Introduction
The Pipeline Toolbox is home to many tools and calculators. The PLTB User’s Guide presents information, guidelines, and procedures for use during design and operations tasks for field or office applications.
Pipeline Hydraulic Fundamentals
For Fluids flowing in a pipeline between two points (A and B), the energy balance is subject to the following equation known as Bernoulli’s equation 2: Z_A+\frac{P_A}{\gamma}+\frac{V_A^2}{2g}+H_p=Z_B+\frac{P_B}{\gamma}+\frac{V_B^2}{2g}+H_f
Z_A+\frac{P_A}{\gamma}+\frac{V_A^2}{2g}+H_p=Z_B+\frac{P_B}{\gamma}+\frac{V_B^2}{2g}+H_f
Where:
𝑍𝐴 = Elevation at point A
𝑍𝐵 = Elevation at point B
𝑃𝐴 = Pressure at point A
𝑃𝐵 = Pressure at point B
𝑉𝐴 = Velocity at point A
𝑉𝐵 = Velocity at point B
𝑔 = gravity constant
𝛾 = gravity times the density of the fluid
𝐻𝑝 = the equivalent head added to the fluid by a compressor at point A
𝐻𝑓 = the total frictional pressure loss between points A and B
According to the results of an in-depth analysis, the industrial equations can produce large amounts of error when compared to a process simulator analysis with the same pipe specifications and conditions. The following table shows the results of the equation study:
Table 1: Conventional Hydraulic Equation Analysis
Equation Name | Range of Error |
---|---|
Panhandle | 3.5-10% |
Colebrook | 2.4-10% |
Modified-Colebrook | 1.0-8.8% |
AGA | 0.2-15% |
Weymouth | 39-59% |
IGT | 7.6-17% |
Spitzglass | 88-147% |
Mueller | 13-20% |
The error produced by these equations is due to the assumptions used to derive the equation from the General Flow Equation. Also, extremely large amounts of error occurred when the equations were applied outside their intended pipeline environment. This error could directly affect theoretical optimal pipeline diameter and cause it to be significantly different from the actual optimal pipe diameter.
We will discuss each of these equations, their limitations, and their applicability.
Erosional and Sonic Velocity has been added to the following Modules and Calculations.
- Panhandle A
- Panhandle B
- Weymouth
- AGA Turbulent Flow
- Colebrook-White
- FM-Fundamental Equation
- IGT Distribution Equation
Erosional Velocity
Pipe erosion begins when velocity exceeds the value of C/SQRT(ρ) in ft/s, where ρ = gas density (in lb./ft3) and C = empirical constant (in lb./s/ft2) (starting erosional velocity). We used C=100 as API RP 14E (1984). However, this value can be changed based on the internal conditions of the pipeline. The following equation is used for the calculation.
Inputs
- C – Factor (dimensionless)
- Compressibility Factor (dimensionless)
- Gas Gravity (dimensionless)
- Operating Pressure (psig)
- Operating Temperature (deg F)
- PLTB
u_{max}=100\sqrt{ \frac{ZRT}{29GP}}
u_{max}=100\sqrt{ \frac{ZRT}{29GP}}
Erosional Velocity is in ft/sec
Sonic Velocity
The maximum possible velocity of compressible fluid gas/liquids in pipe is called sonic velocity.
Inputs
- K = Cp/Cv – the ratio of specific heats at constant pressure to constant volume (fluid directive)
- G=32.2 ft/sec
- R=1544/mol. Wt.
- T = Absolute temperature in deg R
K = A + B(P) – C(T)1/2 – D(API)2 + F(T) (API)
Sonic Velocity is in ft/sec
Module/Application
Gas Correlations
- Panhandle A
- Uses an empirical efficiency factor of 0.92 for partially turbulent flow conditions. It is suitable for Reynolds numbers from 5 x 106 to 11 x 106. Smaller diameter lines such as 12″ and below, the efficiency factors need to be reduced.
- Panhandle B
- Weymouth
- A.G.A. Fully Turbulent Flow
- Colebrook – White
- FM – Fundamental Equation
- IGT Distribution Equation
- Mueller – High Pressure
- Mueller – Low Pressure
- Pittsburgh
- Spitzglass
References
- McAllister, E. W., “Pipeline Rules of Thumb” Gulf Professional Publishing, Seventh Edition
- Menon, Shahi E., “Gas Pipeline Hydraulics”, Systek Technologies, Inc.
- Carroll, Landon and Hudkins, Weston R., “Advanced Pipeline Design”
- American Gas Association (AGA), “Reference: Eq-17-18, Section 17, GPSA”, Engineering Data Book, Eleventh Edition
FAQ
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Purging is a process of removing gas from the pipeline. Controlled purging of gases from pipelines by direct displacement with other gases that have been safely practiced for many years with the recognition that some flammable mixture is present. Purging of gases from pipelines by direct displacement with another gas also has been similarly practiced. It works both ways; however, there will always be an atmosphere of type of a mixture. This is due to the densities of the gases. Check Out
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Pipe erosion begins when velocity exceeds the value of C/SQRT(ρ) in ft/s, where ρ = gas density (in lb./ft3) and C = empirical constant (in lb./s/ft2) (starting erosional velocity). We used C=100 as API RP 14E (1984). However, this value can be changed based on the internal conditions of the pipeline. Check Out
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The maximum possible velocity of a compressible fluid in a pipe is called sonic velocity. Oilfield liquids are semi-compressible, due to dissolved gases. Check Out