| 序号 | 专利名 | 申请号 | 申请日 | 公开（公告）号 | 公开（公告）日 | 发明人 |
|---|---|---|---|---|---|---|
| 1 | 一种测定半结晶高分子材料各相态组分含量的热分析方法 | CN201710040404.7 | 2017-01-19 | CN106770427A | 2017-05-31 | 王昉; 于海洋; 顾正桂 |
| 本发明提供一种测定半结晶高分子材料各相态组分含量的热分析方法，分别采用常规式和步进式升温对样品进行加热，将StepScan DSC曲线解析为一条可逆比热容曲线和一条不可逆热流曲线，通过可逆比热容曲线上比热容的不连续突变来确定玻璃化转变位置，再根据玻璃化转变时的比热容增量和DSC曲线上的熔融焓，确定半结晶高分子不同相态组分的含量。本发明通过SSDSC技术可以将玻璃化转变从动力学过程中分离出来，得到试样升温过程中的可逆比热容和玻璃化转变温度以及熔融焓等参数，不仅可以获得半结晶高分子材料的玻璃化转变温度，还可以准确获得不同温度所对应的可逆比热容，同时可以根据比热容和熔融焓计算出半结晶高分子试样中结晶态，流动无定型态和硬无定型态不同相态的含量。 | ||||||
| 2 | 金属箔的热量测量方法、表面特性的调整方法、激光穿孔方法以及热量测量装置 | CN200810100035.7 | 2003-10-27 | CN101306490A | 2008-11-19 | 坂本胜; 新井英太; 王江涛 |
| 一种金属箔之热量测量方法，对金属箔照射微量的激光，由金属箔的背面所设置的传感器来测量金属箔所吸收的热量；以及一种金属箔的热量测量装置，具备：内面具有光反射面的激光导入管、用以对该激光导入管的底部设置热量测量对象的金属箔的装置、以及与金属箔的背面密合而可测量热量的传感器。提供一种可测量金属箔的热量来高效率形成印刷电路基板的层间连接孔(贯通孔)、激光穿孔变得容易、可形成品质优异的稳定的小孔径层间连接孔的方法以及装置。 | ||||||
| 3 | 金属箔的热量测量方法、表面特性的调整方法、激光穿孔方法以及热量测量装置 | CN200380101383.1 | 2003-10-27 | CN1705876A | 2005-12-07 | 坂本胜; 新井英太; 王江涛 |
| 一种金属箔之热量测量方法，对金属箔照射微量的激光，由金属箔的背面所设置的传感器来测量金属箔所吸收的热量；以及一种金属箔的热量测量装置，具备：内面具有光反射面的激光导入管、用以对该激光导入管的底部设置热量测量对象的金属箔的装置、以及与金属箔的背面密合而可测量热量的传感器。提供一种可测量金属箔的热量来高效率形成印刷电路基板的层间连接孔(贯通孔)、激光穿孔变得容易、可形成品质优异的稳定的小孔径层间连接孔的方法以及装置。 | ||||||
| 4 | 金属箔的激光穿孔方法 | CN200810100035.7 | 2003-10-27 | CN101306490B | 2011-08-17 | 坂本胜; 新井英太; 王江涛 |
| 一种金属箔的激光穿孔方法，对金属箔照射微量的激光，测量金属箔所吸收的热量，根据孔径与吸收热量以及吸收热量与金属箔表面特性之间的相互关系，通过调整金属箔的表面特征，调整激光穿孔时的金属箔的孔径。 | ||||||
| 5 | 液体状态检测传感器 | CN200710000993.2 | 2007-01-17 | CN101008624B | 2010-07-21 | 山本享史; 笹沼威夫; 佐藤美邦 |
| 本发明提供一种用于检测液体状态的液体状态检测传感器，其具有与传感器元件固定连接的端子元件和在其远端部直接地或间接地固持该传感器元件并包围至少一部分该端子元件的固持管，该液体状态检测传感器被设计成可避免在组装态或在实际使用中因受振动而产生的问题。 | ||||||
| 6 | 液体状态检测传感器 | CN200710000993.2 | 2007-01-17 | CN101008624A | 2007-08-01 | 山本享史; 笹沼威夫; 佐藤美邦 |
| 本发明提供一种用于检测液体状态的液体状态检测传感器，其具有与传感器元件固定连接的端子元件和在其远端部直接地或间接地固持该传感器元件并包围至少一部分该端子元件的固持管，该液体状态检测传感器被设计成可避免在组装态或在实际使用中因受振动而产生的问题。 | ||||||
| 7 | 用于测试和评估在高温操作下的传热元件的方法和系统 | CN201410858441.5 | 2014-12-30 | CN104749203A | 2015-07-01 | V·蒂瓦里; U·斯里瓦斯特瓦; A·夏尔马; A·A·格普塔; S·K·萨兰吉; R·K·马洛特拉 |
| 本发明描述了用于测试和评估在高温操作下的传热元件的方法和系统(200)。系统(200)包括各个构件，其配置为：引入传热流体(HTF)和第二流体到至少一个换热器中，测量一个或多个与在HTF和第二流体之间的传热有关的热力学参数，基于所测量的热力学参数确定所述HTF的至少一个热物理参数，并且最后基于所确定的热物理参数对HTF进行分级。 | ||||||
| 8 | 金属箔的热量测量方法、表面特性的调整方法、激光穿孔方法以及热量测量装置 | CN200380101383.1 | 2003-10-27 | CN100516851C | 2009-07-22 | 坂本胜; 新井英太; 王江涛 |
| 一种金属箔之热量测量方法，对金属箔照射微量的激光，由金属箔的背面所设置的传感器来测量金属箔所吸收的热量；以及一种金属箔的热量测量装置，具备：内面具有光反射面的激光导入管、用以对该激光导入管的底部设置热量测量对象的金属箔的装置、以及与金属箔的背面密合而可测量热量的传感器。提供一种可测量金属箔的热量来高效率形成印刷电路基板的层间连接孔(贯通孔)、激光穿孔变得容易、可形成品质优异的稳定的小孔径层间连接孔的方法以及装置。 | ||||||
| 9 | 섬광을 이용한 비열측정장치 및 측정방법 | KR1020060104968 | 2006-10-27 | KR100821508B1 | 2008-04-14 | 김석광 |
| A specific heat measuring apparatus and method using a flash are provided to measure thermal conduction by measuring specific heat simultaneously with thermal diffusion. A specific heat measuring apparatus using a flash comprises as follows. A specimen holder(40) has a first holder hole(44) perforated to expose one surface(52) of a specimen(50) and a second holder hole(42) etched to receive the specimen. A specimen cover(30) put on the holder has a cover hole(35) perforated to expose the other surface(55) of the specimen. A first specimen holder plate(12) has a first penetration hole(20). A specimen fixing unit is closely fixed to one surface of the first specimen holder plate and equipped with a second specimen holder plate(16). A flash irradiator gives a flash to one surface of the specimen. A light receiving sensor receives light irradiated from the other surface. And, a calculator calculates specific heat of the specimen. | ||||||
