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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume: 3 | Issue: 3 | Mar-Apr 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 - 6470
@ IJTSRD | Unique Paper ID – IJTSRD23381 | Volume – 3 | Issue – 3 | Mar-Apr 2019 Page: 1459
Comparative CFD and Simulative Analysis of Flow
Behaviour to Calculate Losses in Different Geometrical Pipes
Er. Ajay Rana1, Er. Nishant Kumar2
1M.tech Scholar, 2Assistant Professor
1,2Department of Mechanical Engineering, Universal Group of Institutions, Lalru, Punjab, India
How to cite this paper: Er. Ajay Rana |
Er. Nishant Kumar "Comparative CFD
and Simulative Analysis of Flow
Behaviour to Calculate Losses in
Different Geometrical Pipes" Published
in International Journal of Trend in
Scientific Research and Development
(ijtsrd), ISSN: 2456-
6470, Volume-3 |
Issue-3, April 2019,
pp.1459-1462, URL:
https://www.ijtsrd.c
om/papers/ijtsrd23
381.pdf
Copyright © 2019 by author(s) and
International Journal of Trend in
Scientific Research and Development
Journal. This is an Open Access article
distributed under
the terms of the
Creative Commons
Attribution License (CC BY 4.0)
(http://creativecommons.org/licenses/
by/4.0)
ABSTRACT
In order to transport the fluid effectively without suffering much energy loss it
becomes very important to understand the frictional losses in fluid flow. And
here basically two very crucial types of Losses are discussed such as Major
Energy Loss ( this occur due to friction) and other one is Minor Energy Loss (
this is due to sudden expansion, sudden contraction and bend in a pipe). This
study will focus on calculating Losses likeMajor and Minorloss in turbulentfluid
flow through pipes of different geometries (expansion, contraction and bend).
And the whole study will be performed using three different techniques:- firstly
being experimentally performed in Fluid Mechanics & Machinery Laboratory,
secondly at nodal centre of IIT DELHI using programme Virtual Labs, a project
initiated by the MHRD, Govt. of India, and thirdly using ANSYS FLUENT a
simulation and modelling software. The results obtained by using the three
above discussed methods would be used for result validation and pointing the
most effective method to calculate losses in flow through pipes.
KEYWORDS: Major Loss, Minor Loss, CFD, Fluent, ANSYS, Virtual Lab.
INTRODUCTION
Transporting of Fluids through piping network is very
common in industries throughout the world; here fluid
and gases are transported from one point to another. The
pressure loss depends on the type of flow of the fluid in
the network, pipe material, and the fluid flowing through
the pipe. When any fluid flows through a pipe, the velocity
adjacent to the pipe wall is zero and the velocity gradually
increases from the wall to the centre of pipe. Maximum
velocity is observed at the centre of the pipe. Due to
increase in the velocity gradient, shear stresses are
produced in the fluid due to its viscosity. This viscous
action attributes to loss of energy which is commonly
known as loss due friction or frictional loss.
A pipe is a closed conduitthroughwhichfluidflowsunderthe
pressure. When in the pipe, fluidflows,some of energy is lost
to overcome hydraulic resistance which is basically caused
due to:-
1. The viscous friction effect associated with molecules of
fluid itself.
2. The local resistance which resultfromflowdisturbances
caused by sudden expansion and contraction in pipe.
3. Obstruction in the form of valves, elbows and other pipe
fittings or Curves and bend in the pipe.
4. Entrance and exit disturbances.
5. Due to resistance between the viscous surface of liquid
and surrounding pipe surface.
A. TYPES OF FLUID FLOWS
1. Laminar flow: -
The type of flow is critical in fluid dynamics to solve any
problems. Laminar flow that is also sometimes called as
streamline flow occurs when a fluid particle flows in a
straight line parallel to a pipe walls comparatively with
low velocity without any disturbance between the layers.
Reynolds number is an important parameter to know the
type of flow in the tube. The flow with Reynolds number
less than 2300 is considered to be a Laminar flow for a
pipe. In laminar flow, the velocity, pressure and other
flow properties at each point in fluid remain constant.
This kind of flow is rare in practice in water systems.
