Dynamic Forces Fig. from Warrick et al. 2005. Nature.

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Dynamic Forces Fig. from Warrick et al. 2005. Na

Transcript of Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Page 1: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Dynamic Forces

Fig. from Warrick et al. 2005. Nature

Page 2: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Solids vs. Fluids

Solids resist shear deformation: they care how far they are

deformed

Fluids care about how rapidly they are deformed: rate of shear

F/S = GF/S = (/t)

Dynamic viscosity

Rate of shearShear modulus

SF

Shear strain

Page 3: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

No-slip condition & Boundary layer

FS

U

z(F/S) = (U/z)

Lingulodinium polyedrum

Page 4: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Viscosity

F SU

z

F/S = (/t)

Viscosity is a measure of the resistance to rate of shear

Page 5: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Physical coupling of temperature and viscosity

Viscosity of water has a sever dependence on temperature(Viscosity doubles from 30 to 5ºC)

Page 6: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Temperature effects on viscosity

Q’ = CJΔT

* More viscous blood should flow more slowly

* Slower mass flow can minimize heat loss

Page 7: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Temperature effects on viscosity

Leopard Seal

Weddell Seal

Crabeater Seal

Blood viscosity triples as temperature decreases (38 - 3ºC)

Page 8: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Principle of Continuity

A1V1 = A2V2

Page 9: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Principle of Continuity: example

200 mm s-1

1 mm s-15.7 x 104 mm2

200 mm2

Total Area Flow speedAorta

Capillaries

Page 10: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Principle of Continuity: example

Page 11: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Continuity in flow fields

The principle of continuity must apply between a pair of streamlines

Narrow streamlines

A1V1 = A2V2

Page 12: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Static Pressure

• Pressure exerted in all directions by a fluid at rest

• Measurable pressure when fluid is brought to a halt

Δp = ½ρU2

Dynamic Pressure

Δp

U

Page 13: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Bernoulli’s Principle

Pressure Drop = ρgh

P1+ ½ ρV1 = P2 + ½ρV2

Fluid has a local static and dynamic pressure: the sum of these is constant

Page 14: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Bowhead Whale:Continuous filter feeder

(Werth 2004, J. Exp. Biol. )

Anterior Opening

Posterior Opening

Page 15: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Venturi manometerShowing pressure drop

ΔP = ρu2/(1-A12/A2

2)

A2A1

A1A2

A1 A2

Bernoulli:

Pressure drop (Werth 2004, J. Exp. Biol. )

Page 16: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Difference in dynamic pressure creates drag

• Flow is redirected around the body, flow is robbed of its momentum• Momentum lost in wake (eventually in the form of heat)

Momentum = mU

Dynamic pressure = ½ ρU2

1.0

0.5

0Cp

-0.5

Cp = Measured pressureDynamic pressure

ΔP → Drag

Page 17: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Difference in dynamic pressure can also create lift

No lift, little drag Lift, Little Drag Stall: Lift & Drag

FL = ½ CLSρU2

Fluid separates from surface: vortices & eddies are generated

Page 18: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Vortex shedding caused by flow past a flat plate

Page 19: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Vortex Street

st = StU/D

Frequency of Vortex Shedding

Strouhal Number(non-dimensional)

Diameter

Page 20: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

1. Drag = mass x acceleration

3. Energy expenditure or Power = drag x velocity

2. Work against drag = drag x distance

Δt

Δx

Δx

Why drag is important

Thrust = Drag

Page 21: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Drag: resists motion through fluid

D = Fh + Fs + Fw + Fi

Total Drag Hydrodynamic or Pressure Drag

Skin Friction Wave Drag Induced Drag

Total DragThrust

Page 22: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Drag: resists motion through fluid

Fh = ½ CDSρU2

D = Fh + Fs + Fw + Fi

Total Drag Hydrodynamic or Pressure Drag

Skin Friction Wave Drag Induced Drag

US = flow-wise area

Due to separation & ΔP, E is invested in moving fluid around object, but isn’t being returned back to the fluid

Page 23: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Drag: resists motion through fluid

Fs = ½ CDSρU2

D = Fh + Fs + Fw + Fi

Total Drag Hydrodynamic or Pressure Drag

Skin Friction Wave Drag Induced Drag

A = “wetted” surface areaU

A direct consequence of the interlamellar stickiness of fluid

Page 24: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Skin friction vs. Pressure drag

Early separation,high pressure drag

relative to skin friction

Flow remains attached, drag dominated by skin friction

Page 25: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Drag: resists motion through fluid

D = Fh + Fs + Fw + Fi

Total Drag Hydrodynamic or Pressure Drag

Skin Friction Wave Drag Induced Drag

Wave drag occurs near the sea surface

Page 26: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Drag: resists motion through fluid

D = Fh + Fs + Fw + Fi

Total Drag Hydrodynamic or Pressure Drag

Skin Friction Wave Drag Induced Drag

Drag generated by the oscillation of appendages

DragLift

Page 27: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

What is the drag coefficient, CD?

Fh = CdS½ρU2

Dynamic pressure

ProjectedArea

Drag

U

Page 28: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Drag depends on shape:D = CdS½ρU2

0.2 0.4 0.6 0.8 1.0 1.2 1.4Drag coefficient (Cd)

Dynamic pressure

Flow-wise projected area

drag

Page 29: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

CD can get even bigger during unsteady motion

CD → 2.0

(Potvin, SLU)

Page 30: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Drag also depends on scaleReynolds number (Re) =

v = viscosity

νρ = density U = velocityL = length

ρLU

Re

Cd

Low Re Intermediate Re

High Re

D = CdS½ρU2

Page 31: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Life at low Reynolds numbers

• Viscous• Difficult to produce vortices• Efficiency of locomotion

decreases• Many organisms resort to

dragging themselves through the medium

• High Cd

D = CdS½ρU2

Page 32: Dynamic Forces Fig. from Warrick et al. 2005. Nature.

Drag reduction: Convergence on streamlined form

What happens when animals deviate from this ideal form?