Author: David Hairston

  • Onshore Natural Gas Pipeline Transportation Alternatives: Capital Cost Comparisons

    In recent TOTMs (January through April, August, and September 2012 and again in January 2013), we discussed several aspects of the physical behavior and transportation of carbon dioxide (CO2) and natural gas in the dense phase. We illustrated how thermophysical properties change in the dense phase and their impacts on pressure drop calculations. The pressure drop calculation utilizing the liquid phase and vapor phase equations was compared.

    In the August 2012  (TOTM), we studied transportation of rich natural gas in the dense phase region and compared the results with the case of transporting the same gas using a two phase (gas-liquid) option. Our study highlighted the pros and cons of dense phase transportation.

    In September 2012 (TOTM), we analyzed pipeline transportation of a lean natural gas at a wide range of operating pressures from the relatively low pressure typical in many gas transmission pipelines to much higher pressures well into the dense phase region.

    In January 2013 (TOTM), we estimated capital costs (CAPEX) as a tool to compare then selected the operating conditions and associated facilities for a long distance – high volume flow gas transmission pipeline.

    In this month’s Tip of the Month (TOTM), we will revisit the January 2013 (TOTM) and continue to explore alternatives specifically for onshore natural gas transportation in pipelines. This month’s focus is also on the estimation of capital costs as a tool to compare then select the operating pressures and associated facilities for a long distance, high volume flow gas transmission pipeline.

     

    Case Study:

     We will continue to use a similar case study basis as used in the September 2012 TOTM. The gas composition and conditions are presented in Table 1. For simplicity, the calculations and subsequent discussion will be done on the dry basis. The feed gas dew point was reduced to -40 ˚C (-40 ˚F) by passing it through a mechanical refrigeration dew point control plant. The resulting composition and conditions of the lean gas are also presented in Table 1. The lean gas has a Gross Heating Value of 40.33 MJ/Sm3 (1082 BTU/scf). The pipeline parameters are:

    • Length is 1609 km (1000 miles) long
    • Pipeline outside diameter is 1067 mm (42 inches) for cases A through C. Case D outside diameter is: 914 mm (36 in)
    • Steady state conditions are assumed.
    • Pressure at delivery point and suction at each compressor station is 7 MPa  (1015 Psia)
    • This is a horizontal pipeline with no elevation change.
    • Overall Heat Transfer Coefficient: 1.42 W/m2-˚C  (0.25 Btu/hr-ft2-˚F).
    • Ambient temperature is 18.3˚C (65˚F).
    • Compressor polytropic efficiency is 75%.
    • Pressure drop in coolers 35 kPa (5 Psia)
    • Simulation software: ProMax and using Equation of State from Soave-Redlich-Kwong (SRK).

    Table 1

     Four cases of onshore transportation of this natural gas are considered and each is explained briefly below. The number of pipeline segments, segment length, and inlet pressure of each segment for the four cases are presented in Table 2 in the SI (System International) and field (FPS, foot, pound and second) sets of units.

    Hydraulics Simulation Results and Discussions:

    The four cases are simulated using ProMax [3] to determine the pressure and temperature profiles, the compression horsepower,  and the after cooler duties. Table 3 presents a summary of simulation results for the three cases in FPS and SI systems of units.

     

    Case A: High Pressure (Dense Phase)

    This pipeline is a single compressor station configuration. The pipeline inlet pressure is in the dense phase zone. After processing and passing through the first stage scrubber, the lean gas  pressure is raised from 4.24 to 9.363 MPa (615 to 1358 Psia), then cooled to 37.8 ˚C (100 ˚F). The gas is compressed further in the second stage to 20.684 MPa (3000 Psia). The high pressure compressed gas is cooled back to 37.8 ˚C (100 ˚F) and then passed through a separator before entering the long pipeline.

     

    Case B: Intermediate Pressure

    This pipeline has three compressor stations each equally spaced at 536 km (333 miles). The pipeline inlet pressure is near the dense phase zone.  In the first station, the pressure is raised from 4.24 to 12.8 MPa (615 to 1858 Psia) and in the subsequent two stations, the pressure is raised from 7 to 12.8 MPa (1015 to 1858 Psia) in one stage, then cooled to 37.8 ˚C (100 ˚F), and finally passed through a separator before entering each pipeline segment.

     

    Case C: Low Pressure

    This pipeline has five compressor stations equally spaced in 322 km (200-mile)  segments. In the first station, the pressure is raised from 4.24 to 10.9 MPa (615 to 1577 Psia) and in the subsequent four stations, the pressure is raised from 7 to 10.9 MPa (1015 to 1577 Psia) in one stage, then cooled to 37.8 ˚C (100 ˚F), and finally passed through a separator before entering each pipeline segment. The pipeline inlet pressure is well below that for dense phase.

