+ All Categories
Home > Documents > Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Date post: 16-Dec-2015
Category:
Upload: makena-lyons
View: 222 times
Download: 3 times
Share this document with a friend
Popular Tags:
21
Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435
Transcript
Page 1: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Chapter 15Fluids

Dr. Haykel Abdelhamid Elabidi

1st/2nd week of December 2013/Saf 1435

Page 2: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Units of Chapter 15

• Density

• Pressure

• Static Equilibrium in fluids

• Archimedes' Principle and Buoyancy

• Fluid Flow and Continuity

• Bernoulli's Equation

Page 3: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Density

Definition of fluid: it is a substance that can readily flow from place to place, and take the shape of a container rather than retain a shape of their own.Examples: gases and liquids

Page 4: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Pressure

Page 5: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Pressure

The pressure in fluid acts equally in all directions, and acts at right angles to any surface, so we don’t usually notice it.

Page 6: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Pressure

Page 7: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Static equilibrium in fluids: Pressure and depth

The increased pressure as an object descends through a fluid is due to the increasing mass of the fluid above it.

Page 8: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Static equilibrium in fluids: Pressure and depth

Page 9: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Static equilibrium in fluids: Pressure and depth

Page 10: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Static equilibrium in fluids: Pressure and depth

Page 11: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Static equilibrium in fluids: Pressure and depth

Page 12: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Archimedes’ principle and buoyancy

A fluid exerts a net upward force on any object it surrounds, called the buoyant force.

the buoyant force is due to the increased pressure at the bottom of the object compared to the top.

Page 13: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Archimedes’ principle and buoyancy

Page 14: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Archimedes’ principle and buoyancy

Page 15: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Fluid flow and continuity

Continuity tells us that whatever the volume of fluid in a pipe passing a particular point per second, the same volume must pass every other point in a second. The fluid is not accumulating or vanishing along the way.

This means that where the pipe is narrower, the flow is faster.

Page 16: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Fluid flow and continuityMost gases are easily compressible; most liquids are not. Therefore, the density of a liquid may be treated as constant, but not that of a gas.

3.

Page 17: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Bernoulli’s equation

The Bernoulli’s Equation is the work – energy theorem applied to fluids. The result is a relation between the pressure of a fluid, its speed, and its height.

If there is no change in height, the Bernoulli’s equation becomes:

Page 18: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Bernoulli’s equation

Page 19: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Bernoulli’s equationExercise 15-4 page 520

There is a difference in height, so we apply the Bernoulli’s equation (the subscript (1) for the bottom and (2) for the top:

Page 20: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Bernoulli’s equation

Figure 15-19

Page 21: Chapter 15 Fluids Dr. Haykel Abdelhamid Elabidi 1 st /2 nd week of December 2013/Saf 1435.

Thank you for your attention

See you next time Inchallah


Recommended