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 Flow meter US40402564 1964-10-15 US3399566A 1968-09-03 BROWN NEIL L
102 Pulsed laser system for relative speed measurement US46292365 1965-06-10 US3388328A 1968-06-11 DRENNING JOHN W
103 Electrical fluid-flow measuring apparatus US68138457 1957-08-30 US3019647A 1962-02-06 BEARD RICHARD B; HUDSON KENNETH C
104 熱式流量計 JP2016549999 2015-07-10 JP6325679B2 2018-05-16 森野 毅; 田代 忍; 深谷 征史; 井上 淳; 猪野 昌信; 斎藤 直生
105 熱式流量計 JP2016551609 2015-07-24 JPWO2016051940A1 2017-04-27 二朗 谷口; 中田 圭一; 圭一 中田; 保弘 浅野; 平山 宏; 平山  宏; 和紀 鈴木
外部と所望の位置で接続端子を接続することができるとともに、流量計測素子による検出精度を安定させることができる熱式流量計を提供することにある。熱式流量計30のフランジ312には接続端子60が設けられている。端子接続部60は、第1曲げ部60cと第2曲げ部60dを有している。第1曲げ部60cは、第1方向d1から第2方向d2に曲がった形状となっている。第2曲げ部60dは、第1曲げ部60cから第3方向d3に曲がった形状となっている。第1仮想平面F1に、複数の接続端子60の接続ピン部60bと、複数の接続端子60の端子接続部60aとを投影したときに、複数の接続端子60の各端子接続部60aの投影領域60Bを通る第1方向d1に沿って延在した仮想線Lが、複数の接続端子60の接続ピン部60bのうち、両側に位置する接続ピン部61,65の投影領域61A,65Aの間を通過するように、第1および第2曲げ部60c,60dが形成されている。
106 成形用材料の流動速度計測方法及び流動速度測定装置 JP2009539127 2008-10-31 JPWO2009057752A1 2011-03-10 秀俊 横井; 範通 増田
キャビティ(3)内を通過する成形用材料(M)のフローフロント(F)に向けて光を投射する単一の光ファイバセンサ(2)を、金型(1)内のキャビティ壁面(4)に設置し、演算装置において、前記光ファイバセンサ(2)のセンサ出に基づき、そのセンサ出力が低下する第1の検出時間と、そのセンサ出力が安定する第2の検出時間との差を示す経過時間を計算し、この経過時間と、光ファイバセンサ(2)のファイバ径及び成形用材料(M)のフローフロントの形状を示す関数とから、前記成形用材料(M)のフローフロント(F)の通過速度を演算する。本発明によれば、2点以上のセンサ組み込みを必要とせず、可視化金型のようなガラス等を組み込んだ特殊な金型を必要とせずに、小型の単一のセンサで容易に、金型内における成形用材料の流動速度を計測することが可能な成形用材料の流動速度計測方法及び流動速度計測装置を提供可能である。
107 Flow rate detecting method and flow rate detecting device using heat signal JP2006069125 2006-03-14 JP2007248118A 2007-09-27 IMAI HIROSHI; MATSUSHIMA KEIICHI; USHIKUSA YOSHISUKE
<P>PROBLEM TO BE SOLVED: To provide a flow rate detecting method using a heat signal allowing accurate flow rate measurement by eliminating the factor of measuring error. <P>SOLUTION: In the flow rate detecting method using the heat signal, the heat signal of temperature variation is written into a medium moving in a flow channel 1, this heat signal is detected by a heat signal detecting means disposed at a position separated from a write-in position, and the moving speed of the medium is measured. A first temperature sensor 20A and second temperature sensor 20B of the heat signal detecting means are arranged on the downstream side of the write-in position at a predetermined interval L, and the moving speed is calculated based on the interval L and the difference between times when these two temperature sensors 20A and 20B detect the heat signal. <P>COPYRIGHT: (C)2007,JPO&INPIT
108 Cylinder of the reciprocating internal combustion engine of the vortex flow rate measuring device and measuring method of the fuel-air mixture in the combustion chamber as well as the reciprocating internal combustion engine JP11909994 1994-05-31 JP3523906B2 2004-04-26 シュッツ マティアス
109 Measurement optical system of the size and distribution of the measuring method and microbubbles and microdroplets of the size and distribution of the microbubbles and microdroplets JP2000001694 2000-01-07 JP3339024B2 2002-10-28 昌信 前田; 達也 川口
110 Method of measuring size and distribution of fine bubble and fine droplet, and measuring optical system for measuring size and distribution of fine bubble and fine droplet JP2000001694 2000-01-07 JP2002257708A 2002-09-11 MAEDA MASANOBU; KAWAGUCHI TATSUYA
