scholarly journals Heat Load Measurements on a Large Superconducting Magnet: An Application of a Void Fraction Meter

2004 ◽  
Vol 14 (2) ◽  
pp. 1704-1707 ◽  
Author(s):  
R. Pengo ◽  
N. Dolgetta ◽  
S. Junker ◽  
G. Passardi ◽  
H. tenKate
Author(s):  
Yoshihiro JIZO ◽  
Hidenari AKAGI ◽  
Takashi YAMAGUCHI ◽  
Motoaki TERAI ◽  
Masatoshi SHINOBU

Author(s):  
Hideo TSUCHISHIMA ◽  
Motoaki TERAI ◽  
Hakaru YOSHIDA ◽  
Hiroyuki WATANABE ◽  
Mutsuhiko YAMAJI ◽  
...  

2021 ◽  
pp. 221-221
Author(s):  
de Oliveira ◽  
Machado Ochoski ◽  
Conrado Chiarello ◽  
Dos Nunes ◽  
Silva da ◽  
...  

The thermosyphon is a type of heat exchanger that has been widely used in many applications. The use of thermosyphons has been intensified in recent years, mainly in the manufacture of solar collectors and various industrial activities. A thermosyphon is a vertical sealed tube filled with a working fluid, consisting of, from bottom to top, by an evaporator, an adiabatic section, and a condenser. The study of geyser-boiling phenomena, which occurs inside the thermosyphon is of extreme importance, therefore the experimental analysis of the parameters related to the two-phase flow (liquid-steam), such as void fraction, bubble frequency, bubble velocity, and bubble length are necessary, since these parameters have a significant influence on heat transfer. In this work, a pair of wire mesh sensors was used, a relative innovative technology to obtain experimental values of the reported quantities for measuring these parameters of slug flow in thermosyphons. An experimental setup is assembled and the sensors are coupled to the thermosyphon enabling the development of the experimental procedure. Here is presented an experimental study of a glass thermosyphon instrumented with two Wire-Mesh Sensors, in which the aforementioned slug flow hydrodynamic parameters inherent to the geyser type boiling process are measured. It was measured successfully, as a function of the heat load (110, 120, 130, 140, and 150W), the void fraction (instantly and average), liquid film thickness, translation velocity of the elongated bubbles, lengths of the bubbles, and the liquid slug (displaced by the bubble rise up). It was observed that the higher the heat load, the lower is the bubble translation velocity. For all heat loads, based on the measured length of liquid slug (consequent displacement of liquid volume), caused by bubbles rise from evaporator to condenser, it could be affirmed to some extent that both boiling regime (pool and film) exist in the evaporator. The measured average void fraction (80%) and liquid film thickness (around 2.5mm) during the elongated bubble passages were approximately constant and independent of the heat load.


2000 ◽  
Vol 10 (1) ◽  
pp. 913-916
Author(s):  
H. Matsue ◽  
E. Suzuki ◽  
K. Nemoto ◽  
M. Kurihara ◽  
T. Okino ◽  
...  

Author(s):  
Sha Bai ◽  
Chenghui Yu ◽  
Yiwei Wang ◽  
Jie Gao

With the discovery of the Higgs boson at around 125 GeV, a circular Higgs factory design with high luminosity [Formula: see text] is becoming more popular in the accelerator world. The CEPC project in China is one of them. Machine Detector Interface (MDI) is the key research area in electron–positron colliders, especially in CEPC, since the synchrotron radiation (SR) photons can contribute to the heat load of the beam pipe and radiation dose may damage the components. And the heat load can cause the temperature rise in some part, and if the temperature rise is too high, the beryllium pipe in the interaction region will melt and the superconducting magnet may quench. Thus, the heat load distribution from synchrotron radiation and beam loss in the interaction region are analyzed carefully and results are given in this paper.


1984 ◽  
Vol 45 (C1) ◽  
pp. C1-867-C1-870
Author(s):  
A. M. Hatch ◽  
P. G. Marston ◽  
R. J. Thome ◽  
A. M. Dawson ◽  
W. G. Langton ◽  
...  

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