Abstract: An analytical instrument suitable for a use in a variety of industrial environments features a housing having a sealed primary chamber filled with a dry, inert gas at a first static pressure. An instrumentation system is disposed within the primary chamber, where fire hazard is eliminated by the inert gas. The housing additionally includes a reference chamber holding a gas a second pressure lower than the first pressure. One or more pressure switches, in pressure-sensing relationship with both chambers, is operative to interrupt the application of power to the instrumentation system if the differential between first and second pressures falls below a predetermined value. In this manner, the instrumentation system is rendered safe whenever the primary chamber is breached or otherwise loses inert gas pressure.

Abstract: A Raman spectrometer optically separates an optical signal scattered by a sample from an incident excitation light beam into an unshifted return component at a first wavelength and one or more Raman scattered components at shifted wavelengths characteristic of the sample. The unshifted return component—but not the Raman scattered components—is attenuated prior to impinging on an optical detector. The unshifted return then serves as the basis for real-time calibration to account for fluctuations in optical intensity, wavelength shift, and/or spectral peak width, based on a comparison of the unshifted return peak to a reference standard for stable reflectance.

Abstract: An analytical instrument suitable for a use in a variety of industrial environments features a housing having a sealed primary chamber filled with a dry, inert gas at a first static pressure. An instrumentation system is disposed within the primary chamber, where fire hazard is eliminated by the inert gas. The housing additionally includes a reference chamber holding a gas a second pressure lower than the first pressure. One or more pressure switches, in pressure-sensing relationship with both chambers, is operative to interrupt the application of power to the instrumentation system if the differential between first and second pressures falls below a predetermined value. In this manner, the instrumentation system is rendered safe whenever the primary chamber is breached or otherwise loses inert gas pressure.

Abstract: A Raman spectroscopy system features free space optics, wherein an excitation laser beam is directed to a sample, and Raman scattered photons are collected from a desired point of the excitation beam's impact on the sample, through the air, without the use of fiber optics. The excitation laser is directed to a sample, such as fluid flowing in a pipe, through a sight glass in the pipe. A front lens assembly, having a fixed focal point at a predetermined z-axis distance in front of the front-most lens, collects Raman scattered photons, which pass through an optical system to a detector. The Collection Point (CP), or the point along the excitation beam (and within the sample) at which Raman scattered photons are collected—which coincides with the focal point of the front lens assembly—is controlled by physically translating the front lens assembly along the optical axis.

Abstract: A Raman spectrometer optically separates an optical signal scattered by a sample from an incident excitation light beam into an unshifted return component at a first wavelength and one or more Raman scattered components at shifted wavelengths characteristic of the sample. The unshifted return component—but not the Raman scattered components—is attenuated prior to impinging on an optical detector. The unshifted return then serves as the basis for real-time calibration to account for fluctuations in optical intensity, wavelength shift, and/or spectral peak width, based on a comparison of the unshifted return peak to a reference standard for stable reflectance.