    Table 2

    Case D: High Pressure

    This case is similar to case B except it operates in the dense phase and the outside diameter is 914 mm (36 inches). This pipeline has three compressor stations each equally spaced at 536 km (333 miles). The pipeline inlet pressure is in the dense phase zone.  After processing and passing through the first stage scrubber, the lean gas  pressure is raised from 4.24 to 8.67 MPa (615 to 1257 Psia), then cooled to 37.8 ˚C (100 ˚F). The gas is compressed further in the second stage to 17.72 MPa (2570 Psia). The high pressure compressed gas is cooled back to 37.8 ˚C (100 ˚F) and then passed through a separator before entering the long pipeline. In each subsequent station, the pressure is raised from 7 to 17.7 MPa (1015 to 2565 Psia) in one stage, then cooled to 37.8 ˚C (100 ˚F), and finally passed through a separator before entering each pipeline segment.

    As can be seen in Table 3, Case A with a single compressor station requires the least total compression power and lowest heat duty requirements. The power increase for Case B (with three compressor stations) is about 38%  compared to Case A and 54% and 89% for Cases C (with 5 compressor stations)  and D (with 3 compressor stations), respectively. These increases in power and heat duty requirements are significant.  Similarly, the heat duty increases are about 6, -1, and 59% for case B through D compared to case A, respectively.

     Table 3

     

    Variation of gas  pressures is shown on Figure 1 for Cases A and B. As discussed in the previous TOTM, when the phase diagram and the pressure profiles are cross plotted using the pressure and temperature profiles the pipeline outlet condition remains  to the right of the dew point curve with the gas remaining as single phase.

     

    Mechanical Design (Wall Thickness and Grade)  

    Pipeline wall thickness is an important economic factor. Pipeline materials have historically represented approximately 40% of the Capital Expense (CAPEX) of a pipeline. Construction has historically  accounted for approximately 40% of the CAPEX as well. The estimation of the CAPEX is developed later in this TOTM. Once the wall thickness is determined, then the total weight (tonnage) of the pipeline can be calculated as well as costs for the pipeline steel.

     

    The wall thickness, t, for the three cases is calculated from a variation of the Barlow Equation found in the ASME B31.8 Standard for Gas Transmission Pipelines:

    Formula 1

     

     

    Where,

    • P is maximum allowable operating  pressure, here set to 1.1 times the inlet pressure,
    • OD is outside diameter,
    • E is joint efficiency (assumed to be 1) since the pipeline will be joined with through thickness butt welds and 100% inspected,
    • F is design factor,(ranges from 0.4 to 0.72) and here set  to be 0.72 (for remote area),
    • T is the temperature derating factor and is also 1.0 with the inlet temperatures no more than 37.8 ˚C (100 ˚F).
    • σ is the pipe material yield stress (Grade X70 = 70,000 psi or 448.2 MPa), and
    • CA is the corrosion allowance (assumed to be 0 in or 0 mm, for this dry gas).

    After calculating the wall thickness, the diameter to wall thickness ratio (D/t) is checked against these rules of thumb:

    • Onshore pipelines will have a maximum D/t of 72.

    If the D/t calculated is too high, the wall thickness will be increased to yield the maximum allowed D/t.

    Figure 1

     Using the calculated pipeline inlet pressures from the hydraulics as the starting point, the MAOP, and then the wall thickness can be calculated. The calculated wall thickness is then checked against the maximum D/t criteria. Table 4 summarizes these calculations for the four cases of onshore locations.

    Knowing the wall thickness and diameter allows the weight per lineal length (foot or meter) to be calculated. The total weight of the steel for the 1609 km (1000 mile) long can then be calculated as well. The unit weight is given in kg/m (lbm/ft) and the total weight in metric tonnes (1000 kg) and short tons (2000 pounds). The results of these weight calculations are in Table 5.

     Table 4&5

    Some observations from these calculations are:

    • Decreasing the pipeline diameter from 42 inch to 36 inch does NOT dramatically reduce the total steel tonnage. This is due to the increased pressures needed to flow the same volume of gas in the smaller diameter, hence increasing the wall thickness.
    • Increasing the steel grade (SMYS – Specified Minimum Yield Stress) from X-70 to X-80 would decrease the steel tonnage approximately 14%. As the cost calculations will show, this reduction would lower the cost significantly.
    • The volume of steel combined with the diameter and wall thicknesses will require a major portion of pipe manufacturing capacity. If this were a sanctioned project, pipe steel procurement would need to bid well in advance of the planned construction.
    • Wall thicknesses are NOT raised to next standard API thicknesses. The large quantity of steel needed allows the buyer to dictate a non-standard thickness. The pipe mills will be glad to accommodate such a requirement.

