Monday, December 23, 2013

1.0 PROPERTIES OF FLUIDS


1.1 WHAT IS FLUIDS?
  • Liquids and gases are both fluids
  • a fluid is any substance that flows and takes the shape of its container.


  • If the fluids are at rest, the study of them is called fluid statics
  • If the fluids are in motion, the study of them is called fluid dynamics.
  • —The science and technology of the mechanical properties of liquids is called hydraulics. 
  • Similarly, the science and technology of the mechanical properties of air and other gases is called pneumatics.



1.2 THERMODYNAMIC PROPERTIES OF A FLUID
1.2.1 DENSITY

  • The density of a fluid is its mass per unit volume:
                                       
  • Liquids are essentially incompressible 
  • Density is highly variable in gases nearly proportional to the pressure. 



  • Note: specific volume is defined as:




1.2.2 SPECIFIC WEIGHT
  • The specific weight of a fluid is its weight, , per unit volume. Density and specific weight are related by gravity: 


1.2.3 SPECIFIC GRAVITY

  • Specific gravity is the ratio of a fluid density to a standard reference fluid, typically water at 4˚C (for liquids) and air (for gases):
  • For example, the specific gravity of mercury is SGHg = 13,580/1000 = 13.6


1.2.4 VISCOSITY
  • Viscosity is a measure of a fluid’s resistance to flow. It determines the fluid strain rate that is generated by a given applied shear stress. 

  • Temperature has a strong and pressure has a moderate effect on viscosity. The viscosity of gases and most liquids increases slowly with pressure.
                                              
  • A Newtonian fluid has a linear relationship between shear stress and velocity gradient:

  • The no‐slip condition: at the wall velocity is zero relative to the wall This is The no slip condition: at the wall velocity is zero relative to the wall. This is a characteristic of all viscous fluid.
  • The shear stress is proportional to the slope of the velocity profile and is greatest at the wall greatest at the wall.


1.2.5 SURFACE TENSION
  • A liquid, being unable to expand freely, will form an interface with a second liquid or gas.

  • The cohesive forces between liquid molecules are responsible for the phenomenon known as surface tension. 
  • Surface tension Υ (pronounced upsilon) has the dimension of force per unit length (N/m) or of energy per unit area (J/m2). 
  • Υair‐water = 0.073 N/m; Υair‐mercury = 0.48 N/m

  • Using a force balance, pressure increase in the interior of a liquid half‐cylinder droplet of length L and radius R is:

  • Contact angle θ appears when a liquid interface intersects with a solid surface.
  • Water is extremely wetting to a clean glass surface with θ≈0. For a clean mercury‐air‐glass interface, θ≈130°.