Transcript unit-1

Mechanics of Fluids
I.GNANASEELAN
lecturer,
department of mechanical Engineering,
Parisutham institute of technology and science
Mechanics of Fluids
SEQUENCE OF CHAPTER 1
 Introduction
 Objective
 History
 Definition of a fluid
 Dimension and units
 Fluid properties
 Continuum Concept of system and control
volume
Introduction
• Defined: the science that deals with the forces on fluids and
their actions.
• Fluids: a substance consisting of particles that change their
position relative to each other.
• A substance that will continuously deform when shear stress
is applied to it.
• Solids resist stress, do not easily deform.
Objectives
 Identify the units for the basic quantities of time,
length, force and mass.
 Properly set up equations to ensure consistency of
units.
 Define the basic fluid properties.
 Identify the relationships between specific weight,
specific gravity and density, and solve problems using
their relationships.
History
Faces of Fluid Mechanics
Archimedes
(C. 287-212 BC)
Navier
(1785-1836)
Newton
(1642-1727)
Stokes
(1819-1903)
Leibniz
(1646-1716)
Reynolds
(1842-1912)
Fluid Mechanics
Bernoulli
Euler
(1667-1748)
(1707-1783)
Prandtl
Taylor
(1875-1953)
(1886-1975)
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Fluid Mechanics
• Definition
– The study of liquids and gases at rest (statics) and in
motion (dynamics)
• Engineering applications
–
–
–
–
–
Blood in capillaries
Oil in pipelines
Groundwater movement
Runoff in parking lots
Pumps, filters, rivers, etc.
States of Matter
• Fluids (gasses and liquids) and solids
• What’s the difference?
– Fluid particles are free to move among themselves
and give way (flow) under the slightest tangential
(shear) force
Shear Stress t
Solid
Fluid
Classes of Fluids
• Liquids and gasses – What’s the difference?
– Liquids: Close packed,
strong cohesive forces,
retains volume, has
free surface
– Gasses: Widely spaced,
weak cohesive forces,
free to expand
Free Surface
Expands
Liquid
Gas
Common Fluids
• Liquids:
– water, oil, mercury, gasoline, alcohol
• Gasses:
– air, helium, hydrogen, steam
• Borderline:
– jelly, asphalt, lead, toothpaste, paint, pitch
Dimensions and Units
• The dimensions have to be the same for each
term in an equation
• Dimensions of mechanics are
L
– length
T
– time
M
– mass
F  ma
– force

– temperature
MLT-2
Dimensions and Units
Quantity
Symbol
Velocity
V
Acceleration
a
Area
A
Volume

Discharge
Q
Pressure
p
Gravity
g
Temperature
T’
Mass concentration C
Dimensions
LT-1
LT-2
L2
L3
L3T-1
ML-1T-2
LT-2

ML-3
Dimensions and Units
Quantity
Symbol Dimensions
Density
Specific Weight
Dynamic viscosity
Kinematic viscosity
Surface tension
Bulk mod of elasticity
r
g
m


E
fluid properties!
These are _______
How many independent properties? _____
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ML-3
ML-2T-2
ML-1T-1
L2T-1
MT-2
ML-1T-2
Fluid Properties
• Density: Mass per unit volume
– How large is the volume?
• Too small: # molecules changes continuously
• Large: # molecules remains almost constant
– At these scales, fluid properties (e.g., density) can
be thought of as varying continuously in space.
r
m
V V * V
lim
Density
• Mass per unit volume (e.g., @ 20 oC, 1 atm)
– Water
– Mercury
– Air
rwater = 1000 kg/m3
rHg = 13,500 kg/m3
rair = 1.22 kg/m3
• Densities of gasses increase with pressure
• Densities of liquids are nearly constant
(incompressible) for constant temperature
• Specific volume = 1/density
Specific Weight
g  rg
[ N / m3 ] or [lbf / ft 3 ]
• Weight per unit volume (e.g., @ 20 oC, 1 atm)
gwater
= (998 kg/m3)(9.807 m2/s)
= 9790 N/m3
[= 62.4 lbf/ft3]
gair
= (1.205 kg/m3)(9.807 m2/s)
= 11.8 N/m3
[= 0.0752 lbf/ft3]
Specific Gravity
• Ratio of fluid density to density at STP
(e.g., @ 20 oC, 1 atm)
SGliquid 
SGgas 
– Water
– Mercury
– Air
rliquid
r water
r gas
r air

SGwater = 1
SGHg = 13.6
SGair = 1

rliquid
9790 kg / m3
r gas
1.205 kg / m3
Ideal Gas Law
• Equation of state
pV  nRnT
p  rRT ,
R  Rn / M
Rn = universal gas constant
M = molecular weight of the gas