SlideShare a Scribd company logo
Government Engineering College,
Bhavnagar.
Civil Engineering Department
FLUID MECHANICS
• Topic:
•Properties of Fluids.
CONTENTS
•Introduction
•Fluid
•Continuum
•Fluid Properties
INTRODUCTION
• Fluid mechanics is the science that deals with the action of forces on
fluids at rest as well as in motion.
• If the fluids are at rest, the study of them is called fluid statics.
• If the fluids are in motion, where pressure forces are not considered,
the study of them is called fluid Kinematics
• If the fluids are in motion and the pressure forces are considered, the
study of them is called fluid dynamics.
FLUID
• Matter exists in two states- the solid state and the fluid state. This
classification of matter is based on the spacing between different
molecules of matter as well as on the behavior of matter when
subjected to stresses.
• Because molecules in solid state are spaced very closely, solids
possess compactness and rigidity of form. The molecules in fluid can
move more freely within the fluid mass and therefore the fluids do
not possess any rigidity of form.
• Thus Fluid exist in two form:-
• Liquid
• Gas
WHAT’S THE DIFFERENCE?
• Liquids flow and take the shape of their container but maintain a
constant volume.
• Gases expand to fill the available volume.
• Liquids are incompressible
While the gas are compressible.
FLUID PROPERTIES
Mass Density
Specific Weight
Specific Volume
Specific Gravity
Viscosity
Surface tension
Vapour Pressure
Capillarity
Cavitation
MASS DENSITY / DENSITY r
• The “mass per unit volume” is mass density. Hence it has
units of kilograms per cubic meter.
• The mass density of water at 4oC is 1000 kg/m3 while it is 1.20
kg/m3 for air at 20oC at standard pressure.
D
m
VVDm
V
m
D 
Density: Example
A quantity of helium gas at 0°C with a volume
of 4.00 m3 has a mass of 0.712 kg at standard
atmospheric pressure.
Determine the density of this sample of helium
gas.
?
712.0
00.4 3



D
kgm
mV
3178.0
00.4
712.0
3 m
kg
m
kg
D
V
m
D


SPECIFIC WEIGHT OR WEIGHT
DENSITY g
• It is the ratio between the weight if a fluid to its
volume.
• It is also weight per unit volume of a fluid.
• Its unit is N/m3.
• Water at 20 oC has a specific weight of 9.79 kN/m3
• g  r g
SPECIFIC VOLUME
• It is defined as the volume of a fluid occupied by a unit
mass or volume per unit mass of a fluid is called specific
volume.
• Specific Volume = Volume of the Fluid / Mass of the Fluid
= 1/mass of the fluid/volume of the fluid
= 1 / r
SPECIFIC GRAVITY S
• The ratio of specific weight of a given liquid to the specific weight of
water at a standard reference temperature (4oC)is defined as specific
gravity, S.
• The specific weight of water at atmospheric pressure is 9810 N/m3.
• The specific gravity of mercury at 20oC is
6.13
3kN/m9.81
3kN/m133
S Hg
Viscosity
• Different kinds of fluids flow more easily than others. Oil, for
example, flows more easily than molasses. This is because
molasses has a higher viscosity, which is a measure of resistance to
fluid flow. Inside a pipe or tube a very thin layer of fluid right near
the walls of the tube are motionless because they get caught up
in the microscopic ridges of the tube. Layers closer to the center
move faster and the fluid sheers. The middle layer moves the
fastest.
• The more viscous a fluid is, the more the layers want to cling
together, and the more it resists this shearing. The resistance is due
the frictional forces between the layers as the slides past one
another. Note, there is no friction occurring at the tube’s surface
since the fluid there is essentially still. The friction happens in the fluid
and generates heat. The Bernoulli equation applies to fluids with
negligible viscosity.
v = 0
VISCOSITY
• It is defined as the property of a fluid which offers resistance to the
movement of one layer of fluid over another adjacent layer of the
fluid.
• The viscosity of a fluid is a measure of its “resistance to deformation.”
NEWTON’S LAW OF VISCOSITY
• It states that the shear stress on a fluid element layer is directly
proportional to the rate of shear strain.
• The constant of proportionality is called the coefficient of viscosity.
•t = μ du/dy
•Where t = shear stress
du/dy = Velocity Gradient
μ = coefficient of viscosity
KINEMATIC VISCOSITY
• It is defined as the ratio between the dynamic viscosity and
density of the fluid.
sm
mkg
msN
/
/
/. 2
3
2