| 10 | 解析装置及び解析方法 | JP2016552773 | 2014-10-09 | JPWO2016056109A1 | 2017-07-27 | 共則 中村 |
| 故障個所に対応した熱源位置を特定することができる装置及び方法を提供する。本発明に係る解析装置は、半導体デバイスの熱源位置を特定する解析装置であって、半導体デバイスに交流信号を印加するテスタと、交流信号に応じた半導体デバイスからの光を検出し、検出信号を出力する赤外線カメラと、検出信号に基づいて熱源位置を特定するデータ解析部と、を備える。 | ||||||
| 11 | 比熱容量の測定 | JP2009524110 | 2007-08-13 | JP5642965B2 | 2014-12-17 | リッチナー，ギリース; ハンバービューラー，コンラッド; シェンカー，ベネディクト |
| 12 | Calorimetry method of the metal foil, the adjustment method of surface characteristics, laser drilling method or calorimeter | JP2002327694 | 2002-11-12 | JP3869352B2 | 2007-01-17 | ジャンタオ・ワン; 勝 坂本; 英太 新井 |
| A method for measuring amount of heat in metal foils wherein a small amount of laser light is directed to a metal foil and the amount of heat absorbed by the metal foil is measured by a sensor disposed on the back surface of the metal foil is disclosed. It is also disclosed an apparatus for measuring amount of heat in metal foils comprising a laser light introducing pipe having a light-reflective inner surface; a unit for placing a metal foil, which is subjected to measurement of amount of heat, on the bottom portion of the laser light introducing pipe; and a sensor for measuring amount of heat, which is in close contact with the back surface of the metal foil. A method for forming a small interlayer connection hole (through hole) in a printed circuit board wherein the amount of heat in a metal foil is measured for efficiently forming the interlayer connection hole and drilling with a laser can be conducted easily is disclosed. The resulting small interlayer connection hole (through hole) is excellent in quality and stable. An apparatus used therefor is also disclosed. | ||||||
| 13 | Display device and plastic identifying device | JP2000261921 | 2000-08-30 | JP2002067032A | 2002-03-05 | MATSUSHIMA TAKAAKI; YOKOYAMA SADAHIKO |
| PROBLEM TO BE SOLVED: To simplify the sorting, reduce cost, and make the sorting surer. SOLUTION: By this plastic identifying device, the sorting of a plastic material 100 by hand is made possible by utilizing the difference in a rising temperature when the temperature is raised depending on the material. The plastic identifying device, is provided with a heater 4, a thermography 12, and a projector 11. In this case, the heater 4 heats the plastic material 100. The thermography 12 outputs the measuring result as temperature image data. The projector 11 projects the input temperature image data as it is on the plastic material 100 which is measured by the thermography 12. By superposing the temperature image data on the plastic material 100 by the projector 11, the difference in the quality of the plastic material 100 is visualized. COPYRIGHT: (C)2002,JPO | ||||||
| 14 | Heat capacity measuring method | JP1377197 | 1997-01-28 | JPH10213558A | 1998-08-11 | HATTA ICHIRO; YAO HARUHIKO; EMA KENJI |
