scholarly journals Thermophoretic force on nanoparticles in free molecule regime

2021 ◽  
Vol 0 (0) ◽  
pp. 0-0
Author(s):  
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Author(s):  
Jun Wang ◽  
Guodong Xia

The thermophoresis of nanoparticles in the free molecule regime plays an important role in the nucleation, collision and coagulation of nanoparticles. In this contribution, on the basis of a rigorous gas kinetic theory, the theoretical expressions for the thermophoretic force on nanoparticles suspended in dilute gas mixtures are derived, wherein the non-rigid-body interactions between the gas molecules and the nanoparticle are taken into account. The analytical formulas in the present work are consistent with those under the rigid-body collision assumption. Negative thermophoresis, is found to be possible for nanoparticles in the free molecule regime, by which the thermophoretic force exerted on the suspended nanoparticle is from low to high temperature, i.e., opposite to the direction of normal thermophoresis.



2018 ◽  
Vol 97 (5) ◽  
Author(s):  
Song Yu ◽  
Jun Wang ◽  
Guodong Xia ◽  
Luxiang Zong


2017 ◽  
Vol 95 (3) ◽  
Author(s):  
Jun Wang ◽  
Shuang Luo ◽  
Guodong Xia






2002 ◽  
Author(s):  
Andrew Ketsdever
Keyword(s):  




1996 ◽  
Vol 104 (9) ◽  
pp. 3329-3337
Author(s):  
P. Zieliński ◽  
M. More ◽  
E. Cochon ◽  
J. Lefebvre


An experimental study has been made of the gaseous drag torque on an isolated sphere rotating at high Mach numbers. The sphere was suspended electromagnetically and spun by induction. The drag torque has been measured through the transition régime from continuum to free molecule flow at Mach numbers (based on equatorial speed) of up to about five. These high Mach numbers were achieved in heavy vapours (diiodomethane, germanium tetrabromide and stannic bromide) with sonic speed as little as a quarter of that in air. To measure the pressure in the vapour a second (smaller) rotating sphere was used as a pressure gauge. The results agree well with those previously obtained and show an unexpected Mach number dependence in the transition régime.



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