‫جمعة‬ ‫هيثم‬
‫امحمد‬
‫عبدالحفيظ‬
022162296
MODELING OF TRANSIENT FLUID
FLOW IN THE SIMPLE PIPELINE
SYSTEMS
Abstact
In this paper, a program was developed to study the hydraulic
shock in a simple pipe system (water hammer program).
Numerical analysis in the transition process of the selected
model is made by changing the spatial and temporal steps of
integration
 a number of hydraulic shocks - water hammer are analyzed.
The frontal movement of the fluid pressure was also analyzed,
depending on the speed of interruption, pressure and time.
the obtained results are presented in tabular form and in diagrams
What is Water Hammer??
Water hammer is a pressure surge or wave resulting when a fluid in
motion is forced to stop or change the velocity
A water hammer commonly occurs when a valve closes suddenly at
an end of a pipeline system, and a pressure wave propagates in the
pipe. It is also called hydraulic shock.
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
Effects of Water Hammer
• Damage to pipes, fittings, and valves, or any connected equipment
causing leaks and shortening the life of the system
Damage to pipes, fittings, and valves, or any connected equipment
causing leaks and shortening the life of the system
Bursting of pipes can occur if the pressure is high enough
Water hammer can have devastating effects on pump system
• n
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
0
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
Table-1. Simulation results according to the
WH Program - transient state of calculation
• n
methodology
The WH program will be tested in these directions:
 The pipe location in the grid system of piping, and
 The closing time of the valve.
The impact of the pipe location in the grid system of pipeline
• The most critical element is the one at the bottom of the pipeline,
that is, the one connected to the valve in that position, which in our
case belongs to the number 5, namely, its end or the entrance to the
valve.
• Valve closing time
The influence of the closing time of the valve will be checked in the
system according to Figure-2 with different closing times: t = 6 s; t = 12
s; t = 18 s and t = 24 s, assuming linear and instantaneous change of
speeds. The simulation calculation results, according to the current
valve closing model presented in Figure-5, are shown for the closing
time: t = 12 s and t = 24 s
• The opening-closing time is simulated with different closing times: t=6
s; t=12 s; t=18 s; t=24 s and t=36 s, while the results are presented
only for t=18 s.
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx
CONCLUSIONS
• The construction of reliable and efficient piping systems represents a
large investment cost due to the number of protective elements to be
installed to keep the system safe from non-stationary phenomena
• The terms for one-dimensional fluid flow, with the introduction of
assumptions and simplifications, are quite complex, therefore
computer programs are used to calculate fluid flow parameters
• Computer programs for the simulation of stationary and non-
stationary fluid flow have made great progress in the construction
and protection of piping systems precisely due to the possibility of
calculating impact parameters due to non-stationary phenomena
• By installing the pressure vessel into the system, the desired effect of
hydraulic shock reduction has been achieved, but it is necessary to
pay attention to the correct dimensioning of the hydraulic shock.
REFERENCES
[1] J.A. Fox. 1979. Hydraulic analysis of unsteady flow in pipe networks
(London, the Macmillan Press, LTD, Second Ed.).
[2] W.R. Fox, T.A. McDonald. 1988. Introduction to the fluid mechanics
(John Wiley & Sons, INC, Fifth Edition).
[3] Xh. Berisha. 2005. Analysis and Synthesis of Work Regimes for
Thermal Networks, Doctoral Thesis, University of Pristina, Faculty of
Mechanical Engineering, Pristina, Kosovo
MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx

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MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE [Autosaved].pptx

  • 2. MODELING OF TRANSIENT FLUID FLOW IN THE SIMPLE PIPELINE SYSTEMS
  • 3. Abstact In this paper, a program was developed to study the hydraulic shock in a simple pipe system (water hammer program). Numerical analysis in the transition process of the selected model is made by changing the spatial and temporal steps of integration  a number of hydraulic shocks - water hammer are analyzed. The frontal movement of the fluid pressure was also analyzed, depending on the speed of interruption, pressure and time.
  • 4. the obtained results are presented in tabular form and in diagrams
  • 5. What is Water Hammer?? Water hammer is a pressure surge or wave resulting when a fluid in motion is forced to stop or change the velocity A water hammer commonly occurs when a valve closes suddenly at an end of a pipeline system, and a pressure wave propagates in the pipe. It is also called hydraulic shock.
  • 10. Effects of Water Hammer • Damage to pipes, fittings, and valves, or any connected equipment causing leaks and shortening the life of the system Damage to pipes, fittings, and valves, or any connected equipment causing leaks and shortening the life of the system Bursting of pipes can occur if the pressure is high enough Water hammer can have devastating effects on pump system
  • 11. • n
  • 15. 0
  • 19. Table-1. Simulation results according to the WH Program - transient state of calculation • n
  • 20. methodology The WH program will be tested in these directions:  The pipe location in the grid system of piping, and  The closing time of the valve.
  • 21. The impact of the pipe location in the grid system of pipeline
  • 22. • The most critical element is the one at the bottom of the pipeline, that is, the one connected to the valve in that position, which in our case belongs to the number 5, namely, its end or the entrance to the valve. • Valve closing time The influence of the closing time of the valve will be checked in the system according to Figure-2 with different closing times: t = 6 s; t = 12 s; t = 18 s and t = 24 s, assuming linear and instantaneous change of speeds. The simulation calculation results, according to the current valve closing model presented in Figure-5, are shown for the closing time: t = 12 s and t = 24 s
  • 23. • The opening-closing time is simulated with different closing times: t=6 s; t=12 s; t=18 s; t=24 s and t=36 s, while the results are presented only for t=18 s.
  • 25. CONCLUSIONS • The construction of reliable and efficient piping systems represents a large investment cost due to the number of protective elements to be installed to keep the system safe from non-stationary phenomena • The terms for one-dimensional fluid flow, with the introduction of assumptions and simplifications, are quite complex, therefore computer programs are used to calculate fluid flow parameters • Computer programs for the simulation of stationary and non- stationary fluid flow have made great progress in the construction and protection of piping systems precisely due to the possibility of calculating impact parameters due to non-stationary phenomena
  • 26. • By installing the pressure vessel into the system, the desired effect of hydraulic shock reduction has been achieved, but it is necessary to pay attention to the correct dimensioning of the hydraulic shock.
  • 27. REFERENCES [1] J.A. Fox. 1979. Hydraulic analysis of unsteady flow in pipe networks (London, the Macmillan Press, LTD, Second Ed.). [2] W.R. Fox, T.A. McDonald. 1988. Introduction to the fluid mechanics (John Wiley & Sons, INC, Fifth Edition). [3] Xh. Berisha. 2005. Analysis and Synthesis of Work Regimes for Thermal Networks, Doctoral Thesis, University of Pristina, Faculty of Mechanical Engineering, Pristina, Kosovo