Is the Bernoulli Equation enough to determine pump selection?

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Discussion Overview

The discussion revolves around the application of the Bernoulli Equation in the context of pump selection, particularly focusing on how to account for elevation changes when determining the required pump head and flow rate. Participants explore the implications of energy balances in fluid systems, addressing both theoretical and practical aspects of pump operation.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant illustrates an energy balance using the Bernoulli Equation but expresses concern that it does not adequately account for significant elevation changes when selecting a pump.
  • Another participant suggests performing two separate energy balances: one from the initial point to the top and another from the top to the bottom, indicating a need for simultaneous solutions.
  • Some participants note that the Bernoulli Equation allows for comparisons between any two points along the flow, but elevation changes may introduce complexities that need to be addressed separately.
  • There is a discussion about the pump's operational head and how it relates to the actual height the liquid must be raised, with some arguing that the pump only needs to consider the flow and head at its discharge point.
  • Concerns are raised about potential issues such as startup problems and flow separation in the system, suggesting that simple Bernoulli flow may not be sufficient for complete analysis.
  • One participant mentions that the analysis differs between positive displacement pumps and non-positive displacement pumps, indicating a need for different approaches based on pump type.
  • There is a debate about the mechanics of how water can be moved up and down in the system, with some suggesting that the flow dynamics can allow for effective pumping even when the pump head appears insufficient at first glance.

Areas of Agreement / Disagreement

Participants express differing views on the adequacy of the Bernoulli Equation for pump selection, particularly regarding elevation changes and the dynamics of fluid flow. There is no clear consensus, as multiple competing perspectives on the analysis and application of the equation are presented.

Contextual Notes

Participants highlight limitations in the analysis, including the need for conditional reasoning based on specific system configurations and the distinction between different types of pumps. The discussion reflects the complexity of real-world applications of theoretical principles.

Who May Find This Useful

Engineers, fluid dynamics researchers, and students involved in pump selection and fluid mechanics may find this discussion relevant to their work and studies.

Tom Hardy
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Here is an illustration of something that came into my head:

http://imgur.com/a/V9V8S

(also attached to question)

If we do a energy balance (in terms of head) between point 1 and point 2 (ignoring friction for now, it's not really important):

$$\frac{P_1}{\rho g} + \frac{v^2_1}{2g} + z_1 + h_p = \frac{P_2}{\rho g} + \frac{v^2_2}{2g} + z_2 $$

Assume the pressure is the same so..:

$$ h_p = \bigg( \frac{v^2_2}{2g} - \frac{v^2_1}{2g} \bigg) + (z_2 - z_1)$$

Fine, but this is what I have an issue with, the end result doesn't really take into account the huge distance the liquid has to go up by. When I'm trying to choose a pump, I have to pick an operating head and flow rate. The issue is, the above equation could give me a required pump head that's very small say 5m or something. If the big distance the liquid has to go up is 100m, this 5m head pump won't provide, so how do I pick a pump in this case?
 

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I think I should just do two balances, first one for 1 to the top, and then another balance from the top to the bottom and solve simultaneously

Edit: So if I do a balance between the top and point 3, I can work out the required velocity at the top I need to get for the whatever I want at the bottom, and then I can solve for pump head at point 1.
 
Tom Hardy said:
I think I should just do two balances, first one for 1 to the top, and then another balance from the top to the bottom and solve simultaneously
You can do that...you might find they combine and simplify via subtraction...

Bernoulli's is a conservation of energy statement. That means you can compare/equate any two points along the flow with it. If you are uncomfortable with how the flow looks at other points, you are welcome to throw them into the analysis as well.

As someone who selects pumps from time to time, I will say that there is a potential hidden issue with elevation changes, as pumps require a certain amount of positive suction head.
 
russ_watters said:
You can do that...you might find they combine and simplify via subtraction...

Bernoulli's is a conservation of energy statement. That means you can compare/equate any two points along the flow with it. If you are uncomfortable with how the flow looks at other points, you are welcome to throw them into the analysis as well.

As someone who selects pumps from time to time, I will say that there is a potential hidden issue with elevation changes, as pumps require a certain amount of positive suction head.

Ah, there's the issue. At the end, if I do the subtraction, I'll be left with $$(z_3 - z_2)$$ as my change in height term. This completely ignores the fact the pump has to raise the liquid to $$z_2$$. So when I'm looking at a pump operating curve, I may pick something that's operating at say, 5m of head and this is fine if I didn't have to take the liquid up to a height greater than 5m.

The only way I see to deal with this, is to solve the two separately. First I can can solve for the velocity I need at the top to get the velocity I want at the bottom, then once I have this velocity, I can just get the proper value for required pump head.
 