r


VARIATION OF VISCOSITY WITH
TEMPERATURE
•Liquids - cohesion and momentum transfer
• Viscosity decreases as temperature increases.
• Relatively independent of pressure
(incompressible)
•Gases - transfer of molecular momentum
• Viscosity increases as temperature increases.
• Viscosity increases as pressure increases
VARIATION OF VISCOSITY WITH
TEMPERATURE
Increasing temp →
increasing viscosity
Increasing temp →
decreasing viscosity
TYPES OF FLUIDS
• Ideal Fluid
• Real Fluid
• Newtonian Fluid
• Non- Newtonian Fluid
• Ideal Plastic Fluid
TYPES OF FLUID
• Newtonian fluid: shear stress is
proportional to shear strain
– Slope of line is dynamic viscosity
• Shear thinning: ratio of shear stress
to shear strain decreases as shear
strain increases (toothpaste,
catsup, paint, etc.)
• Shear thickening: viscosity
increases with shear rate (glass
particles in water, gypsum-water
mixtures).
APPLICATION OF VISCOSITY :-
1. Transparent and storing facilities for fluids i.e., pipes, tanks
2. Bitumen used for road construction.
3. Designing of the sewer line or any other pipe flow viscosity
play an important role in finding out its flow behaviour.
4. Drilling for oil and gas requires sensitive viscosity.
5. To maintain the performance of machine and
automobiles by determining thickness of lubricating oil or
motor oil.
SURFACE TENSION
• Surface tension is a contractive tendency of the surface of a fluid that
allows it to resist an external force. Surface tension is an important
property that mark ably influences the ecosystems.
What’s happening here?
– Bug is walking on water
SURFACE TENSION
• A molecules in the interior of a liquid is under attractive
force in all direction.
• However, a molecule at the surface of a liquid is acted on
by a net inward cohesive force that is perpendicular to the
surface.
• Hence it requires work to move molecules to the surface
against this opposing force and surface molecules have
more energy than interior ones
• Higher forces of attraction at surface
• Creates a “stretched membrane effect”
SURFACE TENSION
• Surface tension, σs: the force resulting from molecular
attraction at liquid surface [N/m]
Fs= σs L
Fs= surface tension force [N]
σs = surface tension [N/m]
L = length over which the surface tension acts [m]
Example: Surface Tension
• Estimate the difference in pressure (in Pa)
between the inside and outside of a bubble of
air in 20ºC water. The air bubble is 0.3 mm in
diameter.
R
p
2

R = 0.15 x 10-3 m  = 0.073 N/m
 
m1015.0
N/m073.02
3

p
hp g waterm1.0
/9806
974
3

mN
Pap
h
g
Statics!
p= 970 Pa
APPLICATION OF SURFACE
TENSION :-
 A water strider can walk on water.
 Some tent are made impermeable of the rain but they are not
really impermeable, but if water is placed on it then the water
doesn’t pass through the fine small pores of the tent cover. But as
you touch the cover while water is on it, you break surface tension
and water passes through.
CAPILLARY ACTION
• How do trees pump water hundreds of feet from the ground to their
highest leaves? Why do paper towels soak up spills? Why does liquid
wax rise to the tip of a candle wick to be burned? Why must liquids on
the space shuttle be kept covered to prevent them from crawling
right out of their containers?! These are all examples of capillary
action--the movement of a liquid up through a thin tube. It is due to
adhesion and cohesion.
• Capillary action is a result of adhesion and cohesion. A liquid that
adheres to the material that makes up a tube will be drawn inside.
Cohesive forces between the molecules of the liquid will “connect”
the molecules that aren’t in direct contact with the inside of the tube.
In this way liquids can crawl up a tube. In a pseudo-weightless
environment like in the space shuttle, the “weightless” fluid could
crawl right out of its container.
CAPILLARY ACTION :-
• Capillary action is the ability of a fluid to flow in narrow spaces
without the assistance of, and in opposition to, external forces like
gravity.
DIFFERENCES BETWEEN ADHESIVE
& COHESIVE
• The force of attraction between unlike charges in the atoms
or molecules of substances are responsible for cohesion and
adhesion.
• Cohesion is the clinging together of molecules/atoms within a
substance. Ever wonder why rain falls in drops rather than individual
water molecules? It’s because water molecules cling together to
form drops.
• Adhesion is the clinging together of molecules/atoms of two different
substances. Adhesive tape gets its name from the adhesion between
the tape and other objects. Water molecules cling to many other
materials besides clinging to themselves.
CAPILLARY EFFECT
• h=height of capillary rise (or depression)
• =surface tension
• q=wetting angle
• G=specific weight
• R=radius of tube
• If the tube is clean, q is 0 for water
APPLICATION OF CAPILLARY
ACTION :-
• Capillary action is found in thermometer where fluid used in
it automatically rises when comes in contact with higher
temperature or falls down with lower ones.
• Capillary action can be performed to transfer fluid from one
vessel to another on its own.
VAPOR PRESSURE
• Vapor pressure: the pressure at which a liquid
will boil.
Vapor pressure ↑ when temperature increases
At atmospheric pressure, water at 100 °C will
boil
Water can boil at lower temperatures if the
pressure is lower
• When vapor pressure > the liquid’s actual pressure
• It will boil.
CAVITATION
• It is the phenomenon of formation of vapour bubbles of a flowing
liquid in a region where the pressure of the liquid falls below the
vapour pressure and sudden collapsing of these vapour bubbles in a
region of a higher pressure.
THANK YOU FOR BEARING
By,
Nitin Charel – 130210106011
Kartik Hingol – 130210106030
Bhavik Shah – 130210106049
Digvijay Solanki – 130210106055