     

    Estimated Capital Costs

     The capital costs (CAPEX) for these estimates are based on two key variables: pipeline wall thickness and the compression power required. Both are dependent of the pipeline pressure profile which is dictated by the number of compressor stations. The estimated cost will be calculated from the following assumptions:

    • Line pipe is priced at US$ 1200 per short ton with a 15% adder for coatings.
    • Pipeline total installed cost is 2.5 times the pipe steel plus coatings cost. This factor  has been surprisingly consistent historically for both onshore and offshore long distance and larger diameter pipelines. Project specific factors such as mountainous terrain for onshore pipelines  can impact this cost multiplier.
    • No additional cost difference is taken into account for this estimate many of the real conditions that are dealt with for the  onshore design  construction. In reality there is a difference that can be significant. These differences are largely dependent on the project location with factors that could include weather and seasonal challenges, terrain for onshore projects, available infrastructure and its impact on logistics, and availability of construction equipment and labor.
    • Compressors and associated equipment (drivers, coolers, and ancillaries) are priced at US$ 1500 per demand horsepower.
    • Onshore compressor stations are priced at US$ 25 million each for site works, buildings and equipment not directly related to gas compression.

     

    With these cost assumptions, an order of magnitude estimate (OME) for the total installed cost (TIC) is developed for the pipeline, then the compressor stations, and finally combined for the total ONSHORE pipeline system in Table 6 – Pipeline Estimate, Table 7 – Compressor Station Estimate, and Table 8 – Total System OME.

     

     Table 6

     

    Table 7&8

    The results are indicative of finding a set of operating pressures, pipe diameter and number of compressor stations that show relatively little change with different combinations of the key parameters (Cases B, C and D). The selection of the “optimum” system configuration will involve more engineering definition, consideration of construction challenges, and evaluation of other parameters such as the operating costs (OPEX), environmental and permitting challenges, and more depth in evaluating the construction plan and costs.

    The total installed costs for this  ONSHORE system declines with decreasing operating pressure (MAOP), although the rate of decline is also decreasing, as more compressor stations are needed. For the onshore systems, the operating cost, particularly fuel costs, may be one of the key deciding parameters for the operating pressure / number of compressor stations decision. It is common for total life cycle costs (OPEX plus CAPEX) to begin rising at some point as the number of compressor stations and total horsepower increases with decreasing operating pressure.

     

    Often, with the operating costs included the “optimum” configuration favors higher operating pressures and fewer compressor stations. The cost adjustments for project location on both CAPEX and OPEX can move to “optimum” configuration either way.

     

     Final Comments:

     We have studied transportation of natural gas in the dense phase region (high pressure) and compared the results with the cases of transporting the same gas using intermediate and low pressures. Our study highlights the following features:

    1. There may be several system configurations (pipe diameter, operating pressures, and number of compressor stations) that show relatively small variation.
    2. As the MAOP increases, the required power and associated cooling duty can significantly decrease.
    3. The decreased costs for compression are offset by increasing pipeline costs. The key is by how much.
    4. Project location can have significant impact on the costs, hence the key decisions are on operating pressures, and the number and power levels at the compressor stations.
    5. With the high power demands of large diameter – high capacity pipelines, the operating costs for fuel can be a key factor in the configuration selection. If the gas at the source is not at high enough pressure, considerable compression power and cooling duty may be required if the decision is to use the dense phase.

     

    In future Tips of the Month, we will consider offshore transportation of natural gas as well as the effect of project location and operating costs on the life cycle costs and the configuration selection.

     

    To learn more, we suggest attending our G40 (Process/Facility Fundamentals), G4 (Gas Conditioning and Processing), G5 (Gas Conditioning and Processing-Special), PF81 (CO2 Surface Facilities), PF4 (Oil Production and Processing Facilities), and PL4 (Fundamentals of Onshore and Offshore Pipeline Systems) courses.

     

    John M. Campbell Consulting (JMCC) offers consulting expertise on this subject and many others. For more information about the services JMCC provides, visit our website at www.jmcampbellconsulting.com, or email us at consulting@jmcampbell.com.