2. Turbulent flow: -
It is a type of flow in which fluids undergoes irregular
fluctuations and mixing. The magnitude and direction are
continuously changing in the turbulent flow due to the
speed of fluid at a point. The flow of wind and rivers are
the example of this kind of flow. Reynolds number is
greater than 4000 and has high velocity in this flow. It is
the most common type of flow and has to face the
difficulty to view with an open eye, fluctuations are very
IJTSRD23381
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23381 | Volume – 3 | Issue – 3 | Mar-Apr 2019 Page: 1460
difficult to detect, and laser can be used for the detection.
Mathematical analysis for this flow is very difficult, so
experimental measurements are applied.
3. Transitional flow: -
It is a type of flow with the medium velocity having the
Reynolds number greater than 2300 and lesser than
4000.
B. LOSSES IN FLOW THROUGH PIPES
When a fluid flow through a pipe, the fluid experiences
some resistance due to which there are some loss in
energy of fluid.
This loss of energy is classified as:
1. Major Energy losses
A. Darcy-Weisbach formula
2. Minor losses
A. Bend in Pipe
B. Sudden contraction
C. Sudden expansion
D. Pipe fitting
C. FORMULAS FOR CALCULATION OF LOSSES IN
FLOW THROUGH PIPES
1. Darcy-Weisbach formula:-
Where,
= loss in head due to friction in unit of length
f= friction factor
D = Pipe Diameter
V = Flow velocity
2. Minor losses;-
Where K is the loss coefficient
2.1 Loss of head due to sudden expansion
2.2 Loss due to sudden contraction
2.3 Loss of head due to bend in pipe
D. OBJECTIVES OF STUDY
The main objectives of study are:-
Calculation of Major loss using Darcy’s equation for
measuring frictional losses.
Calculation of the minor losses (due to sudden
expansion, sudden contraction and bend) for
measuring variation in velocity and pressure.
Study effect of Pipe Material and Fluid Viscosity on
fluid flow.
Results validation and comparison for predicting the
most effective technique for calculation of losses in
fluid flow through pipes.
E. EXPERIMENTAL SETUP
Fig.1:- shows experimental apparatus for pipe losses
F. THEORETICAL FORMULATION (USING VIRTUAL
LABS)
Fig2:- shows process of Virtual Labs(Theoretical Results)
for pipe losses
G. RESULT ANALYSIS
S.
No
Diameter
of Pipe
Experiment
Results
Virtual/
Theoretical
Results
CFD
Results
1 0.050 0.101 0.490 0.3715
2 0.040 0.035 0.325 0.310
3 0.025 0.002 0.029 0.027
Table:- 1 shows comparison of results for Major Losses
S.No
Head
Loss
Diameter
Of Pipe
Experiment
Results
Virtual/
Theoretical
Results
1 He
0.025-
0.050
0.336 0.2973
2 Hc
0.050-
0.025
0.756 0.2825
3 Hb 0.05 0.0615 0.0551
Table:-2 shows comparison of results for minor losses
H. BAR CHART ANALYSIS
Fig.3:- shows comparison of results for Major Losses
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23381 | Volume – 3 | Issue – 3 | Mar-Apr 2019 Page: 1461
Fig.4:- shows comparison of results for Minor Losses
I. CFD ANALYSIS
Computational Fluid Dynamics (CFD) is the simulation of
fluids engineering systems using modeling (mathematical
physical problem formulation) and numerical methods
(discretization methods, solvers, numerical parameters,
and grid generations, etc.) Here, FLUENT workbench was
used for making the analysis.
I.1 SAMPLE CFD PROCESS
In this a sample of cfd process is shown using figures,
each geometry consist of 4 figures. And as our study was
related to Straight Pipe, Sudden expansion, Sudden
Contraction and Sudden Bend so these will makea total of
12 such photos. So for illustrative purpose only Sudden
Bend figures are shown.
I.2 Modeling
Fig.5:- shows modelling for Bent Pipe
I.3 Meshing
Fig.6:- shows meshing for Bent Pipe
I.4 Pressure
Fig.7:- shows pressure contours for Bent Pipe
I.5 Velocity
Fig.8:- shows velocity contours for Bent Pipe
J. CONCLUSION
1. Frictional Loss co-efficient is more in Virtual Lab
results than the result obtained from experiments
and ANSYS. In this the results obtained from both
ANSYS and Virtual/Theoretical are almost same.
2. Loss co-efficient of expansion is more in experimental
results than the result obtained from Virtual Lab and
ANSYS . In this the results obtained from both ANSYS
and Virtual/Theoretical are almost same.