More Related Content

PPT
Fluid properties
PPTX
FLUID MECHANICS
PDF
Fluid statics
PDF
Fluid Mechanics. Chapter 1. Introduction to Fluid Mechanics
PPTX
Fluids and their properties
PPTX
Chapter 2 mechanical properties of fluids
PPTX
DENSITY: SPECIFIC GRAVITY
PPTX
Fluid Mechanics - Fluid Properties
Fluid properties
FLUID MECHANICS
Fluid statics
Fluid Mechanics. Chapter 1. Introduction to Fluid Mechanics
Fluids and their properties
Chapter 2 mechanical properties of fluids
DENSITY: SPECIFIC GRAVITY
Fluid Mechanics - Fluid Properties

What's hot (20)

PPTX
Fluid & Fluid properties
PPTX
Types of flow in fluid mechanics
PPTX
Types of fluid flow
PPTX
Fluid Mechanics - Fluid Pressure and its measurement
PPTX
Hydrostatics
PPTX
Fluid Kinematics
PPTX
Fluid Mechanics - Fluid Dynamics
PPTX
laminar and Turbulent flow
PDF
Fluid Mechanics Chapter 6. Boundary Layer Concept
PPTX
Stability of Submerged Bodies in Fluid
PPT
S3 Chapter 2 Fluid Pressure
PPTX
Boundary layer
PPTX
Flow through pipes
PDF
Chapter 1. introduction to fluid mechanics
PDF
Buoyancy and floatation
PDF
Chapter four fluid mechanics
PPTX
Fluid dynamics 1
PPTX
Fluid mechanics applications
PPTX
Dimensional analysis
PDF
Boundary layer theory
Fluid & Fluid properties
Types of flow in fluid mechanics
Types of fluid flow
Fluid Mechanics - Fluid Pressure and its measurement
Hydrostatics
Fluid Kinematics
Fluid Mechanics - Fluid Dynamics
laminar and Turbulent flow
Fluid Mechanics Chapter 6. Boundary Layer Concept
Stability of Submerged Bodies in Fluid
S3 Chapter 2 Fluid Pressure
Boundary layer
Flow through pipes
Chapter 1. introduction to fluid mechanics
Buoyancy and floatation
Chapter four fluid mechanics
Fluid dynamics 1
Fluid mechanics applications
Dimensional analysis
Boundary layer theory
Ad

Viewers also liked (13)