| PROBLEM TO BE SOLVED: To provide a method for measuring the heat capacity of a specimen at extremely high accuracy without heat leakage and unstable heating. SOLUTION: A tube 12 which is made of stainless steel and can store liquid specimen inside it is arranged in the space of a hot bath 13, an AC current is flown directly through the tube 12 to apply an AC heat flow, and AC temperature at that time is detected by a thermo couple 19 so as to detect an amplitude and a phase difference between the AC heat flow and AC temperature. Then the heat capacity of the liquid specimen to be inspected is obtained by calculation on the base of the amplitude and phase difference under the conditions that the tube 12 is emptied, a standard liquid specimen of which heat capacity and density are already known is contained, and the liquid specimen to be inspected is contained. COPYRIGHT: (C)1998,JPO | ||||||
| 15 | Method for measuring characteristics of gas under reference condition | JP41910190 | 1990-12-28 | JPH06130055A | 1994-05-13 | URITSUHI BOON |
| PURPOSE: To measure the characteristics of a fluid under reference temperature and pressure conditions by not analyzing the fluid for composition nor detecting the pressure of the fluid, but using the measured characteristic of the fluid under a nonreference pressure or temperature condition. CONSTITUTION: On-site calibration is performed by inputting the pressure P, specific heat cp, and heat conductivity (k) of a test gas to a data bank 170. In a system for measuring characteristics of a gas, the error of a sensor is fetched as a correcting value at the time of re-calibrating the specific heat cp and thermal conductivity (k) when the pressure of the gas is not able to be measured irrespectively of the sensor. The values of the sensor for the thermal conductivity (k) and specific heat cp are decided by using the measured values of the output U of a bridge and time difference dt in the same way as that used in a measurement mode. When the values do not coincide with the input values, constants a3 an a5 are changed so that the values can become coincident with the input values. In this method, inspections must be performed by using a second test gas and, when the results are coincident with the input values, re-calibration can be completed. | ||||||
| 16 | JPH0372944B2 - | JP18768883 | 1983-10-08 | JPH0372944B2 | 1991-11-20 | KATO RYOZO; TAKAYA YASUNAGA |
| 17 | Method and instrument for measuring heat conductivity and specific heat of fluid | JP14652589 | 1989-06-08 | JPH03191852A | 1991-08-21 | ROJIYAA ERU AAGAADO; URURITSUHI BON; ROBAATO JIEI MASHISU |
| PURPOSE: To accurately decide the specific heat and heat conductivity of a fluid by using only one detector by giving a transient temperature change and an energy input of such a level and a length that substantially generate a stable-state temperature to a sensor means. CONSTITUTION: An instrument for measuring heat conductivity and specific heat of a fluid is constituted so that the instrument can generate a temperature pulse in one or more heating elements closely arranged in a fluid to be measured. The hourly changing temperature response of a heater to the pulse changes correspondingly to the characteristic values, such as