PROBLEM TO BE SOLVED: To make a method of measuring a diameter of a defocused image obtained by out-of-focus and the number of interference fringes therein to measure a size and a space distribution of a fine droplet expanded for a fine bubble, and to make the method applicable even when space distribution concentrations of the fine droplets and the fine bubbles are high. SOLUTION: A sheetlike parallel laser beam 2 is emitted in a liquid space floated with the fine bibbles 10, the fine bubble 10 irradiated by the laser beam 2 is photographed defocusedly in a defocus face 8 from a sideface direction forming an angle θ with respect to a laser beam advancing direction via an objective lens 6, and the number of the interference fringes in the defocused image 10" corresponding to the fine bubble 10 is measured to find the diameter of the fine bubble 10 pursuant to Expression 4. COPYRIGHT: (C)2002,JPO
111 Powder quantity measuring device, and method therefor JP32765697 1997-11-28 JPH10160540A 1998-06-19 ADAMS HORST DR; SEITZ KURT
PROBLEM TO BE SOLVED: To make it possible to carry out accurate measurement with little disturbance, by detecting the resonance frequency or the change of amplitude with a resonator provided with a wire coil outside a feed pipe in a metal cylinder for obtaining the powder quantity. SOLUTION: A wire coil 44 which is a spiral or coil-like resonant member surrounding a feed pipe 10 is arranged in a shield metal cylinder 38 to form a microwave resonator 36. The resonator 36 requires a very little space, it guarantees high quality, and it can improve the measurement sensitivity of powder density. The coil 44 is formed on the thin film metal layer of the pipe 10. When the coil 44 is made of gold, its quality is further improved, and measurement sensitivity can be improved. The reference resonance frequency is detected on the known reference powder quantity, and two measurement frequencies are set on both sides of it. The resonance voltages of the powder quantity to be measured on these measurement frequencies are detected and compared, and the powder quantity per unit capacity is obtained from the potential difference. COPYRIGHT: (C)1998,JPO
112 Flow measuring device JP10017694 1994-05-13 JPH07128104A 1995-05-19 EDOMUNTO YURIUSU; HARUTOMUUTO HAUPURITSUHI
PURPOSE: To accurately detect speed and the direction of a conductive liquid medium even if a wall of a conductive material is arranged between a device and the medium by arranging a primary magnetic field and the acting direction of a measuring member at a right angle to a component of flow speed, and arranging the measuring member before and behind the flow direction. CONSTITUTION: A liquid medium flows through a primary magnetic field which is generated by constitutive members 2 arranged on an outside surface of a passage 1 and has plural spatial gradients. Constitutive members 4 to measure this magnetic field are arranged on an outside surface of the passage 1 on a plane 3 at a right angle to the lengthwise directional axis of the passage 1 between them and the members 2 so as to be opposed to the members 2. Signals of the members 4 are introduced by an evaluating unit 5. Flow speed can be directly regulated by mutual intervals of the members 4 and a time delay between continuous respective signals since heterogeneity of a flowing medium and the interaction with a generated magnetic field are almost simultaneously generated in the whole members 4. Therefore, motional speed and the direction of the medium can be accurately measured through a conductive constitutive part. COPYRIGHT: (C)1995,JPO
113 JPH0415888B2 - JP2876286 1986-02-12 JPH0415888B2 1992-03-19 HANSU BURAUN; GEORUKU SHUNAIDAA
114 JPH033164B2 - JP5900280 1980-05-02 JPH033164B2 1991-01-17 NAKAMOTO KOICHIRO; ISHII KYOKAZU; OOYAMA NOBUMI
115 JPH01502049A - JP50092786 1986-01-24 JPH01502049A 1989-07-13
116 Fluidity testing device of casting JP14138183 1983-08-01 JPS6033055A 1985-02-20 YUKIFUKI TAKAO; ICHIYANAGI SHINGO
