physics in fluid mechanics sunghwan (sunny) jung 정승환 applied mathematics laboratory courant...
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Physics in Fluid Mechanics
Sunghwan (Sunny) Jung 정승환
Applied Mathematics LaboratoryCourant Institute, New York University
Surface waves on a semi-toroidal ring
Sunghwan (Sunny) JungErica Kim Michael Shelley
Motivation Faraday (1831) - wave formation due to vibration Benjamin & Ursell (1954) - stability analysis
Vertically vibrated
Other geometries of the water surface Quasi-one dimensional surface wave
Vertically vibrated
Vibrating a pool Vibrating a bead
Hydrophobic Materials
Hydrophobic Surface
4 mm1 mm
Hydrophobic Surface
Hydrophobic Surface
Glass SurfaceContact Angle ~ 150O
Experimental Setup
Hydrophobic surfaces
3 cm
1 cm
Speaker
Glass
3 cm
1 cm
3 cm
1 cm
Standing Surface Waves
Coordinate for Water Surface
(m = 2) mode along
Neglect the small curvature along the torus ring.
Surface waves in a water ring
Balance b/t pressure and surface tension
Potential flow
Kinematic boundary condition
pressure, stress and gravitation
Mathieu Equation
In the presence of viscosity, the dominant response frequency is
where is the external frequency.
Stability
k : wavenumber along a toroidal tubea : nondimensionalized vibrating acceleration
Frequency Response
Conclusion
Our novel experimental technique can extend the study of surface waves on any geometry.
We studied a surface wave on a semi-toroidal ring.
Applicable to the industry for a local spray cooling.
Locomotion of Micro-organism
Sunghwan (Sunny) JungErika KimMichael Shelley
Various Bio-Locomotions
• Flagellar locomotion
• Ciliary locomotion
• Muscle-undulatory locomotion
C. Elegans (Nematode)
1 mm
• Length is 1 mm and thickness is 60 μm. • Consists of 959 cells and 300 neurons• Swim with sinusoidal body-waves
Thickness ~ 60 μm
On the plate
In water
• Bending Energy
• Force
where is the curvature of the slender body and
is the coordinate along the slender body
In a simulation
In the high viscous fluid In the low viscous fluid
In a 200 micro meter channel
In a 300 micro meter channel
Swimming C. Elegans
Swimming velocity increases as the width of walls decreases.
Amplitude in both cases is similar.
Effect of nearby boundaries
C. Elegans swim faster with a narrow channel.
Effect of nearby boundaries
As the nematode is close to the boundary, decreases.
Fs Fn
=> It gains more thrust force in the presence of the boundary.(Brennen, 1962)
Conclusion Simple argument explains why C.
Elegans can not swim efficiently in the low viscous fluid.
C. Elegans are more eligible to swim when the boundary exists.
Periodic Parachutes in Viscous Fluid
Sunghwan (Sunny) JungKarishma ParikhMichael Shelley
Why do they rotate?
Shear Flow
T = 0 T = t
Thanks to
Prof. Michael Shelley, Steve Childress (Courant Institute) Prof. Jun Zhang (Phy. Dep., NYU)
Dr. David Hu
Erica Kim, Karishma Parikh
Prof. Albert Libchaber (Rockefeller Univ.)Prof. Lisa Fauci (Tulane Univ.)
Future works
Interaction among helixes Microfluidic pump using Marangoni
stress
Cilia
Why do cells move? Is there any advantage in being motile?
•Microbial locomotion.
•Flagella and motility.
•Different flagellar arrangements.
Energy expenditure
Peritrichous
Polar
Lophotrichous
Wavelength, flagellin.
Flagellar structure: the hook and the motor.
Flagella
Swimming E. Coli
Manner of movement in peritrichously flagellated prokaryotes. (a) Peritrichous: Forward motion is imparted by all flagella rotating counterclockwise (CCW) in a bundle. Clockwise (CW) rotation causes the cell to tumble, and then a return to counterclockwise rotation leads the cell off in a new direction.