Title: 6%20Life%20in%20a%20Fluid%20Medium
16 Life in a Fluid Medium
2CONSIDER FLUID MOVING IN STREAMLINES Water
flow can be visualized as streamlines Particles
entrained in flow move with streamlines and do
not cross
3Streamline
Cylinder (in cross section)
4Some important properties of fluids Density ??
units of g cm-3 Dynamic viscosity ??molecular
stickiness, units of (force x
time)/area Kinematic Viscosity ???gooeyness or
how easily it flows, how likely is to break out
in a rash of vortices, units of
(length2/time) Kinematic viscosity dynamic
viscosity/density
5Properties of Some Common Fluids
6Reynolds Number, Re measure of relative
importance of viscous and inertial forces in fluid
Note that we are always working with seawater, so
we Consider no variation in ? or ???Therefore we
conclude That Re increases with velocity V and
size of object l
7ERROR IN TEXT!
- Pg. 138 SHOULD READ
- ..divided by kinematic viscosity..
8We can make a calculation of Re if an object is
moving in water or stationary, with the water
moving past the object.
9Reynolds numbers for a range of
swimming organisms and sperm
ANIMAL AND VELOCITY Re
Large whale swimming at 10 m/s 300,000,000
Tuna swimming at 10 m/s 30,000,000
Copepod swimming at 20 cm/s 30,000
Sea urchin sperm at 0.2 mm/s 0.03
10Reynolds number implications
- Re gt 1000 inertial forces predominate
- Re lt 1 viscous forces predominate
11Reynolds number implications 2
- Re gt 1000 inertial forces predominate
- Re lt 1 viscous forces predominate
- World of very small size and velocity is a
viscous world takes continuous work to move an
object at this Re range particles will stop
moving when no work exerted (e.g., ciliate can
stop instantaneously and reverse direction by
simply stopping waving of external cilia)
12Reynolds number implications 3
- Re gt 1000 inertial forces predominate
- Re lt 1 viscous forces predominate
- World of very small size and velocity is a
viscous world takes continuous work to move an
object at this Re range particles will stop
moving when no work exerted (e.g., ciliate can
stop instantaeously and reverse direction by
simply stopping waving of external cilia) - World of large size and high velocity is an
inertial world if work is done, object will tend
to continue to move in fluid (e.g., supertanker
at full speed will continue to move several km
after propulsive power shut off)
13Laminar versus turbulent flow
- Laminar flow - streamlines are all parallel, flow
is very regular - Turbulent flow - streamlines irregular to chaotic
- In a pipe, laminar flow changes to turbulent flow
when pipe diameter increases, velocity increases,
or fluid density increases beyond a certain point
14Laminar versus turbulent flow
15Water Moving Over a Surface
- Well above the surface the water will flow at a
mainstream velocity - But, at the surface, the velocity will be zero.
This is known as the no-slip condition - From the surface to the mainstream, there is a
transition zone, known as the boundary layer - The boundary layer, defined as zone near surface
where velocity is gt 1 less than the mainstream
current, increases in thickness as the mainstream
current velocity increases
16Water Moving Over a Surface 2
- Well above the surface the water will flow at a
mainstream velocity - But, at the surface, the velocity will be zero.
This is known as the no-slip condition. - From the surface to the mainstream, there is a
transition zone, known as the boundary layer - The boundary layer, defined as zone near surface
where velocity is gt 1 less than the mainstream
current, increases in thickness as the mainstream
current velocity increases
17Boundary layer
Bottom surface
18Principle of Continuity
- Assume fluid is incompressible and moving through
a pipe
19Principle of Continuity 2
- Assume fluid is incompressible and moving through
a pipe - What comes in must go out!
20Principle of Continuity 3
- Assume fluid is incompressible and moving through
a pipe - What comes in must go out!
- Velocity of fluid through pipe is inversely
proportional to cross section of pipe.
21Principle of Continuity 4
- Assume fluid is incompressible and moving through
a pipe - What comes in must go out!
- Velocity of fluid through pipe is inversely
proportional to cross section of pipe. - Example If diameter of pipe is doubled, velocity
of fluid will be reduced by half
22Principle of Continuity 5
- Assume fluid is incompressible and moving through
a pipe - What comes in must go out!
- Velocity of fluid through pipe is inversely
proportional to cross section of pipe. - Example If diameter of pipe is doubled, velocity
of fluid will be reduced by half - Principle applies to a single pipe, but it also
applies to the case where a pipe splits into
several equal subsections. Product of velocity
and cross sectional area sum of products of all
the velocity and sum of cross-sectional areas of
smaller pipes.
23Principle of continuity
24Continuity, Applied to Sponge Pumping
- Sponges consist of networks of chambers, lined
with cells called choanocytes - Velocity of exit current can be 10 cm/s
- But, velocity generated by choanocytes is 50 ?m
per sec. How do they generate such a high exit
velocity? - Answer is in cross-sectional area of choanocytes,
whose total cross-sectional area are thousands of
times greater than the cross section of the exit
current areas.
25Flagellated chamber
Exit current
Choanocytes
The low velocity of the water from flagellated
choanocyte cells in flagellated chambers is
compensated by the far greater total cross-section
al area of the flagellated chambers, relative to
the exit current opening of the sponge
26Bernoullis Principle
- Pressure varies inversely with the velocity of
the fluid
Upper air stream
Wing moving
Lower air stream
27Bernoullis Principle 2
- Pressure varies inversely with the velocity of
the fluid - Means that pressure gradients can be generated by
different velocities in different areas on a
surface
Upper air stream
Wing moving
Lower air stream
28Bernoullis Principle 3
- Pressure varies inversely with the velocity of
the fluid - Means that pressure gradients can be generated by
different velocities in different areas on a
surface - Example Top surface of a wing has stronger
curvature than bottom of wing, air travels faster
on top, pressure is lower, which generates lift.
Upper air stream
Wing moving
Lower air stream
29Worm
Burrow
Bernoullis Principle Top Difference below and
above flatfish creates lift. Bottom Raised
burrow entrance on right places it in faster
flow, which creates pressure gradient and flow
through burrow.
30Drag
- Water moving past an object creates drag
- At high Reynolds number, the pressure difference
up and downstream explains the pressure drag.
Streamlining and placing the long axis of a
structure parallel to the flow will both reduce
pressure drag - At low Reynolds number, the interaction of the
surface with the flow creates skin friction.
31Drag and fish form. The left hand fish is
streamlined and creates relatively little
pressure drag while swimming. the right hand fish
is more disk shaped and vortices are created
behind the fish, which creates a pressure
difference and, therefore, increased pressure
drag. This disk shape, however, allows the fish
to rapidly turn.
32Sessile Forms - how to reduce drag?
- Problem You are attached to the bottom and
sticking into the current - Drag tends to push you down stream - you might
snap! - Examples Seaweeds, corals
- Solutions
- Flexibility - bend over in current
- Grow into current
- 3. Strengthen body (some seaweeds have
crossweaving)
33The End