PURPOSE:To measure the fluidity of a casting quantitatively by providing plural detection electrodes whose tip parts are exposed to the pouring space of a mold and a common and a start electrode whose tip parts are exposed to the pouring space on the molten metal upstream side of detection electrodes, and detecting the conductivity between electrodes. CONSTITUTION:When molten metal is poured in the pouring space 2 from a pouring cup 9, the common electrode 10 and start electrode 11 to conduct to each other firstly over a down gate 3, and consequently a conductivity detecting circuit 13 sends a start signal Ss, so that a time measuring device 14 starts counting seconds. Then, the molten metal reaches a lower electrode 12, the conductivity detecting circuit 13 generates the electrode number (e.g. 1) of the detection electrode 12 and a conductivity signal, and consequently the time measuring device 14 stores the second counting time in the input of the conductivity signal as a time measured value together with the electrode number and also displays the time measured value and electrode number on the screen of a display device 15a.
117 JPS5952367B2 - JP5056873 1973-05-07 JPS5952367B2 1984-12-19 ARUBIN EDOMONDO BURAUN
118 Correlation type speed measuring apparatus JP2243283 1983-02-14 JPS59147271A 1984-08-23 KATOU SHIGERU
PURPOSE:To obtain a simple and compact equipment by providing a heating element outside a pipeline and thermosensitive elements for detecting a fluid temperature at two points downstream to determine the fluid velocity continuously using the maximum value of a cross-correlation function of a detection signal. CONSTITUTION:A heating element 52 is provided outside a pipeline close to the inner surface thereof and a pulselike current is applied thereto from a power surface 59 to heat an internal fluid. The fluid temperature is detected with thermosensitive elements 54A and 54B provided on the downstream of a passage and the maximum value of the cross-correlation function of these detection signals is determined with an arithmetic unit 60 to determine the fluid speed continuously.
119 JPS59500878A - JP50175183 1983-05-19 JPS59500878A 1984-05-17
120 Microwave speedometer JP13057382 1982-07-27 JPS5919860A 1984-02-01 SAWADA YASUHIRO; GOKAN AKIRA
PURPOSE:To measure a speed without any influence to an optical property of a substance by feeding a microwave to the substance transferred through a pipe at two points which are apart from each other and detecting a speed of the substance from a time difference of a modulation component of a reflected wave which receives an amplitude modulation by the substance. CONSTITUTION:The microwaves oscillated at microwave oscillators 6, 11 pass through circulators 7, 12 respectively, enter directional couplers 4, 5 and advance through a transferring pipe 1 in the same direction as a transferring direction A of the substance. A part of the wave reflected by the substance in the pipe 1 passes through the couplers 4, 5 and is made incident to detectors 8, 13 through the circulators 7, 12. A voltage of the modulation component of the reflected wave detected by the detector 8 becomes the voltage of a waveform shown in a figure (a) corresponding to a rough or dense state of the transferring substance. A voltage of the modulation component of the reflected wave detected by the detector 13 becomes the voltage of the similar waveform delayed by a timer tau for transferring the substance by the distance L. Accordingly, the transferring speed V of the transferring substance is detected by obtaining V=L/tau.
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