序号 专利名 申请号 申请日 公开(公告)号 公开(公告)日 发明人
101 형광 X 선 분석 장치 및 형광 X 선 분석 방법 KR1020110087203 2011-08-30 KR1020120021270A 2012-03-08 하세가와기요시; 잇쿠유타카; 다키구치히데키
PURPOSE: An apparatus for analyzing fluorescent x-ray and a method thereof are provided to have excellent work efficiency and measure specimens safely. CONSTITUTION: An apparatus for analyzing fluorescent x-ray(100) comprises a radiation source(2), a X-ray detector(3), an analyzer(4), a sample stage, a moving unit(8), a casing(10), a door(20), a height measuring unit, a moving unit controller(9), a laser part(7), a door opening/closing detecting part(21), a laser operation controller, and a height measuring device controller. The radiation source irradiates an irradiating point(P1) on a sample(S) with radiation. The X-ray detector detects characteristic x-rays and scattered X-rays emitting from the sample. The analyzer analyzes signals. The sample is placed on the sample stage. The moving unit relatively moves the sample on the sample stage, the radiation source, and the X-ray detector. The casing accommodates at least the radiation source, the sample stage, and the moving unit.
102 뿜칠석면의 고형화 정도 측정장치 및 고형화 정도 측정방법 KR1020100067271 2010-07-13 KR1020110007954A 2011-01-25 송태협; 이세현; 김영훈
PURPOSE: An apparatus and a method for measuring the solidification of asbestos are provided to enable quantitative measurement by collecting samples in the air. CONSTITUTION: An apparatus for measuring the solidification of asbestos comprises a sample box(10), a vibration plate(7), an air suction device(5), and a filter(6). Spraying asbestos sample(2) is fixed on the top inside the sample box. The sample box has an air outlet(3) and sprays air to spraying asbestos sample(2). The vibration plate is placed on the sample box. The vibration plate comprises an excitation device(71). The air suction device sucks air inside the sample box. The filter filters asbestos fibers included in the air sucked from the inside of the sample box.
103 물체의 구성요소들 및 구조물들에 있어서 결함의 존재를모니터하기 위한 방법 및 장치 KR1020037003461 2001-07-02 KR1020030041138A 2003-05-23 데비,케네스,존
본 발명은 주위압력 하에서 소정의 액체(F)를 함유하는 환경에 배치된 구조물(10)의 무결함 상태를 모니터하기 위해 제공되는 방법 및 장치를 개시한다. 상기 구조물(10)은 외피와 다수의 내부 공동들(14)을 포함한다. 본 방법은 공동들(14)에 추가적인 액체를 공급하는 과정을 포함하며, 상기한 공급 액체는 주변의 대기압력(F) 보다 한계적으로 더 큰 압력으로 공급된다. 상기한 공급된 액체의 유동율에 대한 모니터를 수행하여 유동율의 변화를 검출하게 된다. 이러한 유동율에 있어서의 변화는 구조물(10)을 통한 액체의 추가적인 침투량을 지시하는데 이것은 그 구조물(10)에 있어서의 결함여부(무결성)의 문제를 미리 경고해 주는 역할을 하게 된다. 상기한 모니터 기능은 공급된 액체를 높은 유동 임피던스(28)를 통해 통과시키고 소정의 변환기(30)를 사용하여 상기 임피던스(28) 사이의 압력의 변화를 모니터 함으로써 달성된다.
104 SYSTEM AND METHOD FOR MONITORING HYDROGEN FLUX US15564978 2016-04-07 US20180073956A1 2018-03-15 Andrew Feicht
System and method for monitoring hydrogen flux across the wall of a vessel or pipe, the system including a monitored volume for sealing an attachment to an outside surface of the wall of the vessel or pipe for collecting hydrogen escaping across the wall surface; a membrane selectively permeable to hydrogen in fluid communication with the monitored volume for permitting hydrogen to escape from the monitored volume in between the two at a defined rate such that hydrogen pressure equilibrium may be reached in the monitored volume for a given hydrogen flux across the wall surface of the vessel or pipe; a pressure measuring device in fluid communication with the monitored volume for measuring hydrogen pressure in the monitored volume; and a temperature measuring device in fluid communication with the monitored volume for measuring temperature in the monitored volume.
