Pipeflow            (continued)

 

Turbulent Flow through single pipes  -- The energy equation between two sections of pipe is:

or

       P1  +  V12/2g  +  z1  +  dW/dt)/  =  P2  +  V22/2g  +  z2  + HL

 

Here  dW/dt)/  > 0 for pumps and  dW/dt)/   < 0  for turbines

 

Now the “head loss term”, HL, has two parts – the major loss, HL1, and the minor loss, HL2.

 

As before the major head loss is:    HL1  =  (fL/D) (V2/2g)

 

The minor loss  HL2  =  KLV2/2g   where  KL is the loss coefficient which you obtain from

tables for fittings like elbows, bends, tees, valves, entrance sections, reentrant sections, etc.

 

In general there are three types of pipe flow applications.

 

 

Type 1

 

 

The flowrate or average velocity is specified.  Then find the pressure

difference or head loss.  Click for an example.

 

 

 

 

Type 2

 

 

The pressures at sections 1 and 2, P1 and P2 are specified or the head loss

is given.  Then find the flowrate, Q.  The unknowns are the friction factor, f,

the Reynolds Number, and the fluid velocity.  Solve by iteration using a trial and

error solution.  One way is to start with an assumption for f, the friction factor.

Note, you will use the Moody Chart during the solution.  Click to view the

Moody Chart.  Click here for an example.

 

 

 

 

Type 3

 

The pressure drop and flowrate are specified.  Find the required diameter of

the pipe.  The unknowns are friction factor, f, the diameter of the pipe, D,

the relative roughness, ε/D, and the Reynolds Number.  Solve by iteration

using a trial and error solution.  Note, you will use the Moody Chart during

the solution.  Click for an example.

 

 

                                         


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