Fluids: statics and dynamics

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Fluids: statics and dynamics

In class Quiz #25-5

Suppose superman has infinite strength.

How high can he suck the liquid up?

(density of liquid is  )

1.

2.

3.

h = infinity h = 9.8 m h = P

0

/  g

Question from class:

Why can trees grow higher than 10 m?

http://ptonline.aip.org/journals/doc/PHTOAD-ft/vol_61/iss_1/76_1.shtml

Why can trees grow higher than 10 m?

Effective pore diameter inside leaves is 5-10 nm

(spacing between cellulose microfibrils)

Height of capillary water column with 10nm diameter is 3 km!

Why aren’t trees taller?

A: friction, bubbles

Capillary force

(electrostatic attraction of water to glass)

Redwood in CA

Last time: Buoyant Force (will it float?)

The magnitude of the buoyant force always equals the weight of the displaced fluid

B   V  fluid

The buoyant force is the same for a totally submerged object of any size, shape, or density

( remember V fluid means volume of fluid displaced by object )

Floating Object

The forces balance

 obj

 fluid

V fluid

V obj

Totally Submerged Object

If the object is less dense than the fluid, the object experiences a net upward force

If the object is more dense than the fluid the net force is downward

Totally Submerged Object

B   V  mg =

 object

V object g fluid

For completely submerged object:

V object

= V fluid

If

 object

<

 fluid

, mg < B

If

 object

>

 fluid

, mg > B

Example – P9.43

43. A 1.00-kg beaker containing 2.00 kg of oil (density = 916 kg/m 3 ) rests on a scale. A 2.00-kg block of iron (density =

7.86

10 3 kg/m 3 ) is suspended from a spring scale and is completely submerged in the oil (Fig. P9.39). Find the equilibrium readings of both scales.

Equation of Continuity

• A

1 v

1

= A

2 v

2

• The product of the cross-sectional area of a pipe and the fluid speed is a constant

– Speed is high where the pipe is narrow and speed is low where the pipe has a large diameter

• Av is called the flow rate

Bernoulli’s Equation

• States that the sum of the pressure, kinetic energy per unit volume, and the potential energy per unit volume has the same value at all points along a streamline

P

1

 v

2

2

  gy

 constant

Just due to energy conservation

Applications of Bernoulli’s

Principle: Venturi Tube

• Shows fluid flowing through a horizontal constricted pipe

• Speed changes as diameter changes

• Can be used to measure the speed of the fluid flow

• Swiftly moving fluids exert less pressure than do slowly moving fluids

P

1

 v 2

2

  gy

 constant

Application – Airplane Wing

• The air speed above the wing is greater than the speed below

• The air pressure above the wing is less than the air pressure below

• There is a net upward force

– Called lift

• Other factors are also involved

Example: prob. 55

h

1

=10.0 cm h

2

=5.00 cm

(along the way, find v

1 and v

2

!)

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