105 SYSTEM AND METHOD FOR REMOTE MONITORING OF SOLID CONTAMINANT IN FLUIDS US15260087 2016-09-08 US20180067032A1 2018-03-08 Jack D. Burns; Stephen G. Jeane; Jeremy M. Stevens
A pipeline contaminant monitoring apparatus that includes a filter housing and probe configured to isokinetically sample a portion of a pipeline gas stream. The filter housing has a filter configured to trap solid contaminants within the gas stream. A first pressure sensor is located upstream of the filter and a second pressure sensor is located downstream of the filter. A processor is coupled to the first and second pressure sensors. The processor is configured to determine a solid contaminant concentration level in the gas stream based on a rate of change of the pressure drop sensed across the filter.
106 DEVICE AND METHOD FOR DIFFERENTIATING A GAS IN A SAMPLE US14653613 2013-12-19 US20150362400A1 2015-12-17 Thierry Gosse; Philippe Lacarrere; Eric Schaller
A device is provided for testing a sample via a gas stream, including: an opening; structure for generating a device gas stream along at least one flow path passing through the opening; at least one pressure sensor, each pressure sensor being arranged to measure a pressure of the gas stream along at least one flow path; and a mass flowmeter arranged to measure a parameter representative of the mass flow of the gas stream along the flow path. The device is arranged to quantify the presence of a gas of interest within a gas being analyzed and/or to determine the size of a leak hole from a measurement of the parameter representative of the mass flow. A method is also provided that is implemented by such a device. The method can be used to test the integrity of food packaging, and for detecting leaks or problems related to sealing containers.
107 Method and device for the membrane-based analysis of gas components US13518649 2010-12-16 US09010174B2 2015-04-21 Detlef Lazik; Dieter Lazik; Wolfgang Rehak
A method and a device for the analysis of gas components of a matrix employ two sensors, which each comprise a cavity enclosed by a membrane. Both membranes, each on one side of the matrix and on the other side, are exposed to a purge gas and subsequently, the timeline of the differential pressure Δps starting at a start time tA is measured, which is created between the sensors as a consequence of permeation of gas components of the matrix and/or the purge gas through both membranes. From the timeline, a point of time tE is determined, at which the measured differential pressure equals the differential pressure at the point of time tA, whereby the gas component of the matrix, which is different from the purge gas, and its genesis is determined from the time difference Δt=tE−tA.
108 System and Method of Quantifying Impurities Mixed within a Sample of Hydrogen Gas US14320729 2014-07-01 US20140311220A1 2014-10-23 Peter R. Bossard; Luis Breziner, V; Paolo Moreschini
A system and method of taking a sample of hydrogen gas and reducing the hydrogen concentration by a factor greater than 1×108 while increasing the partial pressure of the contaminating gases by a factor greater than 100, so that extremely low levels of contamination can be accurately detected. A sample of hydrogen gas is captured. Only the hydrogen gas is removed leaving all the contaminating gases in the collection chamber. This causes the total pressure of the gas sample within the collection chamber to decrease dramatically since most of the gas was hydrogen. All the contaminants remain in the collection chamber. None are lost through pumping. As such, the concentration of contaminants within the remaining sample increases dramatically. The residual partial pressures of the contaminating gases within the collection chamber and can now be measured by a variety of techniques.
109 Gas probe for sampling gas molecules from a fluid and a system comprising the gas probe US12991212 2008-05-05 US08627710B2 2014-01-14 Claes Nylander; Peter Hebo; Fredrik Enquist
A gas probe for sampling gas molecules from a fluid. A housing includes an orifice and is adapted to be arranged in gas communication with a test gas sensor. The probe includes a stack of layers, whereby gas sample molecules have to pass through all layers of the stack in order reach the sensor. The stack includes at least a first membrane layer, a first spacer layer, a first filter layer and a second spacer layer. The housing includes an inlet for introducing blocking gas molecules into the second spacer layer and an outlet for discharging blocking gas molecules out of the first spacer layer. The gas probe is connectable to a control unit for controlling the blocking gas flow into the second spacer layer.
