Hydrostatic Law
The variation of pressure in the vertical direction in a fluid is directly
 proportional to the specific weight
                                    =
                                   P =ρgh (SI unit is N/m2 )
 When you move vertically down a fluid, the pressure increases as
 +ρgh.
When you move vertically up in a fluid, the pressure decreases as -ρgh.
On the same horizontal level there is no change of pressure.
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                                       What is Viscosity?
“Viscosity” is derived from the latin word “Viscum”, meaning “anything sticky”
It describes the internal friction of a moving fluid
A fluid with large Viscosity resists motion
A fluid with low Viscosity flow
It exists in both liquids and gases and is essentially a friction force between different layers
 of fluid as they move past one another.
In liquids the viscosity is due to the cohesive forces between the molecules
In gases the viscosity is due to collisions between the molecules.
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                                 Viscosity?
 It is represented by the symbol η "eta“
  is the ratio of the shearing stress (ƒ/A) to the strain rate (v/d).
 SI unit of viscosity is the Pascal second [Pa s].
 A common unit is the poise (P) where 1 Pa.s = 10 P
Types of viscosity
1. Dynamic or Simple viscosity
2. Kinematic Viscosity
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                        Factors that Affect Viscosity
Speed of Particles : As speed increases, viscosity decreases
Attraction: As attraction increase, viscosity increases .
Space Between Particles: As the space increases, viscosity decreases
Amount of Energy (heat): As the temperature increases, viscosity decreases
Example :         Volcano
                    Lava
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                       Kinematic Viscosity
 A measure of the resistive flow of a fluid under the influence
  of gravity.
 represented by the symbol ν "nu“
 It is ratio of the viscosity of a fluid to its density.
                    ν = ŋ/ρ
 Can be measured using the Capillary Viscometer.
 SI unit of kinematic viscosity is the [m2/s].
 Common unit used is the stroke (St) = [cm2/s]
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                           Dynamic (or absolute ) Viscosity
                                                                                        ∆
Viscosity (“µ”) is the ratio of the shearing stress (F/A) to the velocity gradient   (     ) in a fluid
                                                                                        ∆
Formula for general Viscosity or Dynamic /Absolute Viscosity is same
                     /
       µ        ∆
                 ∆
Measurement of thickness of fluid i.e. tangential force per unit area required to move one
 horizontal plane with respect to an other plane at an unit velocity . When maintaining an unit
 distance apart in the fluid
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                      Dynamic Vs Kinematic Viscosity
If you are particularly interested in the interaction between molecules that can
 be interpreted in terms of mechanical stress, the dynamic viscosity is more
 appropriate.
 Nevertheless, the kinematic viscosity is νrecommended when you are interested
 in a fluid motion and velocity field
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                   Newton’s law of Viscosity
Newton’s law of viscosity states that “Shear stress is directly
 proportional to the velocity gradient.”
 Mathematically the can be stated as:
                                   V
Where,
   Viscosity of fluid (Pa.s)
  Vx _ Velocity in x direction, (m/s)
  y - Distance,(m)
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                    Newton’s law of Viscosity
Newton’s law of viscosity will tell us the definition of viscosity
 The Viscosity of fluid (gases and liquids) varies with temperature and
 pressure.
Under laminar flow conditions, macules of a fluid move in layers that
 slide passed one another in an orderly fashion.
 Newton's suggest that those fluids which obey Newton's law of
 viscosity be called Newtonian fluids, and those fluids which do not
 obey this law are called non-Newtonian fluids
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                            Newtonian Fluid
Fluids that obey Newton’s law of viscosity are known as Newtonian
 fluids
 When shear is applied Viscosity remains constant at constant
 temperature
Example
Water
Mineral oil
Gasoline
Alcohol
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                                           Non-Newtonian Fluid
 Fluids which does not obey Newton’s law of viscosity.
 When shear is applied, the Viscosity of the fluid changes at a constant
 temperature
                                                                                           Viscosity
 Dilatant - Viscosity of the fluid increases when shear is applied,                                       Dilatant
 Examples corn flour solution, wet beach sand, potassium silicate in water
and starch in water.
 Pseudoplastic - Viscosity of the fluid decreases when shear is applied
Examples : ketchup, polymer solution , biological fluids , detergent, starch
suspension, greases etc                                                                                Pseudoplastic
                                                                                                            Stress
          05-10-2023                               Presenting By: Dr. Shraddha Shirbhate
                              Non-Newtonian Fluid
                                                        Viscosity
Rheopectic – Viscosity of the fluid increases when                       Dilatant
  shear is applied
The difference from dilatant is that in Rheoptectic
viscosity increase is time dependant
Examples: Gypsum paste, bentonite clay, clay                          Pseudoplastic
suspension etc.                                                            Stress
Thixotropic- viscosity of the fluid decreases when                          Rheopectic
                                                          Viscosity
 shear is applied
This is a time dependent property as well .i.e Glue,
 paints, polymer solution etc
                                                                       Thixotropic
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             What is Reynolds number ?