Tom Hardy said:
Ah, there's the issue. At the end, if I do the subtraction, I'll be left with $$(z_3 - z_2)$$ as my change in height term. This completely ignores the fact the pump has to raise the liquid to $$z_2$$. So when I'm looking at a pump operating curve, I may pick something that's operating at say, 5m of head and this is fine if I didn't have to take the liquid up to a height greater than 5m.
No, I do think you missed the second step of the logic: the pump only cares about the water flowing into it. It doesn't care where the water has been. So the up and down has no impact on the pump. The fact that the up and down simplifies right out of the equation reflects that reality.

In your case, since you are on the discharge side, you don't have the issue I mentioned with suction head.
 
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russ_watters said:
No, I do think you missed the second step of the logic: the pump only cares about the water flowing into it. It doesn't care where the water has been. So the up and down has no impact on the pump. The fact that the up and down simplifies right out of the equation reflects that reality.

In your case, since you are on the discharge side, you don't have the issue I mentioned with suction head.

I think you misread my diagram, the water is coming from the left, and it still has to go up and down. It has not gone up and down yet
 
Tom Hardy said:
I think you misread my diagram, the water is coming from the left, and it still has to go up and down. It has not gone up and down yet
?? I'm not sure what I am missing; the flow arrows definitely appear to be pointing to the left...
 
russ_watters said:
?? I'm not sure what I am missing; the flow arrows definitely appear to be pointing to the left...

Right the flow is going to to the left, so it goes up and down after the pump
 
Tom Hardy said:
Right the flow is going to to the left, so it goes up and down after the pump
Ok, so the pump only cares about the flow and head it sees at the discharge. The specifics of the system further downstream don't matter to it except for how they impact the flow and head (and as you found, the up and down part subtracts itself out).
 
  • #10
russ_watters said:
Ok, so the pump only cares about the flow and head it sees at the discharge. The specifics of the system further downstream don't matter to it except for how they impact the flow and head (and as you found, the up and down part subtracts itself out).

I get that, but the thing is, say the 'big distance' is REALLY big, how will a 5m head pump be able to pump water up 200m? If I got rid of the part where it comes back down, the pump would not work, so why does it magically work when I add the part where it goes down?
 
  • #11
(1) Many possible problems with this configuration . Most common are :

Start up problem where the pump may have to build up a head of fluid in the initially empty riser pipe .

Flow separation in the cross over pipe at the top .

(2) There are two distinct cases to analyse for the steady state condition . They are where :

The back pressure at the final outlet is relatively high .

The back pressure at the final outlet is relatively low or atmospheric .

(3) Note that :

Simple Bernoulli flow may not be adequate to analyse this problem completely .

The analysis with a positive displacement pump is different from the analysis with a non positive displacement pump .
 
Last edited:
  • #12
Nidum said:
(1) Many possible problems with this configuration . Most common are :

Start up problem where the pump may have to build up a head of fluid in the initially empty riser pipe .

Flow separation in the cross over pipe at the top .

(2) There are two distinct cases to analyse for the steady state condition . They are where :

The back pressure at the final outlet is relatively high .

The back pressure at the final outlet is relatively low or atmospheric .

(3) Note that :

Simple Bernoulli flow may not be adequate to analyse this problem completely .

The analysis with a positive displacement pump is different from the analysis with a non positive displacement pump .

It's a centrifugal pump
 
  • #13
Too many conditional answers needed to deal with this type of problem in abstract . Draw up a plausible real system for us to look at ?
 
  • #14
Tom Hardy said:
I get that, but the thing is, say the 'big distance' is REALLY big, how will a 5m head pump be able to pump water up 200m?
Let's stay at 5m for a sec: the answer is that it doesn't have to. The water flowing up is pulled up by the water flowing down the other side, like a siphon.

If you go higher/lower than 10m though you may run into a problem where the water flowing down the other side pulls a vacuum.
 
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  • #15
russ_watters said:
If you go higher/lower than 10m though you may run into a problem where the water flowing down the other side pulls a vacuum.

+1
 
  • #16
Nidum said:
Too many conditional answers needed to deal with this system in abstract . Draw up a plausible real system for us to look at ?
russ_watters said:
Let's stay at 5m for a sec: the answer is that it doesn't have to. The water flowing up is pulled up by the water flowing down the other side, like a siphon.

If you go higher/lower than 10m though you may run into a problem where the water flowing down the other side pulls a vacuum.

Ah, I see, so the only issue at the start is priming the system so that a siphon exists?
 
  • #17
For very large rise and fall heights it is common practice to separate the down going flow from the up going flow using a big header tank .

Bad second choice solution is to put a restrictor at bottom of down pipe .
 
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  • #18
Nidum said:
For very large rise and fall heights it is common practice to separate the down going flow from the up going flow using a big header tank .

Bad second choice solution is to put a restrictor at bottom of down pipe .

Thanks, it's not really large in reality, it was just the concept I was confused about.
 
  • #19
Tom Hardy said:
Ah, I see, so the only issue at the start is priming the system so that a siphon exists?
Yes! If the system is not pre-filled, and is filled with that pump, the pump will have to overcome the entire head of the rise.
 
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