PDF
NUMERICAL SIMULATION AND ENHANCEMENT OF HEAT TRANSFER USING CUO/WATER NANO-FL...
PPTX
Microheat Exchangers
PPT
Emerging Trends of Industrial Inkjet Printing
PDF
Fox Philip J. Pritchard-8 ed Mc Donald's Introduction to Fluid Mechanics -wil...
PDF
Fox solution
PDF
FLUID MECHANICS AND MACHINERY FORMULA BOOK
PDF
Solução introduction to fluid mechanics (fox, 6th ed)
PDF
Case studies in BioMEMS
PDF
Solution manual of fluid mechanics fundamentals and applications - cengel [...
PDF
Introdução à mecânica dos fluidos 6ª ed. - robert w. fox; alan t. mc donald...
PDF
Solution manual fundamentals of fluid mechanics, 6th edition by munson (2009)
PPTX
Types of turbine & thier application
PDF
[Solution manual] fluid mechanics fox & mcdonald
NUMERICAL SIMULATION AND ENHANCEMENT OF HEAT TRANSFER USING CUO/WATER NANO-FL...
Microheat Exchangers
Emerging Trends of Industrial Inkjet Printing
Fox Philip J. Pritchard-8 ed Mc Donald's Introduction to Fluid Mechanics -wil...
Fox solution
FLUID MECHANICS AND MACHINERY FORMULA BOOK
Solução introduction to fluid mechanics (fox, 6th ed)
Case studies in BioMEMS
Solution manual of fluid mechanics fundamentals and applications - cengel [...
Introdução à mecânica dos fluidos 6ª ed. - robert w. fox; alan t. mc donald...
Solution manual fundamentals of fluid mechanics, 6th edition by munson (2009)
Types of turbine & thier application
[Solution manual] fluid mechanics fox & mcdonald
Ad

Similar to Properties of Fluids (20)

PDF
Chapter1_fluid.pdf based on Pokhara university
PDF
Lecture 1+2-fluid properties
PPTX
Mechanics OF fluid and fluid machinery (PSC).pptx
PDF
FM-I all slides.pdf
PPTX
FMM Unit 1. Define the expression for Reynold's numberpptx
PPTX
Diploma mechanical iv hhm u i introduction to fluid
PPTX
Properties of fluid.ppt
PDF
Hydraulics Introduction& Hydrostatics.pdf
PDF
Fluid Mechanics lectures slides 1-30.pdf
PPTX
FLUID MECHANICS - DME UPDATED(1) - Copy.pptx
PPT
Fluid Mechanics Comprehensive Lecture Notes_1.ppt
PPTX
Chapter 3.pptx
PDF
Cengel_Fluid_Dynamics_Chapter_Slides_Two
PPTX
Fluid Mechanics : Properties of fluid: numerical : part 1
PPTX
Surface tension.pptx
PPTX
Fluid Properties.pptx
PPTX
Surface tension and viscosity
PDF
Fluid Mechanics - Introduction.pdf
PPTX
Properties of Fluids, Fluid Statics, Pressure Measurement
PPTX
Fluid mechanics fluid properties and characteristics
Chapter1_fluid.pdf based on Pokhara university
Lecture 1+2-fluid properties
Mechanics OF fluid and fluid machinery (PSC).pptx
FM-I all slides.pdf
FMM Unit 1. Define the expression for Reynold's numberpptx
Diploma mechanical iv hhm u i introduction to fluid
Properties of fluid.ppt
Hydraulics Introduction& Hydrostatics.pdf
Fluid Mechanics lectures slides 1-30.pdf
FLUID MECHANICS - DME UPDATED(1) - Copy.pptx
Fluid Mechanics Comprehensive Lecture Notes_1.ppt
Chapter 3.pptx
Cengel_Fluid_Dynamics_Chapter_Slides_Two
Fluid Mechanics : Properties of fluid: numerical : part 1
Surface tension.pptx
Fluid Properties.pptx
Surface tension and viscosity
Fluid Mechanics - Introduction.pdf
Properties of Fluids, Fluid Statics, Pressure Measurement
Fluid mechanics fluid properties and characteristics

More from Bhavik A Shah (20)

PDF
The battle against corruption starts from within
PPTX
Swachchhta shapath
PPTX
Smart city
PPTX
Slope deflection method
PPTX
Purpose of Valuation
PPTX
Development of Sonpari village Under the Scheme of Smart Village
PPTX
Orientation
PPTX
Monetary Policy
PPT
Moment Distribution Method
PPT
Matrix methods
PPTX
Interpolation
PPT
Indeterminate frame by using energy principle
PPTX
Hardened concrete
PPTX
Survey required
PPT
The Water act 1947
PPTX
Traffic engineering
PPTX
Flood management
PPT
Geographic information system
PPT
Strain measurement
PPT
Food chains and food Webs
The battle against corruption starts from within
Swachchhta shapath
Smart city
Slope deflection method
Purpose of Valuation
Development of Sonpari village Under the Scheme of Smart Village
Orientation
Monetary Policy
Moment Distribution Method
Matrix methods
Interpolation
Indeterminate frame by using energy principle
Hardened concrete
Survey required
The Water act 1947
Traffic engineering
Flood management
Geographic information system
Strain measurement
Food chains and food Webs