    By: Mahmood Moshfeghian and David Hairston

    References:

    1. Beaubouef, B., “Nord stream completes the world’s longest subsea pipeline,” Offshore, P30, December 2011.
    2. http://www.jmcampbell.com/tip-of-the-month/
    3. ProMax 3.2, Bryan Research and Engineering, Inc., Bryan, Texas, 2012.
  • Low Pressure Vs High Pressure Dense Phase Natural Gas Pipeline Transportation

    Capital Cost (CAPEX) Comparisons

    High pressure (or dense phase) is increasingly used for transporting large volumes of carbon dioxide (CO2) and natural gas over long distances. In this month’s – Tip of the Month (TOTM), we continue to explore key aspects of dense phase transportation in pipelines. This month’s focus is on the estimation of capital costs as a tool to compare then select the operating pressures and associated facilities for a long distance – high volume flow gas transmission pipeline.

    In recent TOTMs (January through April 2012 and again in August and September 2012), we discussed several aspects of the physical behavior and transportation of carbon dioxide (CO2) and natural gas in the dense phase. We illustrated how thermophysical properties change in the dense phase and their impacts on pressure drop calculations. The pressure drop calculation utilizing the liquid phase and vapor phase equations were compared.

    In the August 2012  (TOTM), we studied transportation of rich natural gas in the dense phase region and compared the results with the case of transporting the same gas using a two phase (gas-liquid) option. Our study highlighted the pros and cons of dense phase transportation.

    In September 2012 (TOTM), we analyzed pipeline transportation of a lean natural gas at a wide range of operating pressures from the relatively low pressure typical in many gas transmission pipelines to much higher pressures well into the dense phase region.

    Case Study:

    We will continue to use the same case study basis as used in the September 2012 TOTM. The gas composition and conditions are presented in Table 1. For simplicity, the calculations and subsequent discussion will be done on the dry basis. The feed gas dew point was reduced to -40 ˚F (-40 ˚C) by passing it through a mechanical refrigeration dew point control plant. The resulting composition and conditions of the lean gas are also presented in Table 1. The lean gas has a Gross Heating Value of 1082 BTU/scf (40.33 MJ/Sm3), which is in the range typically seen for contract quality natural gas in North America. The pipeline parameters are:

    • Length is 1000 miles (1609 km) long
    • Pipeline outside diameter is 42 inches (1067 mm). Initial inside diameters for the hydraulics analyses are: Case A = 39.0 (991 mm) inches, Case B = 40.0 inches (1016 mm), and Case C = 40.5 inches (1029 mm)
    • Steady state conditions are assumed.
    • Pressure at delivery point and suction at each compressor station is 615 Psia (4.24 MPa)
    • This is a horizontal pipeline with no elevation change.
    • Overall Heat Transfer Coefficient: 0.25 Btu/hr-ft2-˚F (1.42 W/m2-˚C).
    • Simulation software: ProMax and using Equation of State from Soave-Redlich-Kwong (SRK).

    Table 1. Composition and conditions of the feed gas and lean gas

    Table 2. Pipeline specifications for the three casesThree cases for transportation of this natural gas are considered and each is explained briefly below.  The number of pipeline segments, segment length, and inlet pressure of each segment for the three cases are presented in Table 2 in the field (FPS, foot, pound and second) and SI (System International) sets of units.

    Table 2. Pipeline specifications for the three cases


    Hydraulics Simulation Results and Discussions:

    The three cases are simulated using ProMax [3] to determine the pressure and temperature profiles, the compression horsepower, and the after cooler duties. Table 3 presents a summary of simulation results for the three cases in FPS and SI systems of units.

    Case A: High Pressure (Dense Phase)

    This pipeline is a single compressor station configuration. The pipeline inlet pressure is in the dense phase zone. After processing and passing through the first stage scrubber, the lean gas  pressure is raised to 1496 psia (10.32 MPa), then cooled to 100 ˚F (37.8 ˚C). The gas is compressed further in the second stage to 3659 Psia (25.22 MPa). The high pressure compressed gas is cooled back to 100 ˚F (37.8 ˚C) and then passed through a separator before entering the long pipeline.

    Case B: Intermediate Pressure

    This pipeline has three compressor stations each equally spaced at 333 miles. The pipeline inlet pressure is near the dense phase zone.  In each station, the pressure is raised from 615 Psia to 2071 Psia (4.24 to 14.28 MPa) in one stage, then cooled to 100 ˚F (37.8 ˚C), and finally passed through a separator before entering each pipeline segment.

    Case C: Low Pressure

    This pipeline has five compressor stations equally spaced in 200-mile (322 km)  segments. The pipeline inlet pressure is well below that for dense phase. In each station, the pressure is raised from 615 Psia to 1637 Psia (4.24 to 11.28 MPa) in one stage, then cooled to 100 ˚F (37.8 ˚C), and finally passed through a separator before entering each pipeline segment.