3. Loss co-efficient of contraction is slightly more in
experimental results than the result obtained from
Virtual Lab and ANSYS. In this the results obtained
from both ANSYS and Virtual/Theoretical are almost
same
4. Loss co-efficient of bends is slightly more in
experimental results than the result obtained from
Virtual Lab and ANSYS. In this the results obtained
from both ANSYS and Virtual/Theoretical are almost
same.
5. Finally concluded that ANSYS has an edge over the
other methods as it is flexible to change according to
need and generates results more close to theoretical
results. And is free from experimental errors that
happen due to friction and leakages etc.
K. FUTURE SCOPE
1. Study of program with thermal effect
2. FEM Analysis of pipe flow and comparing with FDM
Analysis result in case when Dynamic Viscosity,
Laminar flow that are dependent on Temperature.
3. Varying effect study with change in length of pipe
4. Varying effect study with change in material of pipe
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23381 | Volume – 3 | Issue – 3 | Mar-Apr 2019 Page: 1462
L. REFERENCES
[1] L. Halsan, B. nodea “Description on Turbulentflow in
fluid dynamics, assessed online on 10.10.2014”,
http://www.efm.leeds.ac.uk/CIVE/CIVE1400/Sectio
n4/laminar_turbulent.htm
[2] H. Schlichting, K. Gersten (2003), eighth edition,
Boundary-Layer Theory, chapter 9, description of
dimensionless Prandtl number, page 210
[3] Y. A. engel; J. M. Cimbala (2010), Fluid mechanics:
fundamentals and applications, Chapter 8, Flow in
Pipes, description about entrance region and figure,
page 325
[4] A. Holland and R. Bragg. (1973). Fluid Flow for
Chemical and Process Engineers (2nd
ed.)[Online].Available:http://site.ebrary.com.ezprox
y.arcada.fi:2048/lib/arcada/docDetail.action?docID
=10206495&p00
[5] A. engel; J. M. Cimbala (2010), Fluid mechanics:
fundamentals and applications, Chapter 8, Flow in
Pipes, Darcy‟s equation for the calculation of Head
loss in ful-ly developed circular pipe, page 330
[6] A. engel; J. M. Cimbala (2011), Fluid mechanics:
fundamentals and applications, Chapter 8, Flow in
Pipes, description about turbulent flows in pipe and
figure, page 335
[7] H. Schlichting, K. Gersten (2003), eighth edition,
Boundary-Layer Theory, chapter 9, description of
dimensionless Prandtl number, page 210

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Comparative CFD and Simulative Analysis of Flow Behaviour to Calculate Losses in Different Geometrical Pipes

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume: 3 | Issue: 3 | Mar-Apr 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 - 6470 @ IJTSRD | Unique Paper ID – IJTSRD23381 | Volume – 3 | Issue – 3 | Mar-Apr 2019 Page: 1459 Comparative CFD and Simulative Analysis of Flow Behaviour to Calculate Losses in Different Geometrical Pipes Er. Ajay Rana1, Er. Nishant Kumar2 1M.tech Scholar, 2Assistant Professor 1,2Department of Mechanical Engineering, Universal Group of Institutions, Lalru, Punjab, India How to cite this paper: Er. Ajay Rana | Er. Nishant Kumar "Comparative CFD and Simulative Analysis of Flow Behaviour to Calculate Losses in Different Geometrical Pipes" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456- 6470, Volume-3 | Issue-3, April 2019, pp.1459-1462, URL: https://www.ijtsrd.c om/papers/ijtsrd23 381.pdf Copyright © 2019 by author(s) and International Journal of Trend in Scientific Research and Development Journal. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (CC BY 4.0) (http://creativecommons.org/licenses/ by/4.0) ABSTRACT In order to transport the fluid effectively without suffering much energy loss it becomes very important to understand the frictional losses in fluid flow. And here basically two very crucial types of Losses are discussed such as Major Energy Loss ( this occur due to friction) and other one is Minor Energy Loss ( this is due to sudden expansion, sudden contraction and bend in a pipe). This study will focus on calculating Losses likeMajor and Minorloss in turbulentfluid flow through pipes of different geometries (expansion, contraction and bend). And the whole study will be performed using three different techniques:- firstly being experimentally performed in Fluid Mechanics & Machinery Laboratory, secondly at nodal centre of IIT DELHI using programme Virtual Labs, a project initiated by the MHRD, Govt. of India, and thirdly using ANSYS FLUENT a