose frequency is modulated in proportion to the deviation of the instantaneous actual speed of the moving mirror of a double beam interferometer from its constant desired speed. Only the difference frequencies produced as a result of the frequency mixing are digitalized and supplied to an associated computer for analysis of the interferogram. The digital measuring signal thus obtained is distinguished by a substantially reduced data rate without giving rise to additional errors in the frequency transformation. To produce the second frequency modulated electrical signal, a laser source is used which supplies a laser beam into the interferometer parallel to the measuring beam. The interferogram of the laser beam produced in the interferometer is converted by a second optoelectrical converter into an electrical signal frequency modulated in a desired manner and is supplied to a frequency mixer.
Abstract:
A measuring method for a time resolved emission spectrum or a time resolved excitation spectrum, wherein when emission transient waveforms from a pulse-excited sample are measured by the time correlation photon counting method; the emission transient waveforms are measured at every optimum wavelength in a problematical emission spectrum region; the measured emission transient waveforms are stored in a memory in order and at every wavelength; all the transient waveforms in each wavelength are measured; thereafter, the time resolved emission spectrum or the time resolved excitation spectrum is produced on the basis of all the above-mentioned stored emission transient waveform data, thereby enabling the proper spectrum to be produced efficiently.
Abstract:
A method and apparatus for analysis of liquid samples is described. The method involves simultaneously introducing a predetermined quantity of a given sample and a predetermined quantity of a selected reagent therefor directly into separate flow lines by aspiration from separate containers; bringing the extracted sample and the extracted reagent together into a common flow channel; and causing the sample/reagent mixture to travel along the flow channel as a discrete liquid slug interposed in the stream of a carrier liquid to the measurement cell of an analytical instrument. Another aspect of the method is characterized in that a single pump is used to draw sample and reagent into separate arms of the flow channel which subsequently merge, and to drive the sample/reagent mixture along the flow channel; and in that a carrier liquid is drawn into the flow channel by said pump so that the material within the flow channel is carried along as a continuous liquid phase. The apparatus comprises means for extracting the sample and reagent; a peristaltic pump for driving material along the flow channel; a stepping motor connected or connectable to drive the peristaltic pump, the stepping motor being controllable (preferably by a microprocessor) so that it can make precise angular movements; means, for example a Y-piece or T-piece, for bringing the extracted sample and the extracted reagent together into a common flow channel; and means for deriving an analytical measurement from material in the flow channel. The method and apparatus are particularly well suited for use in the automatic analysis of samples of clinical interest.
Abstract:
A fiber optic device consists of bundles of fiber optic rods which extend from an input face of the device, to which images of a spectrogram are directed to an output face. The input and output faces of the bundles are corrected so that images of a spectrogram, which are either tilted with respect to the spectrogram's height axis or are curved due to Berry curvature, pass through the device and appear at its output face in directions perpendicular to the spectrograms length axis and parallel to its height.
Abstract:
The spectrometer comprises a symmetrical ruled diffraction grating with the collimated light beam under examination being incident thereupon diffracting in the right and left diffraction orders, into two light rays of a preset wavelength. One of these light rays returns to the diffraction grating, being reflected from a scanning mirror common to both light rays. The other light ray returns to the same diffraction grating after being reflected from an additional mirror, whose reflecting surface is parallel to the diffraction grating rulings, then from the scanning mirror, common to both light rays, and again from the additional mirror. Upon returning both light rays diffract in the same direction, interfere with each other and are registered. The method of examining the spectral composition of light realized through the use of the above-mentioned spectrometer, consists in using two twice diffracted light rays which have been reflected (2n+1) and (2n+3) times from two reflecting surfaces, where n is a natural number.
Abstract:
A broadband optical discriminator for determining the wavelength of received radiation which is in a narrow band is described. The received radiation is passed through a polarization spoiler, a linear polarizer, a polarization dispersion device, and a beam splitting polarizer forming two beams. The intensity of the two beams is converted into electrical signals. The electrical signals are processed to provide a signal indicative of the wavelength of the incident radiation.
Abstract:
Method and apparatus for causing light to interact with surface acoustic waves so that the light is either scattered out of or coupled into an optical wave guide. In the case of scattering when the light is propagating in an optical wave guide and chirped surface acoustic waves interact with the light, the light is scattered out of the optical wave guide into a focused beam. The focused beam of light travels in a path parallel to the surface acoustic waves and at the same velocity as the acoustic waves. The focused beam can scan objects to obtain electrical signals corresponding to the optical image of the objects and also the beam can be focused on a plurality of photodetectors to multiplex the light. In the case of coupling when the light is incident on an optical wave guide and the frequency of the chirped surface acoustic waves is selectively varied, the light is selectively coupled into the optical wave guide in a corresponding manner. The selective coupling of the light permits the frequency spectrum and the angular distribution of the light to be analyzed.