110 Method for determining diffusion and/or transfer coefficients of a material US12452994 2008-07-28 US08368411B2 2013-02-05 Mihails Kusnezoff; Steffen Ziesche; Anne Paepke
The invention relates to a method for the determination of diffusion coefficients and/or exchange coefficient of a material having electronic and ionic conductivity. The material is permeable to at least one gas. It is the object of the invention to provide a cost-effective, accurate method for the determination of the diffusion coefficient and of the surface exchange coefficient which can be carried out in a short time and can thus be used for a screening of materials, in particular for application in the field of permeation membranes. The procedure is followed in accordance with the invention such that a sample of the material is arranged in a measurement chamber and has an electric current passed through it for a determination of the electric resistance. In this respect, a gas mixture in which the respective gas is contained is conducted through the measurement chamber as a gas flow and the partial pressure of the respective gas in the gas mixture is changed periodically at regular intervals. The change in the electric resistance of the sample is measured and a diffusion coefficient and/or exchange coefficient of the material can be determined for the respective gas from the determined change in the electric resistance.
111 IRRIGATION CONTROL SYSTEM US13240815 2011-09-22 US20120006421A1 2012-01-12 Uri SHANI; Abraham Schweitzer
A tensiometer for use in determining matric potential of a soil includes a water inlet; a hydraulic coupler comprising a porous material for providing hydraulic coupling between water that enters the inlet and the soil; and a septum that seals water that enters the inlet against ingress of air via the porous material.
112 Method and device for investigation of a surface layer US10979082 2004-11-02 US08067244B2 2011-11-29 Sune Svanberg; Mikael Sjoholm; Gabriel Somes-Falean
A method and device for investigation of a surface layer of a material. The material without surface layer is exposed for a gas and the penetration of the gas into the material is measured. Then the surface layer is applied to the material. Finally, the material including the surface layer is exposed for the gas and the penetration of the gas into the material through the surface layer is measured. The measurement of the passage of the gas into the material is performed by a method comprising measurement of light absorption by the gas by absorption spectroscopy.
113 Integrated multi-measurement system for measuring physical properties of gas diffusion layer for polymer electrolyte fuel cell with respect to compression US12406742 2009-03-18 US07913572B2 2011-03-29 Gu-Gon Park; Jin-Soo Park; Min-Jin Kim; Young-Jun Sohn; Seok-Hee Park; Sung-Dae Yim; Tae-Hyun Yang; Young-Gi Yoon; Won-Yong Lee; Chang-Soo Kim
Disclosed is an integrated multi-measurement system for measuring physical properties including thickness, electrical resistance and differential pressure of a gas diffusion layer for a polymer electrolyte fuel cell with respect to compression. The integrated multi-measurement system simultaneously measures changes in the physical properties of the gas diffusion layer depending on pressure upon measurement of the physical properties of the gas diffusion layer of the fuel cell and also measures through-plane permeability in which a gas is passed through a sample in a direction perpendicular to the sample and in-plane permeability in which a gas is passed through a sample in a direction parallel to the sample.
114 Device for passing through a gas mixture US12126557 2008-05-23 US07841227B2 2010-11-30 Andreas Varesi
A device for passing through a gas mixture comprises a capillary apparatus with one or more capillaries connecting a first side of the capillary apparatus to a second side of the capillary apparatus, wherein each capillary tapers from one side towards the other side of the capillary apparatus at least in sections.
115 Systems and Methods for Monitoring Chemical and Biological Activity using Differential Measurements US12777273 2010-05-11 US20100296973A1 2010-11-25 John J. HEFTI; Dean M. Drako
A system operable to monitoring bio/chemical activities includes a first measurement probe, a second measurement probe and a comparator. The first measurement probe is operable to interrogate one or more physical properties of a sample at a first location of the sample, and to output, in response, a first measurement signal. The second measurement probe is operable to interrogate one or more physical properties of the sample at a second location of the sample, and to output, in response, a second measurement signal. The comparator is coupled to receive the first and second measurement signals, the comparator configured to output a difference signal comprising the difference between the first and second measurement signals, the difference signal corresponding to the difference in one or more bio/chemical activities occurring at the first location of the sample relative to the second location of the sample.
