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Properties of Fluids for  Fluid Mechanics P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Basic Steps  to Design………….
Continuum Hypothesis ,[object Object],[object Object],[object Object],[object Object]
Static Fluid For a static fluid Shear Stress should be zero. For A generalized Three dimensional fluid Element, Many forms of shear stress is possible.
One dimensional Fluid Element +X +  +Y u=0 u=U
Fluid Statics ,[object Object],[object Object],[object Object],[object Object],[object Object],X Y Z  xy  xz  yz  yx  zx  zy
Stress Tensor X Y Z  yy  zz  yz  yx  zx  zy  xx  xy  xz  xz
First Law of Pascal Proof ?
Simple Non-trivial Shape of A Fluid Element
 
 
 
 
 
 
 
Fluid Statics for Power Generation P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Steps for Design of Flow Devices………….
Pressure Variation with Elevation ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],1st order Taylor series estimate for pressure variation over dz
 
[object Object],[object Object],[object Object],[object Object]
Pressure Variation for a Uniform-Density Fluid
 
Reading Material ,[object Object],[object Object],[object Object],[object Object]
Pressure Variation for Compressible Fluids Basic equation for pressure variation with elevation Pressure variation equation can be integrated for  γ (p,z) known.  For example, here we solve for the pressure in the atmosphere assuming  ρ (p,T) given from ideal gas law, T(z) known, and g  ≠  g(z).
 
Draft Required to Establish Air Flow   Air in   Flue gas out
Natural Draft H chimney T atm T gas A B p A =  p ref +  p Z ref, ,p ref
 
H chimney T atm T gas A B p A =  p ref +  p Z ref, ,p ref
Pressure variations in Troposphere: Linear increase towards earth surface T ref  & p ref   are known at  Z ref .  Adiabatic Lapse rate : 6.5 K/km
Reference condition: At Z ref  : T=T ref  & p = p ref
Pressure at A: Pressure variation inside chimney differs from atmospheric pressure. The variation of chimney pressure depends on temperature variation along Chimney. Temperature variation along chimney depends on rate of cooling of hot gas Due to natural convection. Using principles of Heat transfer, one can calculate, T gas (Z). If this is also linear: T = T ref,gas  +    (Z ref -Z). Lapse rate of gas,   gas  is obtained from heat transfer analysis.
Natural Draft ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Pressure Measurement Another Application of Fluid Statics
Pressure Measurement Pressure is an important variable in fluid mechanics and many instruments have been devised for its measurement. Many devices are based on hydrostatics such as barometers and manometers, i.e., determine pressure through measurement of a column (or columns) of a liquid using the pressure variation with elevation equation for an incompressible fluid.
PRESSURE ,[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object]
Manometers U Tube Inverted  U Tube Enlarged Leg Two Fluid Inclined Tube
U-tube or differential manometer Right Limb fluid statics : Left Limb fluid statics : Point 3 and 2 are at the same elevation and same fluid
Gauge Pressure:
Absolute, Gauge & Vacuum Pressures System Pressure Atmospheric Pressure Gauge Pressure Absolute Pressure Absolute zero pressure
Absolute, Gauge & Vacuum Pressures System Pressure Atmospheric Pressure Vacuum Pressure Absolute Pressure Absolute zero pressure
Stress Tensor for A Static Fluid 0 0 0 0 0 0 X Y Z  yy  zz  xx
An important Property of A Fluid under Motion
Shear stress (  :  Tangential force on per unit area of contact    between solid & fluid
 
 
 
Elasticity (Compressibility) ,[object Object],[object Object]
 
 
Surface Tension ,[object Object],[object Object],[object Object]
 
Vapour Pressure ,[object Object],[object Object],[object Object],[object Object]
 

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Fm 3

  • 1. Properties of Fluids for Fluid Mechanics P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Basic Steps to Design………….
  • 2.
  • 3. Static Fluid For a static fluid Shear Stress should be zero. For A generalized Three dimensional fluid Element, Many forms of shear stress is possible.
  • 4. One dimensional Fluid Element +X +  +Y u=0 u=U
  • 5.
  • 6. Stress Tensor X Y Z  yy  zz  yz  yx  zx  zy  xx  xy  xz  xz
  • 7. First Law of Pascal Proof ?
  • 8. Simple Non-trivial Shape of A Fluid Element
  • 9.  
  • 10.  
  • 11.  
  • 12.  
  • 13.  
  • 14.  
  • 15.  
  • 16. Fluid Statics for Power Generation P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Steps for Design of Flow Devices………….
  • 17.
  • 18.  
  • 19.
  • 20. Pressure Variation for a Uniform-Density Fluid
  • 21.  
  • 22.
  • 23. Pressure Variation for Compressible Fluids Basic equation for pressure variation with elevation Pressure variation equation can be integrated for γ (p,z) known. For example, here we solve for the pressure in the atmosphere assuming ρ (p,T) given from ideal gas law, T(z) known, and g ≠ g(z).
  • 24.  
  • 25. Draft Required to Establish Air Flow Air in Flue gas out
  • 26. Natural Draft H chimney T atm T gas A B p A = p ref +  p Z ref, ,p ref
  • 27.  
  • 28. H chimney T atm T gas A B p A = p ref +  p Z ref, ,p ref
  • 29. Pressure variations in Troposphere: Linear increase towards earth surface T ref & p ref are known at Z ref .  Adiabatic Lapse rate : 6.5 K/km
  • 30. Reference condition: At Z ref : T=T ref & p = p ref
  • 31. Pressure at A: Pressure variation inside chimney differs from atmospheric pressure. The variation of chimney pressure depends on temperature variation along Chimney. Temperature variation along chimney depends on rate of cooling of hot gas Due to natural convection. Using principles of Heat transfer, one can calculate, T gas (Z). If this is also linear: T = T ref,gas +   (Z ref -Z). Lapse rate of gas,  gas is obtained from heat transfer analysis.
  • 32.
  • 33. Pressure Measurement Another Application of Fluid Statics
  • 34. Pressure Measurement Pressure is an important variable in fluid mechanics and many instruments have been devised for its measurement. Many devices are based on hydrostatics such as barometers and manometers, i.e., determine pressure through measurement of a column (or columns) of a liquid using the pressure variation with elevation equation for an incompressible fluid.
  • 35.
  • 36.
  • 37. Manometers U Tube Inverted U Tube Enlarged Leg Two Fluid Inclined Tube
  • 38. U-tube or differential manometer Right Limb fluid statics : Left Limb fluid statics : Point 3 and 2 are at the same elevation and same fluid
  • 40. Absolute, Gauge & Vacuum Pressures System Pressure Atmospheric Pressure Gauge Pressure Absolute Pressure Absolute zero pressure
  • 41. Absolute, Gauge & Vacuum Pressures System Pressure Atmospheric Pressure Vacuum Pressure Absolute Pressure Absolute zero pressure
  • 42. Stress Tensor for A Static Fluid 0 0 0 0 0 0 X Y Z  yy  zz  xx
  • 43. An important Property of A Fluid under Motion
  • 44. Shear stress (  : Tangential force on per unit area of contact between solid & fluid
  • 45.  
  • 46.  
  • 47.  
  • 48.
  • 49.  
  • 50.  
  • 51.
  • 52.  
  • 53.
  • 54.  

Notas do Editor

  1. Barometric pressure is actual atmospheric pressure