scholarly journals On the Particle Cut Size of Cyclone Dust Collector. (Part4). Separation Grain Size Ratio as a Function of the Froude Number.

1991 ◽  
Vol 28 (7) ◽  
pp. 437-442
Author(s):  
Kikaku IKEMORI
2014 ◽  
Vol 2 (10(68)) ◽  
pp. 11
Author(s):  
Дмитро Олександрович Серебрянський ◽  
Сергій Володимирович Плашихін ◽  
Юрій Олександрович Безносик ◽  
Олександр Миколайович Набок

Author(s):  
Masayoshi OZAWA ◽  
Haruki TAKAHASHI ◽  
Toshihiko SHIMIZU ◽  
Masahiko SAKAI ◽  
Tadahiro OYAMA

1983 ◽  
Vol 20 (4) ◽  
pp. 587-602 ◽  
Author(s):  
David C. Sego ◽  
Norbert R. Morgenstern

This study confirms the existence of two flow laws for polycrystalline ice. One describes the behaviour of ice before the inflection point of a constant stress test, and one the behaviour well into the tertiary portion of the strain–time curve. Each flow law may be represented by a power law with an exponent of 3.0.The inflection point in constant stress experiments and the peak in constant strain rate experiments is shown to occur at about 1% strain in experiments conducted in the ductile material behaviour range. A Cottrell–Aytekin relationship has been used to fit the strain–time material behaviour up to the inflection point.The flow law of ice valid below 1% strain is shown to be dependent on the grain size ratio of the ice. The grain size ratio is a measure of the size effect of the sample tested. The temperature influence on the flow law is best described by using the inverse temperature relationship described by Voytkovskiy. Keywords: ice, creep deformation, long-term, failure strain.


Geomorphology ◽  
2017 ◽  
Vol 278 ◽  
pp. 314-328 ◽  
Author(s):  
Franziska Staudt ◽  
Julia C. Mullarney ◽  
Conrad A. Pilditch ◽  
Katrin Huhn
Keyword(s):  

Author(s):  
Shoji Hayashi ◽  
Masatoshi Watanabe ◽  
Yukiji Iwase ◽  
Kyoichi Kanno ◽  
Keiichi Fujimori

A household vacuum cleaner named “Tatsumaki cyclone” with a new cyclone dust collector was developed. It has a unique horizontal layout called the inverted cyclone layout that features a dust bunker adjacent to a cyclone cylinder with an up-draught airflow. It also has a new airflow arrangement called triple-suction airflow that separates airflow after removing dust at the cyclone cylinder. The main suction airflow is exhausted from the main port (which is downstream of the cyclone cylinder) through an inner cylinder. The sub-suction airflow is exhausted from the dust bunker after it heavily compresses the dust (sub port). The center suction airflow is exhausted from the center port. In this study, we used the Cartesian grid system to simulate the flow field inside the dust collector. This system uses only rectangular parallelepiped meshes; profiles of the dust collector were represented by stepped surfaces of cubic meshes. Each mesh was generated based on whether it was inside or outside the solid body of the dust collector. High-performance computers have recently been used to help generate super-fine meshes that fit closely the smooth shape of a dust collector. The Cartesian grid system has the advantage of being able to quickly generate square-meshes of complex shape that can be converted directly from the CAD data. We simulated the velocity distribution of single-suction, twin-suction and triple-suction models. The single-suction model had only a main port to exhaust airflow, the twin-suction model had a main port, and a sub port, and the triple-suction model had a main port, a sub port, and a center port. In this study, a Cartesian grid system with a finite difference method was used to correct the unsteady three-dimensional flows. After the simulation, we experimented with pressure losses and measured change in air quantity by the dust load of each model. These steps enabled us to develop a new cyclone dust collector called Tatsumaki cyclone as part of a compact household vacuum cleaner with lower pressure loss and a larger capacity dust bunker.


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