Recently uploaded (20)

PPTX
Sustainable Sites - Green Building Construction
PDF
keyrequirementskkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkk
PPTX
FINAL REVIEW FOR COPD DIANOSIS FOR PULMONARY DISEASE.pptx
PPTX
UNIT 4 Total Quality Management .pptx
PPT
Project quality management in manufacturing
PPTX
UNIT-1 - COAL BASED THERMAL POWER PLANTS
PDF
July 2025 - Top 10 Read Articles in International Journal of Software Enginee...
DOCX
ASol_English-Language-Literature-Set-1-27-02-2023-converted.docx
PDF
Mitigating Risks through Effective Management for Enhancing Organizational Pe...
PDF
PRIZ Academy - 9 Windows Thinking Where to Invest Today to Win Tomorrow.pdf
PPTX
CYBER-CRIMES AND SECURITY A guide to understanding
PPTX
Welding lecture in detail for understanding
PPTX
CARTOGRAPHY AND GEOINFORMATION VISUALIZATION chapter1 NPTE (2).pptx
PPTX
Strings in CPP - Strings in C++ are sequences of characters used to store and...
PDF
Model Code of Practice - Construction Work - 21102022 .pdf
PPTX
MCN 401 KTU-2019-PPE KITS-MODULE 2.pptx
PPTX
KTU 2019 -S7-MCN 401 MODULE 2-VINAY.pptx
PDF
BMEC211 - INTRODUCTION TO MECHATRONICS-1.pdf
PDF
composite construction of structures.pdf
PDF
Digital Logic Computer Design lecture notes
Sustainable Sites - Green Building Construction
keyrequirementskkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkk
FINAL REVIEW FOR COPD DIANOSIS FOR PULMONARY DISEASE.pptx
UNIT 4 Total Quality Management .pptx
Project quality management in manufacturing
UNIT-1 - COAL BASED THERMAL POWER PLANTS
July 2025 - Top 10 Read Articles in International Journal of Software Enginee...
ASol_English-Language-Literature-Set-1-27-02-2023-converted.docx
Mitigating Risks through Effective Management for Enhancing Organizational Pe...
PRIZ Academy - 9 Windows Thinking Where to Invest Today to Win Tomorrow.pdf
CYBER-CRIMES AND SECURITY A guide to understanding
Welding lecture in detail for understanding
CARTOGRAPHY AND GEOINFORMATION VISUALIZATION chapter1 NPTE (2).pptx
Strings in CPP - Strings in C++ are sequences of characters used to store and...
Model Code of Practice - Construction Work - 21102022 .pdf
MCN 401 KTU-2019-PPE KITS-MODULE 2.pptx
KTU 2019 -S7-MCN 401 MODULE 2-VINAY.pptx
BMEC211 - INTRODUCTION TO MECHATRONICS-1.pdf
composite construction of structures.pdf
Digital Logic Computer Design lecture notes