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                             What is Reynolds number
Reynolds number used: Scaling of fluid dynamics problems
                       Determine dynamic similitude
                       To identify the different cases of fluid flow
 The Reynolds number is the ratio of inertial forces to viscous forces
  within a fluid which is subjected to relative internal movement due to
  different fluid velocities.
                                                  inertial forces
                                Reynolds number =
                                                  viscous forces
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                                     Reynolds number
The Reynolds number is defined as                                      Velocity of fluid
                                Density of fluid
                                                      =                              Dimeter of pipe
                             Reynolds number                               Dynamics
                                                                           Viscosity of
                                                                           fluid
                      Where,
                          Density of fluid (SI units: kg /m3)
                     V - Velocity of fluid (m/s)
                     µ - Dynamics Viscosity of fluid (Pa.s or N.s/m2)
                     D - Dimeter of pipe (m)
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                 Reynolds number
                 Flow in a pipe or liquid
     Density of fluid (SI units: kg /m3)
 V - Velocity of fluid (m/s)
 Q- Volumetric flow rate
                                            Dynamic Pressure
 D - Dimeter of pipe (m)
      =
      Dynamic viscosity of fluid
 ν – Kinematic Viscosity of fluid          Shearing Stress
 A- cross-sectional area of pipe
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                Reynolds number
The Reynolds number can be used to identify if a flow is laminar or turbulent
 Laminar Flow: Re <2300: Laminar Flow occurs at low Reynolds numbers,
  where viscous forces are dominant , and is characterized by smooth ,
  constant fluid motion
 Turbulent Flow: Re >4000: Turbulent flow occurs at high Reynolds
  numbers and is dominated by inertial forces , which tend to produce chaotic
  eddies, and other flow instabilities
 Transient Flow when 2300 < Re <4000
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                 Poiseuille’s Equation
In fluid dynamics, Hagen–Poiseuille law - the pressure drop in a fluid flowing
 through a long cylindrical pipe.
Defines the relationship between pressure, volume flow, resistance
In a few cases of a laminar flow or a smooth flow, the volume rate of flow
 of a substance is denoted by the difference in the pressure divided by the
 resistance provided by the viscosity
      Mathematically expressed as,                    Where,
                                  P                   Q=Volume flow
                           Q=                         ΔP = Pressure Difference
                                 R
Helps to measure fluid moves through a Vessel        R= Resistance
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                             Poiseuille’s equation
 The rate of flow in a fluid in a round tube depends on the viscosity of the
  fluid, the pressure difference, and the dimensions of the tube.
 The volume flow rate is proportional to the pressure difference, inversely
  proportional to the length of the tube and proportional to the fourth power
  of the radius of the tube.
                                   ∆P                 Q = volume flow
                              Q= R                    P1 – P2 = Pressures at proximal/distal ends
                                                      r = Radius of the tube
                                                      L = Length of the tube
                                  8𝛈L                 n = viscosity of the fluid
                             𝑅=
                                  Π𝑟
                             (P1 –P2) Π𝑟
                        𝑄=
                                 8𝛈L
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            Most important regarding Poiseuille’s Equation
Diameter change has most dramatic effect on
 resistance
Radius of vessel is DIRECTLY proportional to
 volume flow
Small changes in radius may result in large
 changes in volume flow.
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Applications of Poiseuille's Law Formula
Poiseuille's law can be used to calculate the blood flow rate in
 arteries and veins, which is important for understanding blood
 pressure and cardiovascular health.
The assumptions in Poiseuille’s law are wide, such that the
 equation of Poiseuille’s law is derived from Navier-Stokes equation
 of dimensional analysis.
Poiseuille’s law is also applicable to many general situations in our
 day-to-day life, and it is normally with the context of the topic of
 hemodynamics.
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1. A living room has floor dimensions of 3.5 m and 4.2 m and a height of 2.4 m.
        (a) What does the air in the room weigh when the air pressure is 1.0 atm (    1.21 kg/m3 )
        (b) What is the magnitude of the atmosphere’s downward force on the top of your head, which we take
        to have an area of 0.040 m2 ? (1 atm = 1.01 x 105 Pa)
2. If the equation of a velocity profile over a plate is v = 5y 2 + y (where v is the velocity in m/s) determine the
   shear stress at y =0 and at y =7.5cm . Given the viscosity of the liquid is 8.35 poise.
3. A river is 40m wide, 2.2m deep and flows at 4.5 m/s. It passes through a 3.7-m wide gorge, where the flow
    rate increases to 6.0 m/s. How deep is the gorge?
4.   Air at 20°C and atmospheric pressure has a density of 1.23 kg/m . Find its specific gravity. What is the
     ratio of the specific gravity of water to the specific gravity of air at 20°C and atmospheric pressure?
     What is the significance of the ratio?
5.    A cubical block of 20 cm side and of 20 kg weight is allowed to slide down along a plane inclined at 30o to
     the horizontal on which there is a film of oil having viscosity 2.16x10-3 N-s/m2 .What will be the terminal
     velocity of the block if the film thickness is 0.025m
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