SlideShare a Scribd company logo
PTE 316
Piping Design
Design Procedure:
The problem of design procedure is to find a pipeline configuration and size
within the constraints which is safe and economical. The steps in pipeline
design are as follows:
The determination of the problem , which includes the characteristics of the
fluid to be carried, including the flow rates and the allowable head loss
The location of the pipes, its source and destination, and terrain over which
it will pass
The design code to be followed and the material to be used.
The determination of a preliminary pipe route, the line length and static
head difference
Pipe diameter based on allowable head loss
Structural analysis such as wall thickness and stress analysis
The stress analysis is performed in pipe configuration until compliance with
the code is achieved.
Pipe types and applications
• Seamless pipes (SMLs): These pipes are extruded and
have no longitudinal seam. There is no weld and it’s
the strongest of the three types
• Electric resistance welded pipe (ERW): These pipes are
manufactured from plates, where the seam weld is
done by electric resistance welding. The welding
efficiency is 0.8
• Submerged arc welded pipe (SAW): These pipes are
manufactured from plates, normally rolled and steam
welded together. The welding has a joint efficiency of
0.95.
Piping design equations.
• Assuming steady state flow, there are a number
of equations which are based upon the general
energy equation, that can be employed to design
the piping systems. Although piping systems and
pipeline design can get complex, the majority of
the design problems encountered by the
engineers can be solved by the standard flow
equations. Typical example is the Bernoulli
equation.
What is Bernoulli's principle?
• Bernoulli's principle is a seemingly counterintuitive
statement about how the speed of a fluid relates to
the pressure of the fluid. Many people feel like
Bernoulli's principle shouldn't be correct, but this
might be due to a misunderstanding about what
Bernoulli's principle actually says. Bernoulli's
principle states the following,
• Bernoulli's principle: Within a horizontal flow of
fluid, points of higher fluid speed will have less
pressure than points of slower fluid speed.
How can you derive Bernoulli's principle?
• Incompressible fluids have to speed up when they reach
a narrow constricted section in order to maintain a
constant volume flow rate. This is why a narrow nozzle
on a hose causes water to speed up. But something
might be bothering you about this phenomenon. If the
water is speeding up at a constriction, it's also gaining
kinetic energy
• The only way to give something kinetic energy is to do
work on it. This is expressed by the work energy
principle.
Bernoulli equation Conti…
Wexternal = Δk = mvf
2
- mvi
2
So if a portion of fluid is speeding up, something
external to that portion of fluid must be doing work
on it. What force is causing work to be done on the
fluid? Well, in most real world systems there are lots
of dissipative forces that could be doing negative
work, but we're going to assume for the sake of
simplicity that these viscous forces are negligible and
we have a nice continuous and perfectly laminar
(streamline) flow.
• Laminar (streamline) flow means that the fluid flows in parallel
layers without crossing paths. In laminar streamline flow there is
no swirling or vortices in the fluid.
• Consider the diagram below which shows water flowing
along streamlines from left to right. As the outlined
volume of water enters the constricted region it speeds
up. The force from pressure P_1P1​
P, start subscript, 1,
end subscript on the left side of the shaded water pushes
to the right and does positive work since it pushes in the
same direction as the motion of the shaded fluid. The
force from pressure P_2P2​
P, start subscript, 2, end
subscript on the right side of the shaded fluid pushes to
the left and does negative work since it pushes in the
opposite direction as the motion of the shaded fluid.
1587415189PTE_POWERPOINT_1.ppt lecture slides
We know that the water must speed up (due to the continuity
equation) and therefore have a net positive amount of work
done on it. So the work done by the force from pressure on
the left side must be larger than the amount of negative work
done by the force from pressure on the right side. This means
that the pressure on the wider/slower side P1 has to be larger
than the pressure on the narrow/faster side P2.
This inverse relationship between the pressure and speed at a
point in a fluid is called Bernoulli's principle.
Bernoulli's principle: At points along a horizontal streamline,
higher pressure regions have lower fluid speed and lower
pressure regions have higher fluid speed.
• The idea that regions where the fluid is
moving fast will have lower pressure can seem
strange. Surely, a fast moving fluid that strikes
you must apply more pressure to your body
than a slow moving fluid, right? Yes, that is
right. But we're talking about two different
pressures now. The pressure that Bernoulli's
principle is referring to is the internal fluid
pressure that would be exerted in all
directions during the flow, including on the
sides of the pipe. This is different from the
pressure a fluid will exert on you if you get in
the way of it and stop its motion.
• Note that Bernoulli's principle does not say that a fast
moving fluid can't have significantly high pressures. It
just says that the pressure in a slower region of that
same flowing system must have even larger pressure
than the faster moving region.
What is Bernoulli's equation?
• Bernoulli's equation is essentially a more general and
mathematical form of Bernoulli's principle that also
takes into account changes in gravitational potential
energy. let's take a look at Bernoulli's equation and get
a feel for what it says and how one would go about
using it.
• Bernoulli's equation relates the pressure, speed, and height of
any two points (1 and 2) in a steady streamline flowing fluid of
density ρ. Bernoulli's equation is usually written as follows,
P1 + 1/2℮v + ℮gh1 = P2 + 1/2℮v + ℮gh2
The variables P1. v1, h1 refer to the pressure, speed, and height
of the fluid at point 1, whereas the variables P2. V2, h2 refer to
the pressure, speed, and height of the fluid at point 2 as seen
in the diagram below. The diagram below shows one
particular choice of two points (1 and 2) in the fluid, but
Bernoulli's equation will hold for any two points in the fluid.
1587415189PTE_POWERPOINT_1.ppt lecture slides
Derivation of Bernoulli's equation
To conti….

