Application of FBG three-dimensional stress sensor in similar simulation experiment of mining

Author(s):  
Shiming Wei ◽  
Zesheng Zhang ◽  
Liqiang Zhang
2011 ◽  
Vol 26 ◽  
pp. 431-440 ◽  
Author(s):  
Liu Feifei ◽  
Lin Baiquan ◽  
Zhai Cheng ◽  
Li Ziwen ◽  
Li Fei ◽  
...  

Author(s):  
Mitsuhiro Suzuki ◽  
Takeshi Takeda ◽  
Hideo Nakamura

Presented are experiment results of the Large Scale Test Facility (LSTF) conducted at the Japan Atomic Energy Agency (JAEA) with a focus on core exit thermocouple (CET) performance to detect core overheat during a vessel top break loss-of-coolant accident (LOCA) simulation experiment. The CET temperatures are used to start accident management (AM) action to quickly depressurize steam generator (SG) secondary sides in case of core temperature excursion. Test 6-1 is the first test of the OECD/NEA ROSA Project started in 2005, simulating withdraw of a control rod drive mechanism penetration nozzle at the vessel top head. The break size is equivalent to 1.9% cold leg break. The AM action was initiated when CET temperature rose up to 623K. There was no reflux water fallback onto the CETs during the core heat-up period. The core overheat, however, was detected with a time delay of about 230s. In addition, a large temperature discrepancy was observed between the CETs and the hottest core region. This paper clarifies the reasons of time delay and temperature discrepancy between the CETs and heated core during boil-off including three-dimensional steam flows in the core and core exit. The paper discusses applicability of the LSTF CET performance to pressurized water reactor (PWR) conditions and a possibility of alternative indicators for earlier AM action than in Test 6-1 is studied by using symptom-based plant parameters such as a reactor vessel water level detection.


Atmosphere ◽  
2020 ◽  
Vol 11 (12) ◽  
pp. 1312
Author(s):  
Yue Wu ◽  
Zheng Sheng ◽  
Xinjie Zuo ◽  
Minghao Yang

Falling-sphere sounding remains an important method for in situ determination in the middle atmosphere and is the only determination method within the altitude range of 60–100 km. Traditional single-falling-sphere sounding indicates only the atmospheric density and horizontal wind but not the vertical wind; the fundamental reason is that the equation set for retrieving atmospheric parameters is underdetermined. For tractability, previous studies assumed the vertical wind, which is much smaller than the horizontal wind, to be small or zero. Obtaining vertical wind profiles necessitates making the equations positive definite or overdetermined. An overdetermined equation set consisting of six equations, by which the optimal solution of density and three-dimensional wind can be obtained, can be established by the double-falling-sphere method. Hence, a simulation experiment is designed to retrieve the atmospheric density and three-dimensional wind field by double falling spheres. In the inversion results of the simulation experiment, the retrieved density is consistent with the constructed atmospheric density in magnitude; the density deviation rate does not generally exceed 20% (less than 5% below 60 km). The atmospheric density retrieved by the double-falling-sphere method is more accurate at low altitudes than the single-falling-sphere method. The vertical wind below 50 km and horizontal wind retrieved by double-falling-sphere method is highly consistent with the constructed average wind field. Additionally, the wind field deviation formula is deduced. These results establish the fact that the double-falling-sphere method is effective in detecting atmospheric density and three-dimensional wind.


2018 ◽  
Vol 18 (19) ◽  
pp. 7956-7963 ◽  
Author(s):  
Jiayi Yang ◽  
Xiaoping Li ◽  
Xiaozhou Lu ◽  
Weimin Bao ◽  
Renjie Chen

2012 ◽  
Vol 455-456 ◽  
pp. 204-210
Author(s):  
Guo Wang ◽  
Xi Min Cui ◽  
De Bao Yuan ◽  
Ya Hui Qiu ◽  
Jin Lin Yang ◽  
...  

In the two-dimensional experiment of similar material simulation, three-dimensional coordinate data obtained by total station should be conversed to the coordinate system which is concerned in the experiment.When using bursa-wolf model to converse coordinate,the three rotation parameters should be linearized,which will affect the accuracy of coordinate conversion if the three rotation parameters are big.In this paper,it is researched that using an antisymmetric matrix which is consist of three separate parameters to substitute for the three rotation parameters,and then the lodrigues matrix is composed from the antisymmetric matrix. Conversion results showed that: By introducing of lodrigues matrix, not only the algorithm becomes simple but also the coordinate transformation precision is improved.


2020 ◽  
Vol 15 (1) ◽  
pp. 24-41
Author(s):  
Andrey V. Arzhannikov ◽  
Denis A. Samtsov ◽  
Stanislav L. Sinitsky ◽  
Vasily D. Stepanov

The paper presents the results of numerical simulation and experimental studies of the generation of two ribbon beams in an accelerating diode with magnetic insulation at a diode voltage of ~ 0.7 MeV and a current of 10 kA in it. Model-ing is implemented using the Particle CST Studio package. The experiments were conducted on the U-3 accelerator of the ELMI installation. In calculations with three-dimensional geometry corresponding to the experiments, the distribu-tion of electron velocities over the pitch angle at the exit of the beams from the diode under the conditions of an inho-mogeneous magnetic field with an induction of about 1 T was obtained. These calculated data were confirmed in an experiment in which, using a sensor with seven recording channels, a distribution function of the velocity of electrons with a characteristic width at half maximum of 0.03 rad was obtained. Using the GEANT4 software package in processing measurement results with this sensor gives confidence in the correctness of the obtained distribution function.


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