Flows of molecular fluids in nano- structured channels

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Lennard-Jones fluids ARGON: ε/k B =120 K σ = 3.405 A τ = 10 fs r c – cutoff in the potential r c =2.2σ
Interactions with the wall atoms controlled by A - - The channel geometry A=1 strongly attractive or strongly wetting A=0 purely repulsive or non-wetting Knudsen regime Discuss first homogeneous, then patterned walls
Page 1 and 2: Flows of molecular fluids in nanost
Page 3 and 4: Situations that require molecular-l
Page 5 and 6: How does the slip length depend on
Page 7 and 8: microfluidics and nanofluidics “l
Page 9: E-NOSE Detection and monitoring of
Page 13 and 14: Atoms sent normally towards to wall
Page 15: Double the width of the channel v x
Page 19 and 20: The slip length for various values
Page 21 and 22: Variations in the velocity profile
Page 24 and 25: A non-wetting droplet at T/ε=0.8 1
Page 26 and 27: Barthlott & Nienhuis 1997: ‘Purit
Page 28 and 29: Gecko hair (setae) is tiny and faci
Page 30 and 31: GEOMETRICAL PATTERNING very differe
Page 32 and 33: Faster motion at the marginal value
Page 34 and 35: Evaporation of a droplet on a tempe
Page 36 and 37: A moving droplet - molecular combin
Page 38 and 39: CONCLUSIONS Molecular dynamics stud
Page 40 and 41: Molecular Dynamics: fixed volume V
Page 42 and 43: X = x i Xm = x (m) i (Δt)m /m! The
Page 44 and 45: Velocity profiles change little alo
Page 46 and 47: A=1/4 sticks Location of the center
Page 48 and 49: THERMAL SLIP

Flows of molecular fluids in nano- structured channels

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