Centrifugal Pumps

 

Example:  (Cont.)

 

Step 2:  Conservation of mass:  mass flow rate at entrance equals mass flow rate at exit

 

                     

 

   dm/dt  =   ρ A1 Vr1  =  ρ A2 Vr2     which yields:  Q  =  2π r1 b1 Vr1  =  2π r2 b2 Vr2 

 

So the radial components of fluid velocity are:    Vr1 = Q / 2π r1 b1    and  Vr2 = Q / 2π r2 b2     

 

Vr1 = Q / 2π r1 b1   = 28.6 ft/sec   and   Vr2 = Q / 2π r2 b2    =  19 ft/sec

 

Also   r1 ω  =  66.66  ft/sec         and   r2 ω  =  100.0  ft/sec        

 

From the vector diagram on the left:    tan β1  =  Vr1 / r1 ω  =  28.6 / 66.66  =  0.43

 

So                  β1  =  23.3o    (result)

 

 

Step 3:  Conservation of angular momentum    T =  ρQ [ r2Vt2 ]

 

From the vector diagram on the left note that  Vt2  = 0.  From the vector diagram on the right:

 

         Vt2  =  r2 ω  ˗  W2 cos β2    =  r2 ω  ˗  Wt2

 

Note here   Vr2  =  Wr2   and  tan β2  =  Wr2 / Wt2     So that  Wt2   =  Wr2 / tan β2 

 

         Vt2   =  r2 ω  ˗  Wr2 / tan β2  =   r2 ω  ˗  Vr2 / tan β2             Since  Vr2 =  Wr2

 

 

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