    Table 3. Summary of computer simulation results for the three cases.

    As can be seen in this table, Case A with a single compressor station requires the least total compression power and lowest heat duty requirements. The power reduction for Case A is about 51%  compared to Case B (with three compressor stations) and 63% compared to Case C (with 5 compressor stations). These reductions in power and heat duty requirements are significant.  Similarly, the heat duty reduction for Case A is about 39% compared to Case B and 50 % compare to Case C, respectively.

    Variation of gas velocity, pressures, and temperature are shown on Figures 1 through 3 for Cases A and B. As discussed in the previous TOTM, when the phase diagram and the pressure profiles are cross plotted using the pressure and temperature profiles the pipeline outlet condition remains  to the right of the dew point curve with the gas remaining as single phase.

    Figure 1. Variation of gas velocity in the pipeline (Cases A and B)

    Mechanical Design (Wall Thickness and Grade)

    Pipeline wall thickness is an important economic factor. Pipeline materials typically represent approximately 40% of the Capital Expense (CAPEX) of a pipeline. Construction will account for approximately 40% of the CAPEX as well. The estimation of the CAPEX is developed later in this TOTM. Once the wall thickness is determined, then the total weight (tonnage) of the pipeline can be calculated as well as costs for the pipeline steel.

    The wall thickness, t, for the three cases is calculated from a variation of the Barlow Equation found in the ASME B31.8 Standard for Gas Transmission Pipelines:

                                                                                                                         (1)

    Where,

    • P is maximum allowable operating  pressure, here set to 1.05 times the inlet pressure,
    • OD is outside diameter,
    • E is joint efficiency (assumed to be 1) since the pipeline will be joined with through thickness butt welds and 100% inspected,
    • F is design factor,(ranges from 0.4 to 0.72) and here set  to be 0.72 (for remote area),
    • T is the temperature derating factor and is also 1.0 with the inlet temperatures no more than 100 ˚F (37.8 ˚C).
    • σ is the pipe material yield stress (Grade X70 = 70,000 psi or 448.2 MPa), and
    • CA is the corrosion allowance (assumed to be 0 in or 0 mm, for this dry gas).

    After calculating the wall thickness, the diameter to wall thickness ratio (D/t) is checked against these rules of thumb:

    • Onshore pipelines will have a maximum D/t of 72.
    • Offshore pipelines will have a maximum D/t of 42.

    If the D/t calculated is too high, the wall thickness will be increased to yield the maximum allowed D/t.

    Figure 2. Variation of pressure in the pipeline (Cases A and B)

       

    Figure 3. Variation of temperature in the pipeline (Cases A and B)

    Using the calculated pipeline inlet pressures from the hydraulics as the starting point, the MAOP then the wall thickness can be calculated. The calculated wall thickness is then checked against the maximum D/t criteria. Table 4 summarizes these calculations for the three cases for both onshore and offshore locations.

    Knowing the wall thickness and diameter allows the weight per lineal length (foot or meter) to be calculated. The total weight of the steel for the 1000 mile (1609 km) long can then be calculated as well. The unit weight is given in lbm/ft (kg/m) and the total weight in short tons (2000 pounds) and metric tonnes (1000 kg). The results of these weight calculations are in Table 5.

    Some observations from these calculations that can be made are:

    • Increasing the steel grade (SMYS – Specified Minimum Yield Stress) from X-70 to X-80 would decrease the steel tonnage approximately 14%. As the cost calculations will show, this reduction would lower the cost significantly. However, the use of X-80 steels is still not widely accepted in the pipeline industry.
    • The volume of steel combined with the diameter and wall thicknesses will require a major portion of pipe manufacturing capacity. If this were a sanctioned project, pipe steel procurement would need to bid well in advance of the planned construction.
    • Wall thicknesses are NOT raised to next standard API thicknesses. The large quantity of steel needed allows the buyer to dictate a non-standard thickness. The pipe mills will be glad to accommodate such a requirement.