simulation and modelling software. The results obtained by using the three above discussed methods would be used for result validation and pointing the most effective method to calculate losses in flow through pipes. KEYWORDS: Major Loss, Minor Loss, CFD, Fluent, ANSYS, Virtual Lab. INTRODUCTION Transporting of Fluids through piping network is very common in industries throughout the world; here fluid and gases are transported from one point to another. The pressure loss depends on the type of flow of the fluid in the network, pipe material, and the fluid flowing through the pipe. When any fluid flows through a pipe, the velocity adjacent to the pipe wall is zero and the velocity gradually increases from the wall to the centre of pipe. Maximum velocity is observed at the centre of the pipe. Due to increase in the velocity gradient, shear stresses are produced in the fluid due to its viscosity. This viscous action attributes to loss of energy which is commonly known as loss due friction or frictional loss. A pipe is a closed conduitthroughwhichfluidflowsunderthe pressure. When in the pipe, fluidflows,some of energy is lost to overcome hydraulic resistance which is basically caused due to:- 1. The viscous friction effect associated with molecules of fluid itself. 2. The local resistance which resultfromflowdisturbances caused by sudden expansion and contraction in pipe. 3. Obstruction in the form of valves, elbows and other pipe fittings or Curves and bend in the pipe. 4. Entrance and exit disturbances. 5. Due to resistance between the viscous surface of liquid and surrounding pipe surface. A. TYPES OF FLUID FLOWS 1. Laminar flow: - The type of flow is critical in fluid dynamics to solve any problems. Laminar flow that is also sometimes called as streamline flow occurs when a fluid particle flows in a straight line parallel to a pipe walls comparatively with low velocity without any disturbance between the layers. Reynolds number is an important parameter to know the type of flow in the tube. The flow with Reynolds number less than 2300 is considered to be a Laminar flow for a pipe. In laminar flow, the velocity, pressure and other flow properties at each point in fluid remain constant. This kind of flow is rare in practice in water systems. 2. Turbulent flow: - It is a type of flow in which fluids undergoes irregular fluctuations and mixing. The magnitude and direction are continuously changing in the turbulent flow due to the speed of fluid at a point. The flow of wind and rivers are the example of this kind of flow. Reynolds number is greater than 4000 and has high velocity in this flow. It is the most common type of flow and has to face the difficulty to view with an open eye, fluctuations are very IJTSRD23381
  • 2. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23381 | Volume – 3 | Issue – 3 | Mar-Apr 2019 Page: 1460 difficult to detect, and laser can be used for the detection. Mathematical analysis for this flow is very difficult, so experimental measurements are applied. 3. Transitional flow: - It is a type of flow with the medium velocity having the Reynolds number greater than 2300 and lesser than 4000. B. LOSSES IN FLOW THROUGH PIPES When a fluid flow through a pipe, the fluid experiences some resistance due to which there are some loss in energy of fluid. This loss of energy is classified as: 1. Major Energy losses A. Darcy-Weisbach formula 2. Minor losses A. Bend in Pipe B. Sudden contraction C. Sudden expansion D. Pipe fitting C. FORMULAS FOR CALCULATION OF LOSSES IN FLOW THROUGH PIPES 1. Darcy-Weisbach formula:- Where, = loss in head due to friction in unit of length f= friction factor D = Pipe Diameter V = Flow velocity 2. Minor losses;- Where K is the loss coefficient 2.1 Loss of head due to sudden expansion 2.2 Loss due to sudden contraction 2.3 Loss of head due to bend in pipe D. OBJECTIVES OF STUDY The main objectives of study are:- Calculation of Major loss using Darcy’s equation for measuring frictional losses. Calculation of the minor losses (due to sudden expansion, sudden contraction and bend) for measuring variation in velocity and pressure. Study effect of Pipe Material and Fluid Viscosity on fluid flow. Results validation and comparison for predicting the most effective technique for calculation of losses in fluid flow through pipes. E. EXPERIMENTAL SETUP Fig.1:- shows experimental apparatus for pipe losses F. THEORETICAL FORMULATION (USING VIRTUAL LABS) Fig2:- shows process of Virtual Labs(Theoretical Results) for pipe losses G. RESULT ANALYSIS S. No Diameter of Pipe Experiment Results Virtual/ Theoretical Results CFD Results 1 0.050 0.101 0.490 0.3715 2 0.040 0.035 0.325 0.310 3 0.025 0.002 0.029 0.027 Table:- 1 shows comparison of results for Major Losses S.No Head Loss Diameter Of Pipe Experiment Results Virtual/ Theoretical Results 1 He 0.025- 0.050 0.336 0.2973 2 Hc 0.050- 0.025 0.756 0.2825 3 Hb 0.05 0.0615 0.0551 Table:-2 shows comparison of results for minor losses H. BAR CHART ANALYSIS Fig.3:- shows comparison of results for Major Losses
