Abstract:
A photometer in which a measuring phase, a reference phase and a dark phase are produced by means of a chopper. These phases are staggered in time, so that a single detector can be provided for all phases. In the photometer the object to be measured is situated between two light conductors, the one light conductor leading to the detector and the other light conductor leading to the chopper input. The chopper output is carried by an additional light conductor to the detector.
Abstract:
PURPOSE: To obtain a double device with improved accuracy and stability which is provided with double light paths for fluid and reference medium as well as almost the same and self-compensation optical raws for sample fluid and reference medium, concerning new light transmitting device for radiation in the fluid. CONSTITUTION: A light transmitting device 10 is provided with a pair of reference channels 14 and 16 consisting of glass bars and a pair of sample channels 12 and 18 housing a sample fluid. A beam splitter 46 and a mirror 56 allow a first part of incident beam of radiation passing through a reference approach channel 14 and a second part of incident beam passing through a sample approach channel 12 to pass through therein. The first part is reflected through a reference outgoing channel 16 and the second part is reflected through a sample outgoing channel 18. The beam splitter 46 and mirror 56 allow the outgoing beam to direct to a common outlet path 73.
Abstract:
A photometer in which a measuring phase, a reference phase and a dark phase are produced by means of a chopper. These phases are staggered in time, so that a single detector can be provided for all phases. In the photometer the object to be measured is situated between two light conductors, the one light conductor leading to the detector and the other light conductor leading to the chopper input. The chopper output is carried by an additional light conductor to the detector.
Abstract:
PURPOSE:To remove a back light noise and to take accurate measurement by rotary sectors which rotate in synchronization with each other on the optical axis of laser light emitted toward gas to be measured and a reflecting mirror between both sectors, and further providing a reflecting plate behind the gas to be measured on the optical axis. CONSTITUTION:The rotary sectors 5A and 5B are rotated by a motor 6 in synchronization with each other; a transmission hole 15 and a total absorbing plate 16 are arranged on the sector 5A at the side of the laser element 1 in combination and a transmission hole 15, a total absorbing surface 16, and a total reflecting surface 17 are arranged on the sector 5B at the side of the gas 12 to be measured. The half-mirror 7 is provided between the sectors 5A and 5B and a detector 9 is provided at the focus position of an off-axis parabolic mirror 8 opposed to the mirror 7. Those are stored in a main body 10 and measurement light and reference light pass through a window 11 formed in the main body 10. The reflecting surface 13 of a retroreflector, etc., is provided behid the gas 12 to be measured. Thus, the influence of a back light noise is removed and the concn. and partial pressure of many kinds of gas are measured accurately.
Abstract:
PURPOSE:To measure an NOX concn. simply, rapidly and certainly without performing sampling, by using data light and reference light wohse phase are mutually shifted in specific angles. CONSTITUTION:CO laser beam is passed through a beam splitter 6 to be splitted into two parts which are, in turn, converted to data light and reference light which are mutually different 180 deg. in the phases thereof by a chopper 8. In this case, the data light is permeated through the gas to be measured in the flowline 3 for flowing said gas and met with the same light path as the reference light by a beam splitter 11 to be received as one optical beam by a beam detector 14. The amplitude value component A1 due to the frequency component of the data light from the converting electric signal of the detector 14 and the amplitude value component A2 due to the frequency component of one optical beam are applied through lock-in amplifiers 15a, 15b and the ratio A1/A2 corresponding to an NOX concn. is determined by an operator 16. By this constitution, it is unnecessary to perform the sampling of a sample gas and the NOX concn. is measured simply, rapidly and certainly.