    Table 4: Pressures and Wall Thickness Selections

    Table 5: Pipeline Wall Thickness Selections and Total Steel Weight

    Estimated Capital Costs

    The capital costs (CAPEX) for these estimates are based on two key variables: pipeline wall thickness and the compression power required. Both are dependent of the pipeline pressure profile which is dictated by the number of compressor stations. The estimated cost will be calculated from the following assumptions:

    • Line pipe is priced at US$ 1200 per short ton with a 15% adder for coatings.
    • Pipeline total installed cost is 2.5 times the pipe steel plus coatings cost. This factor is surprising consistent for both onshore and offshore long distance and larger diameter pipelines. Project specific factors such as mountainous terrain for an onshore pipelines, or the requirement to trench an offshore pipeline can impact this cost multiplier.
    • No additional cost difference is taken into account for this estimate between onshore and offshore construction. In reality there is a difference that can be significant. These differences are largely dependent on the project location with factors that could include weather and seasonal challenges, water depth for offshore projects, terrain for onshore projects, available infrastructure and its impact on logistics, and availability of construction equipment and labor.
    • Compressors and associated equipment (drivers, coolers, and ancillaries) are priced at US$ 1500 per demand horsepower.
    • Onshore compressor stations are priced at US$ 25 million each for site works, buildings and equipment not directly related to gas compression.
    • Offshore compressor stations are priced at US$250 million each for the fixed structure, topsides not directly related to gas compression, and a quarters complex. This assumption is sensitive to project location, whether the structure is stand-alone or in a group of structures, water depth, and met-ocean conditions.
    • The offshore pipeline cases originate ONSHORE with the lead compressor station.

    With these cost assumptions, an order of magnitude estimate (OME) for the total installed cost (TIC) is developed for the pipeline, then the compressor stations, and finally combined for the total pipeline system in Table 6 – Pipeline Estimate, Table 7 – Compressor Station Estimate, and Table 8 – Total System OME.

    Table 6: Pipeline Total Installed Cost

    Our estimating assumptions can lead to costs that are the same whether for onshore or offshore pipelines. This is where knowledge of the project becomes vital in adjusting the estimate to account for conditions that can affect the assumptions.

    Table 7: Compressor Stations Total Installed Cost

    The most sensitive variable for the compressor stations calculations is the location of any offshore facilities. Location, water depth and met-ocean conditions can and will impact the estimated cost significantly.

    Table 8: Total System OME

    The total installed costs for an ONSHORE system decline with decreasing operating pressure (MAOP), although the rate of decline is also decreasing as more compressor stations are needed. For the onshore systems, the operating cost, particularly fuel costs, can impact the operating pressure / number of compressor stations decision. It is common for total life cycle costs (OPEX plus CAPEX) to begin rising at some point as the number of compressor stations and total horsepower increases with decreasing operating pressure.

    For an OFFSHORE system, show the lowest total installed cost is with a three compressor station configuration. This “optimum” CAPEX solution will be sensitive to project location as discussed above as well as operating costs. Often, with the operating costs included the “optimum” configuration favors higher operating pressures and fewer compressor stations. The cost adjustments for project location on both CAPEX and OPEX can move to “optimum” configuration either way.

    Final Comments:

    We have studied transportation of natural gas in the dense phase region (high pressure) and compared the results with the cases of transporting the same gas using intermediate and low pressures. Our study highlights the following features:

    1. As the MAOP increases, the required power and associated cooling duty can significantly increase.
    2. The decreased costs for compression are offset by increasing pipeline costs. The key is by how much.
    3. Project location can have significant impact on the costs, hence the key decisions are on operating pressures, onshore versus offshore routing (where possible), and the number and power levels at the compressor stations.
    4. With the high power demands of large diameter – high capacity pipelines, the operating costs for fuel can be a key factor in the configuration selection. If the gas at the source is not at high enough pressure, considerable compression power and cooling duty may be required if the decision is to use the dense phase.

    In future Tip of the Months, we will consider the effect of project location and operating costs on the life cycle costs and the configuration selection.

    To learn more, we suggest attending our G40 (Process/Facility Fundamentals), G4 (Gas Conditioning and Processing), G5 (Gas Conditioning and Processing-Special), PF81 (CO2 Surface Facilities), PF4 (Oil Production and Processing Facilities), and PL 4 (Fundamentals of Onshore and Offshore Pipeline Systems) courses. 

    John M. Campbell Consulting (JMCC) offers consulting expertise on this subject and many others. For more information about the services JMCC provides, visit our website at www.jmcampbellconsulting.com, or email us at consulting@jmcampbell.com. 

    By: David Hairston and Mahmood Moshfeghian

    References:

    1. Beaubouef, B., “Nord stream completes the world’s longest subsea pipeline,” Offshore, P30, December 2011.
    2. http://www.jmcampbell.com/tip-of-the-month/
    3. ProMax 3.2, Bryan Research and Engineering, Inc., Bryan, Texas, 2012.

