Page 97 - Industrial Ventilation Design Guidebook
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62                                                  CHAPTER 4 PHYSICAL FUNDAMENTALS

                     When k = 0.03 mm, the ratio k/d — 0.000 375, and therefore the friction
                                                                 5
                  factor £ 01 = 0.0193. Correspondingly, Re 13 = 10 xlO  and £ 13 = 0.0196.
                     The formula for pressure loss is




                  The dimensioning of pipe 3-4 happens by means of Eqs. (4.68) and (4.70).
                  The iteration equation is now




                  Calculations are dealt with in the following stages

                      1. d 4 is chosen.
                     2. Re and k/d 4 are calculated.
                     3. £ 54 is read from the Moody chart as a function of Re and k/d 4_
                     4. A new d 4 is calculated with Eq. (4.71) until the d 4 value is
                        suitable.
                  Calculations are best carried out in a tabular form. The value of d 4 is 29.7 mm.
                  In practice the next larger standard pipe size would be selected.
                     The diameter d 2 is solved analogously. The Bernoulli equation at the in-
                  terval 1-2 is





















                     Example 4
                     A pump lifts water from a lake. At the pump suction entry a foot valve is
                  fitted. Determine the maximum static delivery height the water can be raised
                  without cavitation taking place. The saturation pressure of water is 1.23 kPa
                                                           3     1  1
                  at 10 °C and the dynamic viscosity is 1.3 x 10~  kg nr  s" . The suction pipe
                                       1
                  water velocity is 2.0 m s" , the internal pipe diameter is 100 mm, and the pipe
                  roughness is 0.03 mm. The resistance of the foot valve is 4.5.
                     Note: Cavitation occurs when the pressure at a point in a liquid flow
                  field is equal or less than the vapor pressure of the liquid. At this point
                  bubbles of vapor are formed, this is cavitation. It has serious effects such
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