More Related Content

PPTX
Bernoulli’s equation and its significance
PPTX
Discussion slide on Bernoulli's Equation and Quantinuity equation
PDF
432491132-Physics-Project-Class-11.pdf bb
PDF
Electronic Measurement Flow Measurement
PDF
Part 2 Revision.pdf
PPTX
II - 2 Class 02.pptx
PPT
Lecture 3 bernoulli_s_theorm_it_s_applications
PDF
Lesson 4 bernoulli's theorem
Bernoulli’s equation and its significance
Discussion slide on Bernoulli's Equation and Quantinuity equation
432491132-Physics-Project-Class-11.pdf bb
Electronic Measurement Flow Measurement
Part 2 Revision.pdf
II - 2 Class 02.pptx
Lecture 3 bernoulli_s_theorm_it_s_applications
Lesson 4 bernoulli's theorem

Similar to 1587415189PTE_POWERPOINT_1.ppt lecture slides (20)

PDF
Flow of fluids
PDF
Bernoulli's Theorem, Limitations & its Practical Application
PDF
Pharmaceutical Engineering: Flow of fluids
PPT
Lecture in open channel flow
PPTX
Introduction to Hydraulics Powerpoint.pptx
PPTX
Lecture 3 (1).pptx
PPTX
Applications of bernoulli equation
PDF
Applications of the Bernoulli Equation
PPTX
PPTX
Flow measurement & vibration
PDF
1 2-2 1 1 1 2 2 1 Solution Bernoullis principle is a seemin.pdf
PPTX
Applications of bernoulli equation.
PPTX
Le3-UnSteady Flow.pptx for fluid mechanics
PDF
Bernoulli Principles 1.pdf
PDF
Fluidflowsb-160915165853 (1).pdf
PPTX
CLASS egarding the flow of fluids how velocity pressure measure 111.pptx
PDF
Flowmeter - Brief
PPTX
Berrnouli equation and applications
PPTX
Bernoullis theorem
PPTX
Flow of Fluids Pharmaceutical Engineering
Flow of fluids
Bernoulli's Theorem, Limitations & its Practical Application
Pharmaceutical Engineering: Flow of fluids
Lecture in open channel flow
Introduction to Hydraulics Powerpoint.pptx
Lecture 3 (1).pptx
Applications of bernoulli equation
Applications of the Bernoulli Equation
Flow measurement & vibration
1 2-2 1 1 1 2 2 1 Solution Bernoullis principle is a seemin.pdf
Applications of bernoulli equation.
Le3-UnSteady Flow.pptx for fluid mechanics
Bernoulli Principles 1.pdf
Fluidflowsb-160915165853 (1).pdf
CLASS egarding the flow of fluids how velocity pressure measure 111.pptx
Flowmeter - Brief
Berrnouli equation and applications
Bernoullis theorem
Flow of Fluids Pharmaceutical Engineering
Ad

More from OkologumeWilfredC (8)