116 APPARATUS AND METHOD FOR CONDITION MONITORING OF A COMPONENT OR STRUCTURE US12517720 2007-11-27 US20100139370A1 2010-06-10 Jonathan Fievez
An apparatus (10) monitors the condition of a component (12) by measuring the conductivity to air flow of a sealed cavity (14) formed on the surface of the component (12). The apparatus (10) comprises an unregulated pressure source (16) that is coupled to the cavity (14) via a fluid flow restriction (17). A measurement system (19) provides a measurement of, or related to, the volumetric air flow through the restriction (17), and calculates a conductivity index CI to air flow of the cavity in accordance with the equation CI=flow/pressure difference. In this equation “flow” is the volumetric flow of air through the flow restriction and “pressure difference” is the difference in pressure across the cavity with reference to atmospheric or ambient pressure. In the event that a crack traverses the cavity and provides a flow path to the atmosphere, the conductivity index CI will be a non-zero value. The higher the conductivity index the larger the crack.
117 Modular microfluidic system US11304188 2005-12-15 US07730904B2 2010-06-08 Mark Peter Timothy Gilligan; Philip James Homewood; Robert J. Ranford; Paul M. Crisp
An apparatus (10) for performing microfluidic processes comprising a base (50), a plurality of fluidic modules (20) releasably attached to the base (50), each fluidic module (20) comprising a fluid port (25) and a microfluidic manifold module (40) comprising a plurality of ports (45). A frame (70) is attached to the base (50) for releasably retaining the microfluidic manifold module (40), the frame (70) being moveable relatively to the base (50) to move the microfluidic manifold module (40) into contact with the fluidic modules (20) such that each fluid port (25) of the fluidic modules (20) aligns and seals with a respective port (45) on the microfluidic manifold module (40) thus completing a microfluidic circuit. A method for constructing and testing the apparatus (10) is also disclosed.
118 Systems and methods for monitoring chemical and biological activities using differential measurements US10799000 2004-03-11 US07713477B2 2010-05-11 John J. Hefti; Dean M. Drako
A system operable to monitoring bio/chemical activities includes a first measurement probe, a second measurement probe and a comparator. The first measurement probe is operable to interrogate one or more physical properties of a sample at a first location of the sample, and to output, in response, a first measurement signal. The second measurement probe is operable to interrogate one or more physical properties of the sample at a second location of the sample, and to output, in response, a second measurement signal. The comparator is coupled to receive the first and second measurement signals, the comparator configured to output a difference signal comprising the difference between the first and second measurement signals, the difference signal corresponding to the difference in one or more bio/chemical activities occurring at the first location of the sample relative to the second location of the sample.
119 OSMOTIC REACTION DETECTOR FOR MONITORING BIOLOGICAL AND NON-BIOLOGICAL REACTIONS US12546713 2009-08-25 US20090320573A1 2009-12-31 Francisco E. Torres; Karl Littau; Eric Shrader
A method and apparatus for measuring the presence or absence of reaction between a first and second material of interest by measuring osmotic pressure changes in a reaction cell. The reaction cell is capable of measuring the small changes in pressure that occur due to osmotic pressure shifts during a catalytic or binding reaction at species concentrations down to approximately 10−7 M.
120 Testing Hydrogen Flux Through Solid and Liquid Barrier Materials US12050412 2008-03-18 US20080233010A1 2008-09-25 James G. Blencoe; Michael Naney
Apparatus and methods for testing the hydrogen-gas compatibilities, hydrogen-gas embrittlement susceptibilities, hydrogen-gas containment performances, and/or the hydrogen-gas pressure-cycling durabilities, of hollow enclosures (“test specimens”), with single-layer, double-layer, or multi-layer walls, composed of various barrier materials, are disclosed. Barrier materials include but are not limited to: carbon steel, stainless steel, copper, aluminum, a polymeric material (e.g., high-density polyethylene), and a liquid material (e.g., water, or an aqueous solution). The test gas is either high-purity hydrogen or a hydrogen-bearing gas mixture (e.g., hydrogen gas mixed with methane/natural gas and/or biomethane). A key piece of the testing equipment is an enclosure that surrounds the test specimen. Fabricated from high-strength, porous solid material (e.g., porous stainless steel), the enclosure (i) captures the hydrogen gas that diffuses through the wall(s) of the test specimen, and (ii) channels the flow of that gas toward a volume-calibrated reservoir.
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