WO2012153793A1 - Mesure d'état de matériau, procédé de détection et dispositif de détection - Google Patents
Mesure d'état de matériau, procédé de détection et dispositif de détection Download PDFInfo
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- WO2012153793A1 WO2012153793A1 PCT/JP2012/061944 JP2012061944W WO2012153793A1 WO 2012153793 A1 WO2012153793 A1 WO 2012153793A1 JP 2012061944 W JP2012061944 W JP 2012061944W WO 2012153793 A1 WO2012153793 A1 WO 2012153793A1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N22/00—Investigating or analysing materials by the use of microwaves or radio waves, i.e. electromagnetic waves with a wavelength of one millimetre or more
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- FIG. 14 is an explanatory view schematically showing the detection apparatus used in Example 5.
- FIG. 15 is a graph showing the relationship between the water temperature measured in advance in Example 5 and the resonance frequency.
- FIG. 16 is a graph showing the results of water temperature control performed in Example 5.
- FIG. 17 is an explanatory view schematically showing the detection apparatus used in Example 6.
- FIG. 18 is a graph showing the relationship between the alumina catalyst temperature measured in advance in Example 6 and the resonance frequency.
- FIG. 19 is a graph showing the results of performing alumina catalyst temperature control in Example 6.
- FIG. 20 is an explanatory view schematically showing a cavity, a reaction tube, and an electric field intensity distribution that are used in Example 7 as a TM 110 mode.
- the present invention is not limited to the above adjustment method. For example, if a standing wave of TM 010 having the strongest electric field intensity at the center as shown in the electric field intensity distribution 11 and uniform electric field intensity in the longitudinal direction of the cylindrical axis is formed, the reactants in the reaction tube 15 are made uniform. Can be heated. Since the frequency of the signal generation source 13 at this time is determined by the dielectric constant of the reactant, the state of the reactant can be detected by monitoring the frequency.
- the present embodiment is not limited to a standing wave of TM mn0 (m is an integer of 0 or more and n is an integer of 1 or more), and is not limited to a cylindrical microwave irradiation space.
- the present invention is not limited to the configuration using the signal generation source 13 and the amplifier 12, and can be realized by a microwave generation source capable of adjusting the frequency.
- the microwave incident wave power PF and the reflected wave power PR were measured, and the ratio PF / PR was taken as the microwave reflectance.
- the result is shown in FIG. From the figure, it can be seen that the relationship between reflectance and temperature is monotonically increasing, and from this relationship, the temperature of ethylene glycol can be estimated by actually measuring the reflectance during microwave irradiation. (Ethylene glycol is not vaporized at this temperature.)
- Example 6 With the apparatus shown in FIG. 17, the temperature control of the alumina-supported catalyst 30 arranged in the quartz tube 15 was performed without a temperature sensor.
- the same reference numerals as those in FIG. 14 denote the same components.
- a radiation thermometer is often used for non-contact temperature measurement.
- the radiation thermometer measures the surface temperature of the outer wall of the reaction tube, and the temperature of the catalyst in the reaction tube is measured by the wavelength of the infrared rays to be measured. It was necessary to devise special measures such as In the present embodiment, even the substance in the reaction tube can be detected if there is a change in the dielectric constant temperature, and can be used even when non-contact measurement using a conventional radiation thermometer or the like is not possible.
- Example 9 The ethylene glycol bubbles were sensed in the same manner as in Example 4 except that the cavity in the TM020 mode was used.
- FIG. 22A shows a cavity to be TM 020 used as microwave irradiation means
- FIG. 22B shows the electric field intensity distribution. In this case, the electric field strength at the center is strong, but there is a place where the electric field intensity is maximized on the outside.
- a spiral reaction tube was passed through this part to detect bubbles. As a result, it was found that the same result can be obtained with the form shown in this embodiment as the microwave irradiation means.
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Abstract
L'invention vise à procurer un procédé pour détecter de façon pratique et sûre l'état d'un matériau dans un réacteur chimique ou dans un dispositif de réaction sans l'utilisation d'un capteur spécialisé et sans toucher le matériau. A cet effet, l'invention porte sur un procédé pour mesurer et détecter, par rayonnement de micro-ondes, la température, l'état de phase et la composition d'un matériau irradié, la présence de matières étrangères ou de bulles, de changements dans ces caractéristiques, ou la progression d'un changement chimique ; le procédé comprend les états consistant à irradier le matériau par des micro-ondes, et à mesurer et à détecter l'état du matériau irradié sur la base d'un changement entre avant et après l'irradiation par les micro-ondes.