PPT
Fluid Mechanics Comprehensive Lecture Notes_1.ppt
PPTX
4_Petroleum and NG Engineering EA lecture note
PPTX
effect of modified HEC on stability of drilling mud.pptx
PPTX
Investigation of Rubber Seeds Oil as a base Fluid in the Formulation of Oil-b...
PPTX
Introduction to Petroleum Production.pptx
PPT
LESSON_D.ppt oil and gas separation process
PPTX
online-orientation-ppt-mis.pptx for students
PPT
0902lec.ppt analytical environmental chemistry
Fluid Mechanics Comprehensive Lecture Notes_1.ppt
4_Petroleum and NG Engineering EA lecture note
effect of modified HEC on stability of drilling mud.pptx
Investigation of Rubber Seeds Oil as a base Fluid in the Formulation of Oil-b...
Introduction to Petroleum Production.pptx
LESSON_D.ppt oil and gas separation process
online-orientation-ppt-mis.pptx for students
0902lec.ppt analytical environmental chemistry
Ad

Recently uploaded (20)

PPTX
Infosys Presentation by1.Riyan Bagwan 2.Samadhan Naiknavare 3.Gaurav Shinde 4...
PDF
737-MAX_SRG.pdf student reference guides
PDF
The CXO Playbook 2025 – Future-Ready Strategies for C-Suite Leaders Cerebrai...
PDF
III.4.1.2_The_Space_Environment.p pdffdf
PPTX
Fundamentals of safety and accident prevention -final (1).pptx
PPTX
Sustainable Sites - Green Building Construction
PPTX
FINAL REVIEW FOR COPD DIANOSIS FOR PULMONARY DISEASE.pptx
PPTX
CH1 Production IntroductoryConcepts.pptx
PPTX
UNIT 4 Total Quality Management .pptx
PDF
TFEC-4-2020-Design-Guide-for-Timber-Roof-Trusses.pdf
PDF
BIO-INSPIRED HORMONAL MODULATION AND ADAPTIVE ORCHESTRATION IN S-AI-GPT
PDF
PPT on Performance Review to get promotions
PPT
Mechanical Engineering MATERIALS Selection
PDF
Enhancing Cyber Defense Against Zero-Day Attacks using Ensemble Neural Networks
PDF
BMEC211 - INTRODUCTION TO MECHATRONICS-1.pdf
PDF
Human-AI Collaboration: Balancing Agentic AI and Autonomy in Hybrid Systems
PDF
Evaluating the Democratization of the Turkish Armed Forces from a Normative P...
PPTX
Construction Project Organization Group 2.pptx
PPTX
MET 305 2019 SCHEME MODULE 2 COMPLETE.pptx
PDF
Well-logging-methods_new................
Infosys Presentation by1.Riyan Bagwan 2.Samadhan Naiknavare 3.Gaurav Shinde 4...
737-MAX_SRG.pdf student reference guides
The CXO Playbook 2025 – Future-Ready Strategies for C-Suite Leaders Cerebrai...
III.4.1.2_The_Space_Environment.p pdffdf
Fundamentals of safety and accident prevention -final (1).pptx
Sustainable Sites - Green Building Construction
FINAL REVIEW FOR COPD DIANOSIS FOR PULMONARY DISEASE.pptx
CH1 Production IntroductoryConcepts.pptx
UNIT 4 Total Quality Management .pptx
TFEC-4-2020-Design-Guide-for-Timber-Roof-Trusses.pdf
BIO-INSPIRED HORMONAL MODULATION AND ADAPTIVE ORCHESTRATION IN S-AI-GPT
PPT on Performance Review to get promotions
Mechanical Engineering MATERIALS Selection
Enhancing Cyber Defense Against Zero-Day Attacks using Ensemble Neural Networks
BMEC211 - INTRODUCTION TO MECHATRONICS-1.pdf
Human-AI Collaboration: Balancing Agentic AI and Autonomy in Hybrid Systems
Evaluating the Democratization of the Turkish Armed Forces from a Normative P...
Construction Project Organization Group 2.pptx
MET 305 2019 SCHEME MODULE 2 COMPLETE.pptx
Well-logging-methods_new................