     

  • Low Pressure Versus High Pressure Dense Phase Natural Gas Pipeline Transportation

    Dense phase is a favorable condition for transporting carbon dioxide (CO2) and natural gas as well as carbon dioxide injection into crude oil reservoir for enhanced oil recovery. Pipelines have been built to transport CO2 and natural gas [1] in the dense phase region due to its higher density, and this also provides the added benefit of no liquids formation in the pipeline.

    Recently (January through April 2012 TOTMs) we discussed several aspects of transportation of carbon dioxide (CO2) in the dense phase. We illustrated how thermophysical properties change in the dense phase and their impacts on pressure drop calculations. The pressure drop calculation utilizing the liquid phase and vapor phase equations were compared. In the August 2012 Tip of The Month (TOTM) [2], we studied transportation of rich natural gas in the dense phase region and compared the results with the case of transporting the same gas using a two phase (gas-liquid) option. Our study highlighted the pros and cons of dense phase transportation.

    In this TOTM, we will study the low pressure versus high pressure (dense phase) pipeline transportation of a lean natural gas. The application of dense phase in the oil and gas industry will be discussed briefly.

    Case Study:

    For the purpose of illustration, we will consider transporting a natural gas mixture with composition and conditions presented in Table 1. For simplicity, the calculations and subsequent discussion will be done on the dry basis. The feed gas dew point was reduced to -40 ˚F (-40 ˚C) by passing it through a mechanical refrigeration dew point control plant. Figure 1 presents the phase envelopes for the feed and lean (pipeline) gases. The composition and conditions of the lean gas are also presented in Table 1. The 1000 miles (1609 km) long pipeline with a  diameters of 42 inches (1067 mm) has been considered. A simplistic Process Flow Diagram (PFD) is shown in Figure 2. The following assumptions and correlations are/used:

    1. Dry basis, ignoring water.
    2. C7+ considered as nC8.
    3. Steady state
    4. Delivery pressure is 615 Psia (4.24 MPa).
    5. Pressure drop in each heat exchanger is 5 psi (0.035 MPa).
    6. No pressure drop in scrubbers and separators.
    7. Horizontal pipeline, no elevation change.
    8. Inside surface absolute roughness is 0.0018 in (0.046 mm).
    9. Single Phase Friction Factor: Colebrook
    10. For calculation purpose, each line segment was divided into 10 sub segments.
    11. Overall Heat Transfer Coefficient: 0.25 Btu/hr-ft2-˚F (1.42 W/m2-˚C).
    12. Simulation software: ProMax [3]
    13. Equation of State: Soave-Redlich-Kwong (SRK).

    Table 1. Composition and conditions of the feed gas and lean gas


    Figure 1. Phase envelopes for the feed (rich) and pipeline (lean) gas

     

    Three cases for transportation of this natural gas are considered and each is explained briefly in the proceeding section. Figure 2 presents the PFDs for Cases A and B. Case C PFD is similar to Case B with 2 more pipeline segments, compressors and coolers. Figure 3 illustrates the pipeline systems in a block diagram.  The number of pipeline segments, segment length, and inlet pressure of each segment for the three cases are presented in Table 2 in the field (FPS, foot, pound and second) and SI (System International) sets of units.

    Figure 2. Process flow diagrams (PFD) for Cases A and B (Case C is similar to Case B)

     

    Figure 3. Pipeline Block Diagrams for Cases A, B, and C

    Table 2. Pipeline specifications for the three cases


     

    Case A: High Pressure (Dense Phase)

    After passing through the first stage scrubber, the lean gas enters the first stage of compressor where its pressure is raised to 1407 psia (9.703 MPa), then it is cooled to 100 ˚F (37.8 ˚C) and compressed further in the second stage to 3220 Psia (22.2 MPa). The high pressure compressed gas is cooled back to 100 ˚F (37.8 ˚C) and then passed through a separator before entering the long pipeline (See Case A in Figure 2).

     

    Case B: Intermediate Pressure

    The process flow diagram (PFD) for this case is also shown in Figure 2. In this case, the pipeline is divided into three 333.3-mile (536.2 km) pipelines with one lead compressor station and two intermediate compressor stations. In each station, the pressure is raised from 615 Psia to 1966 Psia (4.24 to 13.56 MPa) in one stage and then cooled to 100 ˚F (37.8 ˚C), passed through a separator before entering the downstream pipeline segment.

     

    Case C: Low Pressure

    This case is similar to Case B except the pipeline is divided into five 200-mile (322 km) pipeline segments with one lead compressor station and 4 intermediate compressor stations. In each station, the pressure is raised from 615 Psia to 1600 Psia (4.24 to 11.03 MPa) in one stage and then cooled to 100 ˚F (37.8 ˚C), passed through a separator before entering the downstream pipeline segment.

