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FLUID MECHANICS


                       c.         Inverted Differential U-Tube Manometer


                              Now consider an inverted differential manometer whose two ends are connected

                       to two different points A and B. Let us assume that the pressure at point A is more than

                       that at point B, a greater pressure at A will force the light liquid in the inverted U-tube to

                       move  upwards.  This  upward  movement  of  liquid  in  the  left  limb  will  cause  a
                       corresponding fall of the light liquid in the right limb as shown in Figure 3.12. Let us take

                       C-D as the datum line in this case.






















                                                   Figure 3.12 : Inverted Differential Manometer


                       We know that pressures in the left limb and right limb below the datum line are equal.



                                          p
                                Pressure   C  at C =  Pressure p
                                                                D

                                at D

                                   For the left right limb :  p =  p −  P h
                                                                        2
                                                          D
                                                                B
                                                                       h 
                                 For the left hand limb :  p =  p −  P 1  −  Q h
                                                           C
                                                                A
                                  since,       p =  p
                                                     D
                                                C
                                  p −   P h −  Q h =  p −  P h 2
                                                        B
                                           1
                                   A
                                                  2
                                      p −  p =   P h −  P h −  Q h
                                       B
                                                                   2
                                                           1
                                                    2
                                            A








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