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Fluid Mechanics

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Fluid Mechanics
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Page 1: Fluid Mechanics

Fluid Mechanics

Page 2: Fluid Mechanics

Fluid Mechanics Overview

Gas Liquids Statics Dynamics

Air, He, Ar, N2, etc.

Water, Oils, Alcohols, etc.

0 iF 0 iF , Flows

Stability

Fluid Mechanics

Page 3: Fluid Mechanics

Characteristics of Fluids

• Gas or liquid state• “Large” molecular spacing relative to a solid• “Weak” intermolecular cohesive forces• Can not resist a shear stress in a stationary

state• Will take the shape of its container• Generally considered a continuum• Viscosity distinguishes different types of fluids

Page 4: Fluid Mechanics

Measures of Fluid Mass and Weight: Density

v

m

The density of a fluid is defined as mass per unit volume.

•Different fluids can vary greatly in density

•Liquids densities do not vary much with pressure and temperature

•Gas densities can vary quite a bit with pressure and temperature

•Density of water at 4° C : 1000 kg/m3

•Density of Air at 4° C : 1.20 kg/m3

Alternatively, Specific Volume:

1

m = mass, and v = volume.

Page 5: Fluid Mechanics
Page 6: Fluid Mechanics

Pressure

the only stress that canbe exerted on an object submerged in a static fluid is one that tends to compress theobject from all sides.

Page 7: Fluid Mechanics

Check your understanding

Suppose you are standing directly behind someone who steps back and accidentally stomps on your foot with the heel of one shoe. Would you

be better off if that person were (a) a large professional basketball player wearing sneakers (b) a petite woman wearing spike-heeled shoes?

Page 8: Fluid Mechanics
Page 9: Fluid Mechanics

Variation of Pressure with Depth

Page 10: Fluid Mechanics

Pascal's principle Pascal’s law: a change in the pressure applied to a fluid is transmitted undiminished to every point of the fluid and to the walls of the container.

Page 11: Fluid Mechanics

Check your understanding

The pressure at the bottom of a filled glass of water (1 000 kg/m3) is P. The water is poured out and the glass is filled with ethyl alcohol (806 kg/m3). The pressure at the bottom of the glass is (a) smaller than P(b) equal to P (c) larger than P (d) indeterminate.

Page 12: Fluid Mechanics

In a car lift used in a service station, compressed air exerts a force on a small piston that has a circular cross section and a radius of 5.00 cm. This pressure is transmitted by a liquid to a piston that has a radius of 15.0 cm. What force must the compressed air exert to lift a car weighing 13 300 N? What air pressure produces this force?

Page 13: Fluid Mechanics

Buoyant Forces and Archimedes’s Principle

Archimedes’s principle - the magnitude of the buoyant force always equals the weight of the fluid displaced by the object.

Page 14: Fluid Mechanics

Fluid Dynamics

Ideal fluid flow1. The fluid is nonviscous. In a nonviscous fluid, internal friction is neglected. An object moving through the fluid experiences no viscous force.

2. The flow is steady. In steady (laminar) flow, the velocity of the fluid at each point remains constant.

3. The fluid is incompressible. The density of an incompressible fluid is constant.

4. The flow is irrotational. In irrotational flow, the fluid has no angular momentum about any point. If a small paddle wheel placed anywhere in the fluid does not rotate about the wheel’s center of mass, then the flow is irrotational.

Page 15: Fluid Mechanics

Equation of continuity for fluids

Page 16: Fluid Mechanics

Bernoulli’s Equation

Page 17: Fluid Mechanics

The horizontal constricted pipe , known as a Venturi tube, can be used to measure the flow speed of an incompressible fluid. Determine the flow speed at point 2 if the pressure difference P1 - P2 is known.

Page 18: Fluid Mechanics

Measures of Fluid Mass and Weight: Specific Weight

g The specific weight of fluid is its weight per unit volume.

•Specific weight characterizes the weight of the fluid system

•Specific weight of water at 4° C : 9.80 kN/m3

•Specific weight of air at 4° C : 11.9 N/m3

g = local acceleration of gravity, 9.807 m/s2

Page 19: Fluid Mechanics

Measures of Fluid Mass and Weight: Specific Gravity

OH

SG2

The specific gravity of fluid is the ratio of the density of the fluid to the density of water @ 4° C.

•Gases have low specific gravities

•A liquid such as Mercury has a high specific gravity, 13.2

•The ratio is unitless.

•Density of water at 4° C : 1000 kg/m3

Page 20: Fluid Mechanics

Viscosity:

dy

du

. A fluid can not resist a shear and under shear begins to flow. The shearing stress and shearing strain can be related with a relationship of the following form for common fluids such as

is the absolute viscosity or dynamics viscosity of the fluid, u is the velocity of the fluid and y is the vertical coordinate.

Page 21: Fluid Mechanics

Viscosity: MeasurementsA Capillary Tube Viscosimeter is one method of measuring the viscosity of the fluid.

Viscosity Varies from Fluid to Fluid and is dependent on temperature, thus temperature is measured as well.

Units of Viscosity are N·s/m2 or lb·s/ft2

Page 22: Fluid Mechanics

Viscosity: Kinematic Viscosity

•Kinematic viscosity is another way of representing viscosity•Used in the flow equations•The units are of L2/T or m2/s and ft2/s

Page 23: Fluid Mechanics

Vapor Pressure: Evaporation and Boiling Evaporation occurs in a fluid when liquid molecules at the surface have sufficient momentum to overcome the intermolecular cohesive forces and escapeto the atmosphere.

Vapor Pressure is that pressure exerted on the fluid by the vapor in a closedsaturated system where the number of molecules entering the liquid are the same as those escaping. Vapor pressure depends on temperature and type of fluid.

Boiling occurs when the absolute pressure in the fluid reaches the vapor pressure.Boiling occurs at approximately 100 °C, but it is not only a function of temperature,but also of pressure. For example, in Colorado Spring, water boils at temperaturesless than 100 °C.

Cavitation is a form of Boiling due to low pressure locally in a flow.

Page 24: Fluid Mechanics

Surface Tension At the interface between a liquid and a gas or two immiscible liquids, forces develop forming an analogous “skin” or “membrane” stretched over the fluid mass which can support weight.

This “skin” is due to an imbalance of cohesive forces. The interior of the fluid is in balance as molecules of the like fluid are attracting each other while on the interface there is a net inward pulling force.

Surface tension is the intensity of the molecular attraction per unit length alongany line in the surface.

Surface tension is a property of the liquid type, the temperature, and the other fluid at the interface.

This membrane can be “broken” with a surfactant which reduces the surface tension.


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