     

    Simulation Results and Discussions:

    The PFDs for the three cases are simulated using ProMax [3]. To improve the accuracy and to take care of variations of physical properties of gas, each pipeline segment length was divided into 10 sub segments. For Case A in which pipeline segment was considerably longer, we tried 50 and 100 sub segments and no change in the outlet pressure and temperature was observed. Table 3 presents a summary of simulation results for the three cases in the field and SI system of units. As can be seen in this table, Case A requires the least total compression power and heat duty requirements. The power reduction for Case A is about 51%  compare to Case B and 63% compare to Case C. These reductions in power and heat duty requirements are considerable.  Similarly, the heat duty reduction for Case A is about 39% compared to Case B and 50 % compare to Case C, respectively.

    Table 3. Summary of computer simulation results for the three cases.

    Figure 4 presents the phase envelope, the required compression and cooling stages and pipeline pressure-temperature profile for Case A. This figure shows that the pipeline outlet condition ends up to the right of the dew point curve with the gas remaining as single phase.

    Figure 4. Phase envelope, compression and cooling stages and pipeline pressure-temperature profile (ID=42 in = 1067 mm)

    Pipeline wall thickness is an important economic factor. The wall thickness, t, for the three cases was calculated by:

    Where,

    P is maximum allowable operating pressure, here set to 1.1 times the inlet pressure,

    OD is outside diameter,

    E is joint efficiency (assumed to be 1),

    f1 is wall thickness tolerance (assumed to be 1.0),

    f2 is design factor, 0.4 to 0.72  and here set  to be 0.72 for remote area),

    σ is the pipe material yield stress (assumed pipe material grade X65 to be 65,000 psi or

    448.2 MPa), and

    CA is the corrosion allowance (assumed to be 0 in or 0 mm, for dry gas).

     

    Figure 5 presents the calculated wall thickness as a function of the inlet pressure (for the three cases). Notice Case A requires the largest and Case C requires the smallest wall thickness.

    Variation of density, viscosity, velocity, pressure, and temperature along the pipeline are shown in Figures 6 through 10 for Cases A and B.

    Conclusions:

    We have studied transportation of natural gas in the dense phase region (high pressure) and compared the results with the cases of transporting the same gas using intermediate and low pressures. Our study highlights the following features:

    1. If the gas at the source is not at high enough pressure, considerable compression power and cooling duty may be required if the decision is to use the dense phase.
    2. For the dense phase – Case A, (high pressure), higher wall thickness is required.
    3. For the dense phase – Case A, lower compressor power and heat duty are required.
    4. For the dense phase – Case A, the friction pressure drop / mile is lower .
    5. For the dense phase – Case A and the same diameter, on the average the velocity is lower compared to lower pressure gas transportation.

    Other logical results can be stated as well including:

    1. Composition of the gas plays an important role.
    2. Pipeline elevation profile and distance may be  important factors at the higher operating pressures.
    3. A detailed economic analysis in terms of CAPEX and OPEX should be made for a sound comparison.

    In a future Tip of the Month, we will consider the design and order of magnitude costs impacts when constructing each of these three cases, first onshore then offshore.

    To learn more about similar cases and how to minimize operational problems, we suggest attending our G40 (Process/Facility Fundamentals), G4 (Gas Conditioning and Processing), G5 (Gas Conditioning and Processing-Special), P81 (CO2 Surface Facilities), PF4 (Oil Production and Processing Facilities), and PL 4 (Fundamentals of Onshore and Offshore Pipeline Systems) courses.

    John M. Campbell Consulting (JMCC) offers consulting expertise on this subject and many others. For more information about the services JMCC provides, visit our website at www.jmcampbellconsulting.com, or email your consulting needs to consulting@jmcampbell.com.

    By: Mahmood Moshfeghian and David Hairston

    References:

    1. Beaubouef, B., “Nord stream completes the world’s longest subsea pipeline,” Offshore, P30, December 2011.
    2. http://www.jmcampbell.com/tip-of-the-month/
    3. ProMax 3.2, Bryan Research and Engineering, Inc., Bryan, Texas, 2012.

     

    Figure 5. Variation of wall thickness with pipeline inlet pressure

    Figure 6. Variation of gas density in the pipeline (Cases A and B)

    Figure 7. Variation of gas viscosity in the pipeline (Cases A and B)

    Figure 8. Variation of gas velocity in the pipeline (Cases A and B)

    Figure 9. Variation of pressure in the pipeline (Cases A and B)

    Figure 10. Variation of temperature in the pipeline (Cases A and B)