1587415189PTE_POWERPOINT_1.ppt lecture slides

  • 1. PTE 316 Piping Design Design Procedure: The problem of design procedure is to find a pipeline configuration and size within the constraints which is safe and economical. The steps in pipeline design are as follows: The determination of the problem , which includes the characteristics of the fluid to be carried, including the flow rates and the allowable head loss The location of the pipes, its source and destination, and terrain over which it will pass The design code to be followed and the material to be used. The determination of a preliminary pipe route, the line length and static head difference Pipe diameter based on allowable head loss Structural analysis such as wall thickness and stress analysis The stress analysis is performed in pipe configuration until compliance with the code is achieved.
  • 2. Pipe types and applications • Seamless pipes (SMLs): These pipes are extruded and have no longitudinal seam. There is no weld and it’s the strongest of the three types • Electric resistance welded pipe (ERW): These pipes are manufactured from plates, where the seam weld is done by electric resistance welding. The welding efficiency is 0.8 • Submerged arc welded pipe (SAW): These pipes are manufactured from plates, normally rolled and steam welded together. The welding has a joint efficiency of 0.95.
  • 3. Piping design equations. • Assuming steady state flow, there are a number of equations which are based upon the general energy equation, that can be employed to design the piping systems. Although piping systems and pipeline design can get complex, the majority of the design problems encountered by the engineers can be solved by the standard flow equations. Typical example is the Bernoulli equation.
  • 4. What is Bernoulli's principle? • Bernoulli's principle is a seemingly counterintuitive statement about how the speed of a fluid relates to the pressure of the fluid. Many people feel like Bernoulli's principle shouldn't be correct, but this might be due to a misunderstanding about what Bernoulli's principle actually says. Bernoulli's principle states the following, • Bernoulli's principle: Within a horizontal flow of fluid, points of higher fluid speed will have less pressure than points of slower fluid speed.
  • 5. How can you derive Bernoulli's principle? • Incompressible fluids have to speed up when they reach a narrow constricted section in order to maintain a constant volume flow rate. This is why a narrow nozzle on a hose causes water to speed up. But something might be bothering you about this phenomenon. If the water is speeding up at a constriction, it's also gaining kinetic energy • The only way to give something kinetic energy is to do work on it. This is expressed by the work energy principle.
  • 6. Bernoulli equation Conti… Wexternal = Δk = mvf 2 - mvi 2 So if a portion of fluid is speeding up, something external to that portion of fluid must be doing work on it. What force is causing work to be done on the fluid? Well, in most real world systems there are lots of dissipative forces that could be doing negative work, but we're going to assume for the sake of simplicity that these viscous forces are negligible and we have a nice continuous and perfectly laminar (streamline) flow.
  • 7. • Laminar (streamline) flow means that the fluid flows in parallel layers without crossing paths. In laminar streamline flow there is no swirling or vortices in the fluid. • Consider the diagram below which shows water flowing along streamlines from left to right. As the outlined volume of water enters the constricted region it speeds up. The force from pressure P_1P1​ P, start subscript, 1, end subscript on the left side of the shaded water pushes to the right and does positive work since it pushes in the same direction as the motion of the shaded fluid. The force from pressure P_2P2​ P, start subscript, 2, end subscript on the right side of the shaded fluid pushes to the left and does negative work since it pushes in the opposite direction as the motion of the shaded fluid.
  • 9. We know that the water must speed up (due to the continuity equation) and therefore have a net positive amount of work done on it. So the work done by the force from pressure on the left side must be larger than the amount of negative work done by the force from pressure on the right side. This means that the pressure on the wider/slower side P1 has to be larger than the pressure on the narrow/faster side P2. This inverse relationship between the pressure and speed at a point in a fluid is called Bernoulli's principle. Bernoulli's principle: At points along a horizontal streamline, higher pressure regions have lower fluid speed and lower pressure regions have higher fluid speed.
  • 10. • The idea that regions where the fluid is moving fast will have lower pressure can seem strange. Surely, a fast moving fluid that strikes you must apply more pressure to your body than a slow moving fluid, right? Yes, that is right. But we're talking about two different pressures now. The pressure that Bernoulli's principle is referring to is the internal fluid pressure that would be exerted in all directions during the flow, including on the sides of the pipe. This is different from the pressure a fluid will exert on you if you get in the way of it and stop its motion.
  • 11. • Note that Bernoulli's principle does not say that a fast moving fluid can't have significantly high pressures. It just says that the pressure in a slower region of that same flowing system must have even larger pressure than the faster moving region. What is Bernoulli's equation? • Bernoulli's equation is essentially a more general and mathematical form of Bernoulli's principle that also takes into account changes in gravitational potential energy. let's take a look at Bernoulli's equation and get a feel for what it says and how one would go about using it.
  • 12. • Bernoulli's equation relates the pressure, speed, and height of any two points (1 and 2) in a steady streamline flowing fluid of density ρ. Bernoulli's equation is usually written as follows, P1 + 1/2℮v + ℮gh1 = P2 + 1/2℮v + ℮gh2 The variables P1. v1, h1 refer to the pressure, speed, and height of the fluid at point 1, whereas the variables P2. V2, h2 refer to the pressure, speed, and height of the fluid at point 2 as seen in the diagram below. The diagram below shows one particular choice of two points (1 and 2) in the fluid, but Bernoulli's equation will hold for any two points in the fluid.
  • 14. Derivation of Bernoulli's equation To conti….