Properties of Fluids

  • 4. INTRODUCTION • Fluid mechanics is the science that deals with the action of forces on fluids at rest as well as in motion. • If the fluids are at rest, the study of them is called fluid statics. • If the fluids are in motion, where pressure forces are not considered, the study of them is called fluid Kinematics • If the fluids are in motion and the pressure forces are considered, the study of them is called fluid dynamics.
  • 5. FLUID • Matter exists in two states- the solid state and the fluid state. This classification of matter is based on the spacing between different molecules of matter as well as on the behavior of matter when subjected to stresses. • Because molecules in solid state are spaced very closely, solids possess compactness and rigidity of form. The molecules in fluid can move more freely within the fluid mass and therefore the fluids do not possess any rigidity of form. • Thus Fluid exist in two form:- • Liquid • Gas
  • 6. WHAT’S THE DIFFERENCE? • Liquids flow and take the shape of their container but maintain a constant volume. • Gases expand to fill the available volume. • Liquids are incompressible While the gas are compressible.
  • 7. FLUID PROPERTIES Mass Density Specific Weight Specific Volume Specific Gravity Viscosity Surface tension Vapour Pressure Capillarity Cavitation
  • 8. MASS DENSITY / DENSITY r • The “mass per unit volume” is mass density. Hence it has units of kilograms per cubic meter. • The mass density of water at 4oC is 1000 kg/m3 while it is 1.20 kg/m3 for air at 20oC at standard pressure. D m VVDm V m D 
  • 9. Density: Example A quantity of helium gas at 0°C with a volume of 4.00 m3 has a mass of 0.712 kg at standard atmospheric pressure. Determine the density of this sample of helium gas. ? 712.0 00.4 3    D kgm mV 3178.0 00.4 712.0 3 m kg m kg D V m D  
  • 10. SPECIFIC WEIGHT OR WEIGHT DENSITY g • It is the ratio between the weight if a fluid to its volume. • It is also weight per unit volume of a fluid. • Its unit is N/m3. • Water at 20 oC has a specific weight of 9.79 kN/m3 • g  r g
  • 11. SPECIFIC VOLUME • It is defined as the volume of a fluid occupied by a unit mass or volume per unit mass of a fluid is called specific volume. • Specific Volume = Volume of the Fluid / Mass of the Fluid = 1/mass of the fluid/volume of the fluid = 1 / r
  • 12. SPECIFIC GRAVITY S • The ratio of specific weight of a given liquid to the specific weight of water at a standard reference temperature (4oC)is defined as specific gravity, S. • The specific weight of water at atmospheric pressure is 9810 N/m3. • The specific gravity of mercury at 20oC is 6.13 3kN/m9.81 3kN/m133 S Hg
  • 13. Viscosity • Different kinds of fluids flow more easily than others. Oil, for example, flows more easily than molasses. This is because molasses has a higher viscosity, which is a measure of resistance to fluid flow. Inside a pipe or tube a very thin layer of fluid right near the walls of the tube are motionless because they get caught up in the microscopic ridges of the tube. Layers closer to the center move faster and the fluid sheers. The middle layer moves the fastest. • The more viscous a fluid is, the more the layers want to cling together, and the more it resists this shearing. The resistance is due the frictional forces between the layers as the slides past one another. Note, there is no friction occurring at the tube’s surface since the fluid there is essentially still. The friction happens in the fluid and generates heat. The Bernoulli equation applies to fluids with negligible viscosity. v = 0
  • 14. VISCOSITY • It is defined as the property of a fluid which offers resistance to the movement of one layer of fluid over another adjacent layer of the fluid. • The viscosity of a fluid is a measure of its “resistance to deformation.”
  • 15. NEWTON’S LAW OF VISCOSITY • It states that the shear stress on a fluid element layer is directly proportional to the rate of shear strain. • The constant of proportionality is called the coefficient of viscosity. •t = μ du/dy •Where t = shear stress du/dy = Velocity Gradient μ = coefficient of viscosity
  • 16. KINEMATIC VISCOSITY • It is defined as the ratio between the dynamic viscosity and density of the fluid. sm mkg msN / / /. 2 3 2  r  
  • 17. VARIATION OF VISCOSITY WITH TEMPERATURE •Liquids - cohesion and momentum transfer • Viscosity decreases as temperature increases. • Relatively independent of pressure (incompressible) •Gases - transfer of molecular momentum • Viscosity increases as temperature increases. • Viscosity increases as pressure increases
  • 18. VARIATION OF VISCOSITY WITH TEMPERATURE Increasing temp → increasing viscosity Increasing temp → decreasing viscosity
  • 19. TYPES OF FLUIDS • Ideal Fluid • Real Fluid • Newtonian Fluid • Non- Newtonian Fluid • Ideal Plastic Fluid
  • 20. TYPES OF FLUID • Newtonian fluid: shear stress is proportional to shear strain – Slope of line is dynamic viscosity • Shear thinning: ratio of shear stress to shear strain decreases as shear strain increases (toothpaste, catsup, paint, etc.) • Shear thickening: viscosity increases with shear rate (glass particles in water, gypsum-water mixtures).