  • 3. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23381 | Volume – 3 | Issue – 3 | Mar-Apr 2019 Page: 1461 Fig.4:- shows comparison of results for Minor Losses I. CFD ANALYSIS Computational Fluid Dynamics (CFD) is the simulation of fluids engineering systems using modeling (mathematical physical problem formulation) and numerical methods (discretization methods, solvers, numerical parameters, and grid generations, etc.) Here, FLUENT workbench was used for making the analysis. I.1 SAMPLE CFD PROCESS In this a sample of cfd process is shown using figures, each geometry consist of 4 figures. And as our study was related to Straight Pipe, Sudden expansion, Sudden Contraction and Sudden Bend so these will makea total of 12 such photos. So for illustrative purpose only Sudden Bend figures are shown. I.2 Modeling Fig.5:- shows modelling for Bent Pipe I.3 Meshing Fig.6:- shows meshing for Bent Pipe I.4 Pressure Fig.7:- shows pressure contours for Bent Pipe I.5 Velocity Fig.8:- shows velocity contours for Bent Pipe J. CONCLUSION 1. Frictional Loss co-efficient is more in Virtual Lab results than the result obtained from experiments and ANSYS. In this the results obtained from both ANSYS and Virtual/Theoretical are almost same. 2. Loss co-efficient of expansion is more in experimental results than the result obtained from Virtual Lab and ANSYS . In this the results obtained from both ANSYS and Virtual/Theoretical are almost same. 3. Loss co-efficient of contraction is slightly more in experimental results than the result obtained from Virtual Lab and ANSYS. In this the results obtained from both ANSYS and Virtual/Theoretical are almost same 4. Loss co-efficient of bends is slightly more in experimental results than the result obtained from Virtual Lab and ANSYS. In this the results obtained from both ANSYS and Virtual/Theoretical are almost same. 5. Finally concluded that ANSYS has an edge over the other methods as it is flexible to change according to need and generates results more close to theoretical results. And is free from experimental errors that happen due to friction and leakages etc. K. FUTURE SCOPE 1. Study of program with thermal effect 2. FEM Analysis of pipe flow and comparing with FDM Analysis result in case when Dynamic Viscosity, Laminar flow that are dependent on Temperature. 3. Varying effect study with change in length of pipe 4. Varying effect study with change in material of pipe
  • 4. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23381 | Volume – 3 | Issue – 3 | Mar-Apr 2019 Page: 1462 L. REFERENCES [1] L. Halsan, B. nodea “Description on Turbulentflow in fluid dynamics, assessed online on 10.10.2014”, http://www.efm.leeds.ac.uk/CIVE/CIVE1400/Sectio n4/laminar_turbulent.htm [2] H. Schlichting, K. Gersten (2003), eighth edition, Boundary-Layer Theory, chapter 9, description of dimensionless Prandtl number, page 210 [3] Y. A. engel; J. M. Cimbala (2010), Fluid mechanics: fundamentals and applications, Chapter 8, Flow in Pipes, description about entrance region and figure, page 325 [4] A. Holland and R. Bragg. (1973). Fluid Flow for Chemical and Process Engineers (2nd ed.)[Online].Available:http://site.ebrary.com.ezprox y.arcada.fi:2048/lib/arcada/docDetail.action?docID =10206495&p00 [5] A. engel; J. M. Cimbala (2010), Fluid mechanics: fundamentals and applications, Chapter 8, Flow in Pipes, Darcy‟s equation for the calculation of Head loss in ful-ly developed circular pipe, page 330 [6] A. engel; J. M. Cimbala (2011), Fluid mechanics: fundamentals and applications, Chapter 8, Flow in Pipes, description about turbulent flows in pipe and figure, page 335 [7] H. Schlichting, K. Gersten (2003), eighth edition, Boundary-Layer Theory, chapter 9, description of dimensionless Prandtl number, page 210