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Cited By (10)
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JP2014221446A (ja) * | 2013-05-13 | 2014-11-27 | 東京理化器械株式会社 | 反応装置 |
JP2015161597A (ja) * | 2014-02-27 | 2015-09-07 | 国立研究開発法人産業技術総合研究所 | 電磁波特性評価装置 |
WO2015146600A1 (fr) * | 2014-03-28 | 2015-10-01 | 株式会社前川製作所 | Procédé de mesure de la température interne d'un objet à congeler et dispositif de mesure de la température interne d'un objet à congeler |
JP2016079971A (ja) * | 2014-10-17 | 2016-05-16 | 兵神装備株式会社 | 容積式ポンプ |
WO2017051461A1 (fr) * | 2015-09-24 | 2017-03-30 | 株式会社前川製作所 | Procédé de mesure de la température interne d'un objet congelé et dispositif pour mesurer la température interne d'un objet congelé |
JP2017220461A (ja) * | 2017-08-30 | 2017-12-14 | 光洋サーモシステム株式会社 | マイクロ波加熱に関する被加熱物の負荷推定装置、マイクロ波加熱装置、および、マイクロ波加熱に関する被加熱物の負荷推定方法 |
FR3057062A1 (fr) * | 2016-10-04 | 2018-04-06 | Centre National D'etudes Spatiales | Procede de mesure de temperature d'un milieu, produit programme d'ordinateur, dispositif de traitement et ensemble de mesure associes |
JP2020038060A (ja) * | 2018-08-31 | 2020-03-12 | 国立研究開発法人産業技術総合研究所 | 触媒反応方法、及び触媒反応システム |
JP2020148713A (ja) * | 2019-03-15 | 2020-09-17 | 国立研究開発法人産業技術総合研究所 | 解析装置、方法及びプログラム |
JP7446599B2 (ja) | 2019-12-16 | 2024-03-11 | 国立研究開発法人産業技術総合研究所 | 樹脂乾燥装置及び樹脂乾燥方法 |
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Cited By (17)
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JP2014221446A (ja) * | 2013-05-13 | 2014-11-27 | 東京理化器械株式会社 | 反応装置 |
JP2015161597A (ja) * | 2014-02-27 | 2015-09-07 | 国立研究開発法人産業技術総合研究所 | 電磁波特性評価装置 |
US10161809B2 (en) | 2014-03-28 | 2018-12-25 | Mayekawa Mfg. Co., Ltd. | Method for measuring internal temperature of freezing target object and internal temperature measurement device for freezing target object |
WO2015146600A1 (fr) * | 2014-03-28 | 2015-10-01 | 株式会社前川製作所 | Procédé de mesure de la température interne d'un objet à congeler et dispositif de mesure de la température interne d'un objet à congeler |
EP3109606A4 (fr) * | 2014-03-28 | 2017-03-15 | Mayekawa Mfg. Co., Ltd. | Procédé de mesure de la température interne d'un objet à congeler et dispositif de mesure de la température interne d'un objet à congeler |
JPWO2015146600A1 (ja) * | 2014-03-28 | 2017-04-13 | 株式会社前川製作所 | 凍結対象物の内部温度測定方法及び凍結対象物の内部温度測定装置 |
AU2015235436B2 (en) * | 2014-03-28 | 2017-07-20 | Mayekawa Mfg. Co., Ltd. | Method for measuring internal temperature of object to be frozen and device for measuring internal temperature of object to be frozen |
JP2016079971A (ja) * | 2014-10-17 | 2016-05-16 | 兵神装備株式会社 | 容積式ポンプ |
WO2017051461A1 (fr) * | 2015-09-24 | 2017-03-30 | 株式会社前川製作所 | Procédé de mesure de la température interne d'un objet congelé et dispositif pour mesurer la température interne d'un objet congelé |
JPWO2017051461A1 (ja) * | 2015-09-24 | 2018-04-12 | 株式会社前川製作所 | 凍結対象物の内部温度測定方法及び凍結対象物の内部温度測定装置 |
FR3057062A1 (fr) * | 2016-10-04 | 2018-04-06 | Centre National D'etudes Spatiales | Procede de mesure de temperature d'un milieu, produit programme d'ordinateur, dispositif de traitement et ensemble de mesure associes |
JP2017220461A (ja) * | 2017-08-30 | 2017-12-14 | 光洋サーモシステム株式会社 | マイクロ波加熱に関する被加熱物の負荷推定装置、マイクロ波加熱装置、および、マイクロ波加熱に関する被加熱物の負荷推定方法 |
JP2020038060A (ja) * | 2018-08-31 | 2020-03-12 | 国立研究開発法人産業技術総合研究所 | 触媒反応方法、及び触媒反応システム |
JP7074340B2 (ja) | 2018-08-31 | 2022-05-24 | 国立研究開発法人産業技術総合研究所 | 触媒反応方法、及び触媒反応システム |
JP2020148713A (ja) * | 2019-03-15 | 2020-09-17 | 国立研究開発法人産業技術総合研究所 | 解析装置、方法及びプログラム |
JP7315200B2 (ja) | 2019-03-15 | 2023-07-26 | 国立研究開発法人産業技術総合研究所 | 解析装置、方法及びプログラム |
JP7446599B2 (ja) | 2019-12-16 | 2024-03-11 | 国立研究開発法人産業技術総合研究所 | 樹脂乾燥装置及び樹脂乾燥方法 |
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