Parallel pipes and the size of pizzas When is 8+8 not equal to 16 and what has that got to do with Luigi’s Trattoria and the size of its pizzas? Pump expert Harry Rosen unravels the relationship between flow rate, pipe area and velocity and the effect these values can have on the friction losses of a piping system.
I recently worked on a pumping project where the engineer sizing the pipeline thought that rather than specifying one 16" pipe, he would use two 8" pipes in parallel. Simple mathematics suggests this should be OK, i.e. 8+8=16. Half the flow goes through each smaller pipe and so the velocity in the smaller pipes should be the same as the velocity in the large pipe. Wrong! I also had a heated debate with one of my pump course delegates who could not grasp the relationship between the increase in fric- tion losses through a pipe and the velocity in the pipeline. In the end I realised he was getting stuck on the difference between flow rate and velocity. Both of the above cases got me wondering whether one of the basic principles of pump systems is actually misunderstood – the re- lationship between flow rate, pipe area and velocity. The formula for flow through a pipe says that Flow (Q) equals fluid velocity times pipe area (Q=vA). This means that with constant flow, if we halve the area we would double the velocity. In our case we would be halving the flow rate in the smaller pipes, therefore the velocity would remain unchanged. This is what the engineer was counting on when he pro- posed two 8" pipes rather than one 16" pipe. But he was probably confusing area with pipe diameter, and we know the formula for area of a pipe A =D2/4. Area is proportional to diameter squared, so what effect does this have on the velocity? Let’s take a step back and replace the pipes with pizza, we should all know (at least sub-consciously) that the area of an 8" pizza is a lot smaller than half the area of the 16" size. Think of how big a 16" pizza would be (watch any American TV show and you will often see them eating one of these monster pizzas). Our largest pizza is around 12", which is only around half as big (because of area) as the 16". That is why pizzas increase in small increments of diameter as the relationship between pizza size (area) and diameter is a squared relationship. This means that an 8" pizza is one quarter the size (area) of a 16" pizza, not half the size, which also means the area of the 8" pipe is only one quarter the area of the 16" pipe! It follows that installing two 8” pipes (or buying two small pizzas) only gives you half the area of the original 16" pipe, the equivalent of halving
was to pump out of a submerged pit, which made the suction friction losses even more critical. In terms of NPSH (net positive suc- tion head) and cavitation, the 4 m of friction reduced the NPSH available in the system by 4 m, which became less than the NPSH required by the pump, resulting in the brand new pump cavitating the first time it was operated. Back to the consultants, and the good news that they did learn from their mistake. A single 16" diameter suction pipe was installed and the suction problems disappeared. When it came to sizing the discharge piping, 1 250 m of overland pipeline, they did not make the same mistake and selected one pipe with a 16” diameter. If they had gone for two pipes, they would have two 12" pipes to give the same friction loss as the single 16" pipe. This doesn't sound like a lot, but we happen to be referring make matters worse, using a self-priming pump to pump w now suddenly a problem application in terms of NPSH (net The 4 m of friction reduces the NPSH available in the system brand new pump cavitating the first time it is operated. Back to the consultants, and the good news that they did le diameter suction pipe was installed and the suction problem the discharge piping, 1 250 m of overland pipeline, they did selected one pipe with a 16" diameter. If they had gone for pipes to give the same friction loss as the single 16" pipe. So if friction is proportional to velocity squared, and velocit it follows that increase in friction is proportional to reductio actually to the 5 th power as you will see the derivation. Sma very large increases in friction loss. So pipe friction in a pipe diameter reduces, way steeper than even the COVID curve [Set in box] The derivation of the relationship between pipe friction an ! " =$× ' & × ( ) *+ and ,= - . = /× - 0 1 ) ⇒ ,∝ ' 4 ) , * ∝ ' 4 1 ⇒ ! " ∝ ' 4 5 f : Friction loss in m; f: friction factor; L: length of pipe; d: d gravitational acceleration; A: area. [End box] H f : Friction loss in m; f: friction factor; L: length of pipe; d: diameter of pipe; v: flow velocity; g: gravitational acceleration; A: area. The derivation of the relationship between pipe friction and internal pipe diameter And twice the velocity is bad. Really bad. Think of the COVI growing exponentially, surging upwards at ridiculously stee friction in a pipeline as the velocity increases, which it will i The equation for friction loss within a pipeline states that fr squared, so small increases in velocity create large increase quadruple the friction and in our suction pipe design above the system must now handle losses of over 4 m.
On a centrifugal pump curve, the increase in friction head pushes the pump back on its curve toward shut off, resulting in reduced flow rate.
the pizza area of the monster 16”. Why is the area so important? Well, that is easy to answer for pizza as you are going to end up hungry if you were expecting the equivalent of a large 16" pizza when buying two 8" pizzas. But this is where the pizza anal- ogy breaks down, so back to the humdrum of pumping systems. When we have two parallel pipes of half the diameter, we get half the flow rate going through each pipe, but one quarter the area for each pipe. To maintain the continuity equa- tion for flow (Q=vA) at half the flow rate, the velocity in the smaller pipes will be double the velocity of the one large pipe. And twice the velocity is bad. Really bad. Think of the COVID curve, with the rate of infections growing exponentially, surging upwards at ridiculously steep rates. This is what happens with friction in a pipeline as the velocity increases, which it will if the diameter reduces. The equation for friction loss within a pipeline states that friction is proportional to velocity squared, so small increases in velocity create large increases in friction. Doubling the velocity will quadruple the friction and in our suction pipe design above, instead of around 1 m of friction loss, the system must now handle losses of over 4 m. This doesn’t sound like a lot, but the prob- lem piping in this case was on the suction side of the pump. And even worse, the application
6 ¦ MechChem Africa • July-August 2022
Why is this important? We are not talking about new system and system designers are aware of this relationship and sho It is much more of an issue with existing systems and what
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