Particle Separations by Filtration and Sedimentation

Author(s):  
Steve Tarleton ◽  
Richard Wakeman
Keyword(s):  
1984 ◽  
Vol 19 (11-12) ◽  
pp. 783-800 ◽  
Author(s):  
L. A. Kaye ◽  
R. J. Fiocco

2007 ◽  
Vol 342-343 ◽  
pp. 637-640
Author(s):  
Sang Heum Youn ◽  
Z. X. Yang ◽  
Kyu Hong Hwang ◽  
Jong Kook Lee ◽  
Seog Young Yoon

Particle separations occurred frequently in sintered hydroxyapatite when immersed in distilled water or simulated body fluid. This dissolution initiated at grain boundary creating nano-size defects such as small pores and grew up to micro scale by increasing immersion time. The dissolution, probably due to the appearance of secondary phases in grain boundary, resulted in grain separation at the surfaces and finally in degradation and fracture. And the dissolution concentrated on those grains adjacent to pores rather than those in the dense region. Hydroxyapatite ceramics incorporated with calcium silicate glass were prepared by slip casting to enhance the sinterability as well as to reduce dissolution. Glass phase was incorporated into hydroxyapatite to act as sintering aids followed by crystallization in order to improve the mechanical properties without reducing biocompatibility. From dissolution test, significant damage was reduced even more than 7 days and the dissolution pattern somewhat changed than pure hydroxyapatite. X-ray diffraction and SEM showed no decomposition of secondary phases in grain boundary and fracture toughness somewhat increased.


1998 ◽  
Vol 22 (3) ◽  
pp. 351-356 ◽  
Author(s):  
Sabine M. Agena ◽  
I.David L. Bogle ◽  
Alan R.H. Cornish

1969 ◽  
Vol 3 (1) ◽  
pp. 107-118 ◽  
Author(s):  
C. J. Myerscough

The approximations usually made to truncate the BBGKY hierarchy for a plasma are discussed; their failure at small inter-particle separations leads to divergence of the Balescu—Lenard collision integral. A number of authors have obtained convergent kinetic equations, often by rather complicated methods.It is shown here that, if the standard truncation procedure is modified in a way which makes it less obviously inconsistent for close approaches, the standard methods maybe closely followed in deriving a convergent collision integral which agrees to dominant order with the ‘cutoff’ Balescu—Lenard integral and with the other work on the problem. In fact, the kinetic equation obtained is identical with the Balescu—Lenard equation except that the Coulomb potential is replaced by another that is non-singular at the origin. A physical interpretation of this result is suggested.


2018 ◽  
Vol 90 (3) ◽  
pp. 1827-1835 ◽  
Author(s):  
Jeong-ah Kim ◽  
Je-Ryung Lee ◽  
Tae-Jin Je ◽  
Eun-chae Jeon ◽  
Wonhee Lee

Author(s):  
Yun Chen ◽  
Souran Manoochehri

This paper presents the optimal design of electrode structure and microfluidics channel for effective particle separations. The purpose of the microfluidics chip is to generate the DEP (dielectrophoresis) force within the micro channel to separate both negative DEP (nDEP) and positive DEP (pDEP) particles of same sizes. The particles will experience DEP force when passing through the electric field created by electrode arrays located in different positions within the channel. The channel contains several electrode arrays where the pDEP particles are moved away from the electrodes and the nDEP particles are attracted towards them. In some existing microfluidics chips, because of the high intensity of the electric field around the electrodes, which results in a very high DEP force near the electrodes, most of the positive DEP particles are captured in the space between electrodes without being guided to the target outlet. Moreover, the effective area of DEP force is limited to a small region near the corner of the electrodes, therefore only those particles very close to the electrodes will experience sufficient attractive forces to be guided towards the target locations. This will decrease the efficiency of the particle separation. In this study, we developed an optimization methodology for design of electrode configurations using numerical modeling. The optimized electrode structure can provide much more evenly distributed DEP field. The design of the channel, the number and position of the electrode arrays were optimized in order to improve the efficiency of the particle separation. Finally, the optimized electrode structure and microfluidics channel were modeled and tested using multiphysics simulation software and the results show that this optimized design of microfluidics channel can provide high throughput and more effectiveness for particle separation compared to many existing microfluidics devices.


2017 ◽  
Vol 252 ◽  
pp. 606-615 ◽  
Author(s):  
P.Y. Yeh ◽  
Z. Dai ◽  
X. Yang ◽  
M. Bergeron ◽  
Z. Zhang ◽  
...  

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