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    • 4. 发明专利
    • Method and device for measuring thickness of pure zirconium liner of fuel coating pipe
    • 用于测量燃料涂层管的纯锆衬层厚度的方法和装置
    • JPS58223006A
    • 1983-12-24
    • JP10620082
    • 1982-06-22
    • Nippon Atom Ind Group Co LtdToshiba Corp
    • TAMURA TOSHIYUKITAJIMA JIYUNICHIROU
    • G01B15/02G01N23/223G21C17/06
    • G01B15/02
    • PURPOSE:To perform nondestructive measurement, by irradiating X rays from the inside of a coating pipe, generating the characteristic X rays of component other than zirconium among the component of zircaloy, measuring the X rays by a detector, and obtaining the thickness of a linter from the relationship with the attenuation factor of the characteristic X rays. CONSTITUTION:A liner 2 comprising pure zirconium is provided on the inner surface of a coating pipe 1 comprising a zircaloy alloy. An X ray source 3 and X ray detector 4 are arranged in the coating pipe 1. An Am-241 radiation source 6, which is provided in the X ray source 3 radiates gamma rays, excites zirconium target 7, and generates characteristic KX rays 8. The rays are irradiated on the coating pipe 1 from a radiating port 5a. Then only component elements Fe, Cr, and Ni other than zirconium in the zircaloy alloy generate characteristic X rays 9. The characteristic X rays 9 are transmitted through a liner 2 and inputted in the X ray detector 4. The characteristic X rays 9 are attenuated when they are transmitted through the liner 2. Since the relationship between the attenuation factor and the thickness of the liner is known, the attenuation factor is obtained from the output of the X ray detector 4, and the thickness of the liner is obtained from this factor.
    • 目的:进行非破坏性测量,通过从涂层管内照射X射线,在锆石组分中产生除锆以外的成分的特征X射线,用检测器测量X射线,并获得短绒的厚度 从与特征X射线的衰减因子的关系。 构成:包含纯锆的衬里2设置在包括锆石合金的涂覆管1的内表面上。 X射线源3和X射线检测器4布置在涂覆管1中。设置在X射线源3中的Am-241辐射源6辐射伽马射线,激发锆靶7,并产生特征KX射线8 射线从辐射口5a照射在涂布管1上。 然后,在锆石合金中只有组分元素Fe,Cr和Ni以外的锆产生特征X射线9.特征X射线9通过衬垫2透射并输入到X射线检测器4中。特征X射线9被衰减 由于衰减因子与衬垫的厚度之间的关系是已知的,所以衰减系数是从X射线检测器4的输出获得的,并且衬垫的厚度由此获得 因子。
    • 6. 发明专利
    • METHOD AND APPARATUS FOR NONDESTRUCTIVE ANALYSIS OF IODINE
    • JPH0875681A
    • 1996-03-22
    • JP21475594
    • 1994-09-08
    • TOSHIBA CORP
    • TAMURA TOSHIYUKIIGARASHI NOBORUHIRAYAMA FUMIO
    • G01N23/222
    • PURPOSE: To provide a device, which can be conveyed and set into an iodine adsorbing device that cannot be moved, can discriminate other components of radioactive product that coexists with the iodine and has a high analysis accuracy. CONSTITUTION: A material under inspection 1 is arranged in front of a neutron irradiating mechanism 2, and the neutrons are irradiated for the specified time. Then, the material under inspection 1 is moved to front part of a gamma-ray detecting mechanism 3 with a moving mechanism for the material under inspection. The gamma rays emitted from the material under inspection are detected and measured with a gamma-ray detector 10. The time from the end of the irradiation of the neutrons to the start of the detection of the gamma rays is set at the constant time including the moving time. Basically, cooling is performed for 10 minutes, and the attenuation for 2.4 minutes is allowed for the case of Ag-108. The gamma ray of 536KeV discharged from I-130m having the half-life of 9.16 minutes are noted, and the spectrometry measurement of the gammarays is performed.
    • 8. 发明专利
    • METHOD FOR MEASURING CONCENTRATION OF ELEMENT
    • JPH02249960A
    • 1990-10-05
    • JP1410489
    • 1989-01-25
    • TOSHIBA CORP
    • KAWAI AKIOTAMURA TOSHIYUKITSUNODA AKIO
    • G01N23/06
    • PURPOSE:To effectively utilize measurement data and to improve the accuracy of an analysis by calculating the power value to be substd. with an unfixed coefft. in such a manner that a model function attains a optimum regression curve function and determining the concn. of the element to be measured. CONSTITUTION:The term having the mass absorption coefft. of the element to be measured which is the constant intrinsic to every energy of photons or the product of the total sectional areas of the photons and the concn. of the element to be measured which is the unfixed coefft. is subtracted from the term which does not contain the concn. of the element to be measured and is continuous and smooth with the energy of the photons. The value to be substd. with the unfixed coefft. is calculated in such a manner that the model function attains the optimum regression curve function with respect to the relative count rate or relative transmittance measured with the resulted difference as the model function and the energy of the photons transmitting the measuring sample contg. the element to be measured as a parameter.
    • 10. 发明专利
    • Spent fuel inspection device
    • 空气燃料检测装置
    • JP2003004888A
    • 2003-01-08
    • JP2001182540
    • 2001-06-15
    • Central Res Inst Of Electric Power IndToshiba Corp株式会社東芝財団法人電力中央研究所
    • TAMURA TOSHIYUKIGOTO TETSUOMATSUMURA TETSUO
    • G21C17/07G01T1/167G01T1/29G21C19/32G21F5/12
    • PROBLEM TO BE SOLVED: To raise detection sensitivity of gamma ray emitted by radioactive gas such as Kr-85 and improve quantification accuracy by suppressing the incidence into a detector, of background gamma ray such as scattered gamma ray to be a disturbance of measurement.
      SOLUTION: A spent fuel storage vessel 1 storing spent fuel, an inspection shield body 2 covering the spent fuel storage vessel and a gamma ray detector are provided. The gamma ray radiated out of the radioactive gas to a measurement space set near the fuel in the spent fuel storage vessel is measured with the gamma ray detector through a collimator built in the shield body. In a position in the measurement space 8 excluding the region that the collimator 10 views, a gamma ray shield member 14 is provided. Nearby the wall of the spent fuel storage vessel in the region the collimator 10 views, magnetic field devices 16 and 17 for a positron reflection are placed so that the magnetic field is arranged vertical to the collimator direction.
      COPYRIGHT: (C)2003,JPO
    • 要解决的问题:为了提高诸如Kr-85的放射性气体发射的γ射线的检测灵敏度,并且通过抑制入射到检测器中的诸如散射伽马射线的背景伽马射线成为测量干扰来提高定量精度。 解决方案:提供储存乏燃料的乏燃料储存容器1,覆盖乏燃料储存容器的检查屏蔽体2和伽马射线检测器。 通过伽马射线检测器通过内置在屏蔽体内的准直仪测量从放射性气体辐射出的伽马射线到设在废燃料存储容器内的燃料附近的测量空间。 在除了准直仪10所看到的区域之外的测量空间8中的位置,设置有伽马射线屏蔽构件14。 在准直器10所看到的区域中,在废燃料存储容器的壁附近,放置用于正电子反射的磁场装置16和17,使得磁场垂直于准直器方向排列。