EULERIAN AND LAGRANGIAN FLUID
FLOW APPROACH
• Focus on overall/ average fluid
flow passing over a fixed location
• Example: observer sitting on the
bank of a river and watching flow
• Focus on individual fluid parcels
and bubble-scale information
• Example: observer sitting in a
boat and follows the flow of river
Eulerian flow Lagrangian flow
STREAM LINES, PATH LINES AND
STREAK LINES
• Streamlines: an imaginary curve or line in the flow field so that the
tangent to the curve at any point represents the direction of the
instantaneous velocity at that point
• Stream lines can never intersect each other and can not be observed in
experiments
Streamlines around an air foil
and upper lower stream tubes
STREAM LINE, PATH LINE AND STREAK
LINE
• Streakline: is the locus of the temporary locations of all particles that
have passed though a fixed point in the flow field at any instant of time
• can be observed in experimental flow visualization
• Dye line
Streak line used to visualize the flow around a car
inside a wind tunnel
ONE’, TWO’’, THREE’’’ DIMENSIONAL
FLOW
One dimensional flow: All the flow parameters may be expressed as
functions of time and one space coordinate only
Example: the fully-developed flow through a pipe
ONE’, TWO’’, THREE’’’ DIMENSIONAL
FLOW
In reality, flow is never one-dimensional because viscosity causes the
velocity to decrease to zero at the solid boundaries
Two dimensional flow: All the flow parameters are functions of time and
two space coordinates (say x and y)
ONE’, TWO’’, THREE’’’ DIMENSIONAL
FLOW
Three dimensional flow: The hydrodynamic parameters are functions of
three space coordinates and time.
BASIC LAWS OF CONSERVATION
• Conservation of mass (continuity equation)
• Conservation of momentum (Newton’s second law of motion)
• Conservation of energy (First law of thermodynamics)
• involve equation of state and fluid properties, physical properties etc.
CONSERVATION OF MASS –
THE CONTINUITY EQUATION
•
QUESTIONS
• Find the depth of point below sea water surface where the pressure intensity is
404.8 kN/m2
. The specific gravity of sea water is given to be 1.03.
• Solution hint:
Total pressure on the surface, P = Weight of liquid above the immersed surface
= Specific weight of liquid * Volume of liquid
= Specific weight of liquid * area of the surface * depth of the liquid
OR
Intensity of the pressure at the base (point) per unit area = sp. wt. * depth
QUESTIONS
• A soap bubble 50 mm in diameter has an internal pressure in excess of the
outside pressure of 30 N/mm2
. Calculate the surface tension in the film of the
soap bubble.
• Solution hint: Consider the equilibrium of the upper hemisphere of the drop,
• the upward force on the plane face ABCD is , Fup = Pπr
• the surface tension force acting downward along the
• circumference (ABCD) = T 2πr
• A soap bubble has two liquid surfaces in contact with air, one inside the bubble
and another outside the bubble, at equilibrium, Pπr = T 2πr
BERNOULLI'S EQUATION
• Bernoulli's principle: " For a perfect incompressible liquid, flowing in a
continuous stream, the total energy of a particle remains the same,
while the particle moves from one point to another."
VENTURI METER
VENTURI METER
VENTURI METER
VENTURI METER
• Uses and applications:

phenomena and correlations of flowmeters.pptx

  • 1.
    EULERIAN AND LAGRANGIANFLUID FLOW APPROACH • Focus on overall/ average fluid flow passing over a fixed location • Example: observer sitting on the bank of a river and watching flow • Focus on individual fluid parcels and bubble-scale information • Example: observer sitting in a boat and follows the flow of river Eulerian flow Lagrangian flow
  • 2.
    STREAM LINES, PATHLINES AND STREAK LINES • Streamlines: an imaginary curve or line in the flow field so that the tangent to the curve at any point represents the direction of the instantaneous velocity at that point • Stream lines can never intersect each other and can not be observed in experiments Streamlines around an air foil and upper lower stream tubes
  • 3.
    STREAM LINE, PATHLINE AND STREAK LINE • Streakline: is the locus of the temporary locations of all particles that have passed though a fixed point in the flow field at any instant of time • can be observed in experimental flow visualization • Dye line Streak line used to visualize the flow around a car inside a wind tunnel
  • 4.
    ONE’, TWO’’, THREE’’’DIMENSIONAL FLOW One dimensional flow: All the flow parameters may be expressed as functions of time and one space coordinate only Example: the fully-developed flow through a pipe
  • 5.
    ONE’, TWO’’, THREE’’’DIMENSIONAL FLOW In reality, flow is never one-dimensional because viscosity causes the velocity to decrease to zero at the solid boundaries Two dimensional flow: All the flow parameters are functions of time and two space coordinates (say x and y)
  • 6.
    ONE’, TWO’’, THREE’’’DIMENSIONAL FLOW Three dimensional flow: The hydrodynamic parameters are functions of three space coordinates and time.
  • 7.
    BASIC LAWS OFCONSERVATION • Conservation of mass (continuity equation) • Conservation of momentum (Newton’s second law of motion) • Conservation of energy (First law of thermodynamics) • involve equation of state and fluid properties, physical properties etc.
  • 8.
    CONSERVATION OF MASS– THE CONTINUITY EQUATION •
  • 9.
    QUESTIONS • Find thedepth of point below sea water surface where the pressure intensity is 404.8 kN/m2 . The specific gravity of sea water is given to be 1.03. • Solution hint: Total pressure on the surface, P = Weight of liquid above the immersed surface = Specific weight of liquid * Volume of liquid = Specific weight of liquid * area of the surface * depth of the liquid OR Intensity of the pressure at the base (point) per unit area = sp. wt. * depth
  • 10.
    QUESTIONS • A soapbubble 50 mm in diameter has an internal pressure in excess of the outside pressure of 30 N/mm2 . Calculate the surface tension in the film of the soap bubble. • Solution hint: Consider the equilibrium of the upper hemisphere of the drop, • the upward force on the plane face ABCD is , Fup = Pπr • the surface tension force acting downward along the • circumference (ABCD) = T 2πr • A soap bubble has two liquid surfaces in contact with air, one inside the bubble and another outside the bubble, at equilibrium, Pπr = T 2πr
  • 11.
    BERNOULLI'S EQUATION • Bernoulli'sprinciple: " For a perfect incompressible liquid, flowing in a continuous stream, the total energy of a particle remains the same, while the particle moves from one point to another."
  • 13.
  • 14.
  • 15.
  • 16.
    VENTURI METER • Usesand applications: