Advanced Hydrodynamic Problem - University level

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SUMMARY

The forum discussion revolves around calculating the necessary force of a hydraulic piston to empty a 48 m³ tank in 25 seconds. The calculations involve fluid dynamics principles, including hydrostatic pressure, localized and continuous head losses, and the effects of dynamic viscosity and density of water at 20 degrees Celsius. The initial force estimate was approximately 3000 kN, but further analysis revealed a total force requirement of 2650 kN, factoring in various pressure drops and the need to compress air in a closed system. The discussion emphasizes the importance of accurate velocity calculations and understanding pressure gradients throughout the process.

PREREQUISITES
  • Fluid dynamics principles, including Bernoulli's equation and Darcy's formula
  • Hydrostatic pressure calculations and their implications in hydraulic systems
  • Understanding of Reynolds number and its significance in flow characterization
  • Basic mechanical engineering concepts related to hydraulic systems and piston mechanics
NEXT STEPS
  • Study the application of Bernoulli's equation in hydraulic systems
  • Learn about the Darcy-Weisbach equation for calculating head loss in pipes
  • Investigate the effects of compressible flow in closed systems
  • Explore advanced fluid dynamics simulations using software like ANSYS Fluent
USEFUL FOR

This discussion is beneficial for mechanical engineers, hydraulic system designers, and students studying fluid dynamics, particularly those working on advanced hydrodynamic calculations and piston-driven systems.

  • #31
erobz said:
No, in Bernoullis the flow is invisicid. If the flow was inviscid the force on the piston to evacuate the tank at any rate would simply be the weight of the vertical water column.
ok thanks for the answer, then it is not enough to calculate reynolds and determine if the motion is turbulent or laminar and consider the frictions accordingly? ok then of the inviscid fluids, this part of physics I think I have never done it

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  • #32
Hydro2022 said:
ok thanks for the answer, then it is not enough to calculate reynolds and determine if the motion is turbulent or laminar and consider the frictions accordingly? ok then of the inviscid fluids, this part of physics I think I have never done it

View attachment 316515
These are viscous flows. It is like that. You will calculate the Reynolds Number, and refer to the Moody Diagram to determine the friction factor for each section of pipe.The Energy Equation: (It looks like Bernoulli's, but they are different).

$$ \frac{P_1}{\gamma} + z_1 + \alpha\frac{V_1^2}{2g} + h_p = h_t + \frac{P_2}{\gamma} + z_2 + \alpha\frac{V_2^2}{2g} + \sum_{1 \to 2} h_{loss} $$

##h_p## is pump head
##h_t## is turbine head
## \alpha## is the kinetic energy correction factor (turbulent flow ## \alpha \approx 1.05## , laminar flow ##\alpha = 2##)
## \sum h_{loss}## is the total head loss between ##(1)## to ##(2)##

You are also going to use continuity for incompressible flow:

$$Q = V_1 A_1 = V_2 A_2$$

You are going to simplify what is above, and solve for ##P_1##, which will be the pressure acting over the surface of the piston.
 
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  • #33
erobz said:
These are viscous flows. It is like that. You will calculate the Reynolds Number, and refer to the Moody Diagram to determine the friction factor for each section of pipe.The Energy Equation: (It looks like Bernoulli's, but they are different).

$$ \frac{P_1}{\gamma} + z_1 + \alpha\frac{V_1^2}{2g} + h_p = h_t + \frac{P_2}{\gamma} + z_2 + \alpha\frac{V_2^2}{2g} + \sum_{1 \to 2} h_{loss} $$

##h_p## is pump head
##h_t## is turbine head
## \alpha## is the kinetic energy correction factor (turbulent flow ## \alpha \approx 1.05## , laminar flow ##\alpha = 2##)
## \sum h_{loss}## is the total head loss between ##(1)## to ##(2)##

You are also going to use continuity for incompressible flow:

$$Q = V_1 A_1 = V_2 A_2$$

You are going to simplify what is above, and solve for ##P_1##, which will be the pressure acting over the surface of the piston.
ok thank you very much for the formula you are really helping me to solve the problem I am getting closer to the solution, but hp and ht where I find these data because I don't have a pump or a turbine in the problem/hydraulic scheme :)
 
  • #34
Hydro2022 said:
ok thank you very much for the formula you are really helping me to solve the problem I am getting closer to the solution, but hp and ht where I find these data because I don't have a pump or a turbine in the problem/hydraulic scheme :)
If there is no pump or turbine between the points of interest i.e. the outlet of lower tank and inlet of upper tank, then those terms are zero.
 
  • #35
erobz said:
If there is no pump or turbine between the points of interest i.e. the outlet of lower tank and inlet of upper tank, then those terms are zero.
ok thank you very much now I try to calculate with this formula, just a last thing sorry
1667330110530.png

the y in the image here attached (sorry but on the keyboard i don't know how to write it) what it is ? and Z it is the piezometric height right ? in this case would be 100 m the maximum height that the water reaches ? Am I correct ?
sorry to ask so many questions but as you can see I am really bad at physics :(

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  • #36
Hydro2022 said:
ok thank you very much now I try to calculate with this formula, just a last thing sorry View attachment 316536
the y in the image here attached (sorry but on the keyboard i don't know how to write it) what it is ? and Z it is the piezometric height right ? in this case would be 100 m the maximum height that the water reaches ? Am I correct ?
sorry to ask so many questions but as you can see I am really bad at physics :(

View attachment 316537
##\gamma## (gamma) is the specific weight of the fluid. ##\gamma = \rho g##

## z## is the static elevation head for the point of reference. I would take ##z_1 = 0##.
 
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  • #37
@erobz
I tried to calculate the pressure with the equation but I can't solve it as unfortunately I have two unknowns both P1 that of the tank but also P2 that is the pressure inside the 250 mm diameter pipe. Do you think there is anothe way to calculate the pressure ?

thanks in advance

luckily I have another 2 weeks before I have to submit the exercise

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  • #38
##P_2## is 0 gauge. You should be taking point 1 as the entrance of the 0.9 m diameter pipe. Point 2 should be the exit of the 0.25 m pipe. We are assuming the upper tank is at atmospheric pressure (0 gauge).

The only issue that you would need to split it up for, is if the flow in the large 0.9 m pipe is laminar. We know the flow in the 0.25 m pipe is turbulent.
 
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  • #39
erobz said:
##P_2## is 0 gauge. You should be taking point 1 as the entrance of the 0.9 m diameter pipe. Point 2 should be the exit of the 0.25 m pipe. We are assuming the upper tank is at atmospheric pressure (0 gauge).

The only issue that you would need to split it up for, is if the flow in the large 0.9 m pipe is laminar. We know the flow in the 0.25 m pipe is turbul

erobz said:
##P_2## is 0 gauge. You should be taking point 1 as the entrance of the 0.9 m diameter pipe. Point 2 should be the exit of the 0.25 m pipe. We are assuming the upper tank is at atmospheric pressure (0 gauge).

The only issue that you would need to split it up for, is if the flow in the large 0.9 m pipe is laminar. We know the flow in the 0.25 m pipe is turbulent.
@erobz
ok I tried again with the calculation, I eliminated from the equation the factors that are not present in the problem, so z1 / hp / ht / P2 as it is 0.
formula 1.png

formula 2.png

V1 = 3.02 m / s (speed in the section of 0.9 m) calculated with the flow rate of 1.92 m3 / s
V2 = 39.2 m / s (speed in the section of 0,25m) calculated from the flow rate of 1.92 m3 / s
With these speeds I calculated the continuous and localized pressure drops for a total of 500 meters of water column

in the end the formula comes to me like this

formula 3.PNG


where x = P1

in the end the result is P1 = 6 670 000 Pascal
 

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  • #40
@erobz
this pressure now to get the Force I have to multiply it by which surface? that of the tank therefore 48 m2 or that of the 0.9 m section where the water comes out of the tank?
thank you

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  • #41
because if I multiply it by the area with a diameter of 0.9 meters, the result is a force of 4235 kN
while if I multiply it by the surface of the tank comes a monstrous force of 320 000 kN

the first solution is the one that comes closest to the true result of 11,000 kN

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  • #42
maybe we are getting closer to the solution I hope so

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  • #43
Hydro2022 said:
@erobz
this pressure now to get the Force I have to multiply it by which surface? that of the tank therefore 48 m2 or that of the 0.9 m section where the water comes out of the tank?
thank you

View attachment 316768
It should be multiplied by the piston surface area. We are ignoring head losses in the tank.
 
  • #44
If you completely ignore head losses it comes out to about ## \approx 85 \cdot 10^3 \, \rm{kN}##. Clearly there is a serious issue.

The static elevation head alone is well over the supposed answer.

$$F_{z} = z_2 \cdot \rho \cdot g \cdot A = 100 \rm{m} \cdot 997 \rm{\frac{kg}{m^3}} \cdot 9.81 \rm{\frac{m}{s^2}} \cdot 48\rm{m^2} \approx 47 \cdot 10^3 \rm{kN}$$
 
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  • #45
erobz said:
If you completely ignore head losses it comes out to about ## \approx 85 \cdot 10^3 \, \rm{kN}##. Clearly there is a serious issue.

The static elevation head alone is well over the supposed answer.

$$F_{z} = z_2 \cdot \rho \cdot g \cdot A = 100 \rm{m} \cdot 997 \rm{\frac{kg}{m^3}} \cdot 9.81 \rm{\frac{m}{s^2}} \cdot 48\rm{m^2} \approx 47 \cdot 10^3 \rm{kN}$$
thank you very much for your answer I really appreciate your help, I will try to understand why the result is much lower than the monstrous value we get

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  • #46
Hydro2022 said:
thank you very much for your answer I really appreciate your help, I will try to understand why the result is much lower than the monstrous value we get

View attachment 316781
I don't think you are going to be able too. Are you sure it's not ##110,000 \, \rm{kN}##? What I showed was simply the force on the cylinder to simply hold the ##100 \rm{m}## column statically was practically 5 times the quoted result of ##11,000 \rm{kN}##. That is as low as the force could possibly get. The result of ##11,000 \rm{kN}## is unattainable.
 
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  • #47
erobz said:
If you completely ignore head losses it comes out to about ## \approx 85 \cdot 10^3 \, \rm{kN}##. Clearly there is a serious issue.

The static elevation head alone is well over the supposed answer.

$$F_{z} = z_2 \cdot \rho \cdot g \cdot A = 100 \rm{m} \cdot 997 \rm{\frac{kg}{m^3}} \cdot 9.81 \rm{\frac{m}{s^2}} \cdot 48\rm{m^2} \approx 47 \cdot 10^3 \rm{kN}$$
only a doubt, in the calculation of the hydrostatic force of 47 000 kN, the force is vertical, why the surface of the 0.25 m is not considered but is multiplied by the entire surface of the tank? the force does not act vertically at the base of the tube of 0,25 m?
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  • #48
Hydro2022 said:
only a doubt, in the calculation of the hydrostatic force of 47 000 kN, the force is vertical, why the surface of the 0.25 m is not considered but is multiplied by the entire surface of the tank? the force does not act vertically at the base of the tube of 0,25 m?View attachment 316785
You need to review hydrostatic pressure if you are having conceptual difficulty with that part. You should be well beyond that in coursework if you are expected to solve these problems.
 
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  • #49
Hydro2022 said:
only a doubt, in the calculation of the hydrostatic force of 47 000 kN, the force is vertical, why the surface of the 0.25 m is not considered but is multiplied by the entire surface of the tank? the force does not act vertically at the base of the tube of 0,25 m?View attachment 316785
The diameter of the pipes carrying the flowing water are only relevant when estimating the resistance that those present to that flow.
Only the height of the vertical column of water matters, regarding hydrostatic (non-moving fluid) pressure.

Please, see:
https://en.wikipedia.org/wiki/Torricelli's_law

https://en.wikipedia.org/wiki/Pascal's_law

Not considering the final pressure of the compressed air in the spherical top tank (assuming that the top tank is open to the atmosphere), the value of the static pressure along the horizontal line that runs through the centers of the blue tank, the 0.9 m diameter pipe and the horizontal section and elbow of the 0.25 m diameter pipe would be the same: ##980.64~kPa## or ##980.64~N/m^2##.

Since ##P=F/A##, that pressure would push the ##48~m^2## piston with a force of ##47040~kN##.

Yes, the walls of the 0.25 m diameter pipe will be "feeling" that same pressure, as well as the masses of fluid located directly forward and after that section.

Please, see:
https://courses.lumenlearning.com/suny-osuniversityphysics/chapter/14-1-fluids-density-and-pressure/

8KIEY0t.jpg
 
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  • #50
Perhaps the length of the vertical pipe could be 10 meters rather than 100?
A 10-meter water column would induce a static pressure of ##98.06 ~kN/m^2## on the piston.

Please, see attached PDF drawing at scale to appreciate the real dimensions of the problem as shown at post #1.
 

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