  • 21. APPLICATION OF VISCOSITY :- 1. Transparent and storing facilities for fluids i.e., pipes, tanks 2. Bitumen used for road construction. 3. Designing of the sewer line or any other pipe flow viscosity play an important role in finding out its flow behaviour. 4. Drilling for oil and gas requires sensitive viscosity. 5. To maintain the performance of machine and automobiles by determining thickness of lubricating oil or motor oil.
  • 22. SURFACE TENSION • Surface tension is a contractive tendency of the surface of a fluid that allows it to resist an external force. Surface tension is an important property that mark ably influences the ecosystems. What’s happening here? – Bug is walking on water
  • 23. SURFACE TENSION • A molecules in the interior of a liquid is under attractive force in all direction. • However, a molecule at the surface of a liquid is acted on by a net inward cohesive force that is perpendicular to the surface. • Hence it requires work to move molecules to the surface against this opposing force and surface molecules have more energy than interior ones • Higher forces of attraction at surface • Creates a “stretched membrane effect”
  • 24. SURFACE TENSION • Surface tension, σs: the force resulting from molecular attraction at liquid surface [N/m] Fs= σs L Fs= surface tension force [N] σs = surface tension [N/m] L = length over which the surface tension acts [m]
  • 25. Example: Surface Tension • Estimate the difference in pressure (in Pa) between the inside and outside of a bubble of air in 20ºC water. The air bubble is 0.3 mm in diameter. R p 2  R = 0.15 x 10-3 m  = 0.073 N/m   m1015.0 N/m073.02 3  p hp g waterm1.0 /9806 974 3  mN Pap h g Statics! p= 970 Pa
  • 26. APPLICATION OF SURFACE TENSION :-  A water strider can walk on water.  Some tent are made impermeable of the rain but they are not really impermeable, but if water is placed on it then the water doesn’t pass through the fine small pores of the tent cover. But as you touch the cover while water is on it, you break surface tension and water passes through.
  • 27. CAPILLARY ACTION • How do trees pump water hundreds of feet from the ground to their highest leaves? Why do paper towels soak up spills? Why does liquid wax rise to the tip of a candle wick to be burned? Why must liquids on the space shuttle be kept covered to prevent them from crawling right out of their containers?! These are all examples of capillary action--the movement of a liquid up through a thin tube. It is due to adhesion and cohesion. • Capillary action is a result of adhesion and cohesion. A liquid that adheres to the material that makes up a tube will be drawn inside. Cohesive forces between the molecules of the liquid will “connect” the molecules that aren’t in direct contact with the inside of the tube. In this way liquids can crawl up a tube. In a pseudo-weightless environment like in the space shuttle, the “weightless” fluid could crawl right out of its container.
  • 28. CAPILLARY ACTION :- • Capillary action is the ability of a fluid to flow in narrow spaces without the assistance of, and in opposition to, external forces like gravity.
  • 29. DIFFERENCES BETWEEN ADHESIVE & COHESIVE • The force of attraction between unlike charges in the atoms or molecules of substances are responsible for cohesion and adhesion. • Cohesion is the clinging together of molecules/atoms within a substance. Ever wonder why rain falls in drops rather than individual water molecules? It’s because water molecules cling together to form drops. • Adhesion is the clinging together of molecules/atoms of two different substances. Adhesive tape gets its name from the adhesion between the tape and other objects. Water molecules cling to many other materials besides clinging to themselves.
  • 30. CAPILLARY EFFECT • h=height of capillary rise (or depression) • =surface tension • q=wetting angle • G=specific weight • R=radius of tube • If the tube is clean, q is 0 for water
  • 31. APPLICATION OF CAPILLARY ACTION :- • Capillary action is found in thermometer where fluid used in it automatically rises when comes in contact with higher temperature or falls down with lower ones. • Capillary action can be performed to transfer fluid from one vessel to another on its own.
  • 32. VAPOR PRESSURE • Vapor pressure: the pressure at which a liquid will boil. Vapor pressure ↑ when temperature increases At atmospheric pressure, water at 100 °C will boil Water can boil at lower temperatures if the pressure is lower • When vapor pressure > the liquid’s actual pressure • It will boil.
  • 33. CAVITATION • It is the phenomenon of formation of vapour bubbles of a flowing liquid in a region where the pressure of the liquid falls below the vapour pressure and sudden collapsing of these vapour bubbles in a region of a higher pressure.
  • 34. THANK YOU FOR BEARING By, Nitin Charel – 130210106011 Kartik Hingol – 130210106030 Bhavik Shah – 130210106049 Digvijay Solanki – 130210106055