Page 213 - WCS - Electrical
P. 213

WORKSHOP CALCULATION & SCIENCE  - CITS



           EXERCISE 19 : Introduction to Fluid Mechanics



           Heat & Temperature
           Introduction
           The Fluid Mechanics is the branch of engineering science which deals with the behavior of fluids systems also the
           action of forces on the fluids and corresponding flow patterns.
           Fluid
           Any substance which is capable to flow is called as fluid.

           Fluid is a substance that deform continuously under the action of shear stress, no matter if it is small
           It has no definite shape of its own, but confirms to the shape of the container.
           Fluid consists of liquid and gases.
           Example: breathing, drinking, blood circulation  in the human body,  Fluid is everywhere, in the ocean, in the
           atmosphere and around the aircraft or a missile etc.
           Liquids and Gases
           Liquid
           Fluids, which are not able to compress, but possess a definite volume, which are not affected appreciably by the
           change in pressure and temperature is called as liquid. e.g. Water, Kerosene, Petrol etc
           A liquid being composed of relatively closed-packed molecules with strong cohesive forces tends to retain its
           volume and will form a free surface in gravitational field or in container
           Gases
           A fluid which are compressible and posses no definite volume, it is compressed or expands at any change in
           temperature is called as gases, e.g. Air, Ammonia, CO, etc. Gas molecules are widely spaced with negligible
           cohesive forces, so that it is free to expand until it encounters confining walls
           Fluid Properties
           Density or Mass Density

           The density of a liquid is defined as the mass per unit volume.
    Weight  m  m.g
            p.g
 vγ =  =  =  = It is denoted by “p” (rho). S.1. unit is kg/m².
 Volume  v  v
           Mass density of water is 1000kg/m².
                                               Mass     m
    Volume  v                             P =         =
 v =  =                                       Volume    v
 Weight  m
           Weight Density or Specific Weight or Unit Density
           The specific weight of a fluid is defined as weight per unit volume at a valet temperature and pressure.
    Volume  v
 v  =  =   It is denoted by ‘w’ or ‘Y’ (gamma). It has S.1. unit is N/m². Specific weight of water is 9810 N/m² (9.81kN/m²).
 2  Mass  m
                                    Weight   m   m.g
           Weight W Y= Volume vγ =          =   =    = p.g
  Density  of   any  substance      Volume    v    v
 Density  of  water   at 4    c °

                                                                                          Mass
                                                                                                   m
           The specific weight is depends on gravitational acceleration and the mass density, S gravitational attraction varies

                                                                                                 =
                                       Volume
                                                                                     P =
                                                 v
           from place to place, the specific weight will also vary                       Volume    v
                                              =
                                   v =
    du                                 Weight   m
 τα        Specific weight of pure water under standard atmospheric pressure of 76 cm of mercury at mean sea level and
 dy        a temperature of 4°C, is 9810 N/m
                                      Volume    v
  du                             v  =         =
 dy                               2    Mass     m
    τ
 μ  =                          Density  of   any  substance
  du 
                           Density  of  water   at  4    c °  200
  dy 
           2                           τα du
 μ =    Shear   stress  =  N/m  =  Newton   sec  dy
   Change   of  Velocity   m/s  2
              m
  Change   of   distance   m         du
                                       dy

  Dyne.sec                           μ =  τ
 cm 2                                  du 
                                          
                                       dy  
  Newton   sec
 m 2
                                                      2
   1                     μ =      Shear   stress  =  N/m  =  Newton   sec
 100                           Change   of  Velocity    m/s  m  2

                              Change   of   distance    m
  Force
 Area                                Dyne.sec

                                       cm 2

                                   Newton   sec
                                       m 2
                                       1
                                     100


                                    Force
                                    Area
   208   209   210   211   212   213   214   215   216   217   218