the heat conductivity (k) and specific heat cp of the fluid. When the fluid flows in the state of a relatively stable sample flow, the hourly changing responses of one or more heat-sensitive sensors coupled with heat generating bodies through the fluid change. The length of the thermal pulse from a supply source must be such a degree that the heat generating bodies reach stable states only during a short period. The pulse causes both stable states and transient states in the sensors. Therefore, the heat conductivity (k) is decided from the flat section of a temperature graph indicating the stable states and the specific heat cp is obtained from the conductivity (k) and the rate of temperature change. COPYRIGHT: (C)1991,JPO | ||||||
| 18 | Method for measurement of heat conductivity and heat capacity | JP1844681 | 1981-02-10 | JPS57132046A | 1982-08-16 | OOTSUKA KANJI |
| PURPOSE:To make the simultaneous and accurate measurement of heat conductivity and heat capacity possible through measurement for some ten seconds by sandwiching a material to be measured beteen two pieces of standard materials of known heat conductivity and heat capacity and mutually different temps., and measuring the change in the temp. on the contact surfaces of the respective materials. CONSTITUTION:As a standard material on a heat accepting side, a thick acrylic plate 2a is used, and a thermocouple 4 for temp. measurement is beforehand affixed in the central part on the top surface thereof. On the other hand, as a standard material on a heat supplying side, a thick copper plate 3a is used, and a thermocouple 5 for temp. measurement is beforehand affixed on the surface to be brought into contact with an object to be measured (for example, a living leaf of pasture, etc.) 1a. The surfaces other than these surfaces are kept covered with heat insulating materials 6. Prior to measurement, the thickness of the sample is measured, after which it is brought in tight contact with the central part on the top surface of the plate 2a, and these are left standing at room temp. until the plate 2a and the sample 1a attain an equal temp. Thereafter, the copper plate 3a is maintained at temp. higher by a few degrees than room temp. in a thermostat and is removed from the chamber and is brought quickly into tight contact with the sample 1a. In about 30 seconds right after the tight contact, the temps. of both contact surfaces are measured with the thermocouple 45 and the heat conductivity and heat capacity are known by using a graph obtained beforehand from the relations. | ||||||
| 19 | 해석 장치 및 해석 방법 | KR1020177011285 | 2014-10-09 | KR1020170066472A | 2017-06-14 | 나카무라도모노리 |
| 고장지점에대응한열원위치를특정할수 있는장치및 방법을제공한다. 본발명에따른해석장치는반도체디바이스의열원위치를특정하는해석장치로서, 반도체디바이스에교류신호를인가하는테스터와, 교류신호에따른반도체디바이스로부터의광을검출하여, 검출신호를출력하는적외선카메라와, 검출신호에기초하여열원위치를특정하는데이터해석부를구비한다. | ||||||
| 20 | 매질의 적어도 하나의 속성을 결정하기 위한 유량 측정 시스템 및 방법 | KR1020167022779 | 2015-01-23 | KR1020160111982A | 2016-09-27 | 루터스,요스트콘라드 |
| 본발명은매질의유량을결정하기위한유량측정시스템에관한것으로서, 코리올리유량센서, 열류센서, 및거기에접속된프로세싱유닛을포함한다. 본발명에의하면, 프로세싱유닛은, 코리올리유량센서및 열센서양자의출력신호에기반하여, 유량측정시스템에서의매질의열전도율및 비열용량중 적어도하나를결정하도록배열된다. 본발명은또한매질의열전도율및 비열용량중 적어도하나를결정하는방법에관한것이다. | ||||||
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