Compressor Efficiency Calculation 301y3x
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How to Estimate Compressor Efficiency? In the November 2011 tip of the month (TOTM) we presented the compressor calculations of a case study. We compared the rigorous method results with the values from the shortcut methods. The rigorous method was based on an equation of state like the Soave-Redlich-Kwong (SRK) for calculating the required enthalpies and entropies. The enthalpies and entropies are used to determine the power requirement and the discharge temperatures. The results indicated that the accuracy of the shortcut method is sensitive to the value of ideal gas state heat capacity ratio, k. From a calculation viewpoint alone, the power calculation is particularly sensitive to the specification of mass flow rate, suction temperature and pressure, and discharge temperature and pressure. A compressor is going to operate under varying values of the variables affecting its performance. Thus the most difficult part of a compressor calculation is specification of a reasonable range for each variable and not the calculation itself. Reference [1] emphasizes that using a single value for each variable is not the correct way to evaluate a compression system. Normally, the thermodynamic calculations are performed for an ideal (reversible) process. The results of a reversible process are then adapted to the real world through the use of a thermodynamic efficiency. In the compression process there are three ideal processes that can be visualized: 1) an isothermal process (PV1=C1), 2) an isentropic process (PVk=C2) and 3) a polytropic process (PVn=C3). Any one of these processes can be used suitably as a basis for evaluating compression power requirements by either hand or computer calculation. The isothermal process, however, is seldom used as a basis because the normal industrial compression process is not even approximately carried out at constant temperature. Note that Dresser Rand is doing quite a lot of work with “Near constant temperature” compression especially for CO2compression from vent stacks. For detail refere to: http://www.nist.gov/pml/high_megawatt//6_1-Approved-Moore.pdf In this TOTM, we will demonstrate how to determine the efficiency of a compressor from measured flow rate, composition, suction and discharge temperatures and pressures. A rigorous calculation based on an equation of state and a shortcut method are considered and the results are compared. Compress Efficiency Compressor efficiencies vary with compressor type, size, and throughput. They can only be determined (afterward) by a compressor test, although compressor manufacturers can usually provide good estimates. For planning purposes, reference [2] suggests the following values for the overall efficiencies: Table 1. Overall Compressor Efficiencies [2]
Compressor Type
Efficiency, η
Centrifugal
0.70 – 0.85
High Speed Reciprocating0.72 – 0.85
Low Speed Reciprocating 0.75 – 0.90
Rotary Screw
0.65 – 0.75
Reference [2] indicates that these overall efficiencies include gas friction within the compressor, the mechanical losses (bearings, seals, gear-box, etc.), and gear-box losses. The mechanical efficiency varies with compressor size and type, but 95% is a useful planning number. When calculating the compressor head and discharge temperature the efficiency used will be isentropic or polytropic (isentropic efficiency is sometimes called adiabatic efficiency). Adding 3-4 % efficiency (mechanical losses) to the overall efficiencies in Table 1 will generally give a good estimate of the thermodynamic efficiency [2]. To evaluate the performance of an existing compressor, the objective is to calculate the compressor efficiency (η) and power requirement. Known and measured properties are: a. Standard condition gas volume flow rate (qS) or gas mass rate () b. Gas composition (zi) c. Suction pressure (P1) and temperature (T1) d. Discharge pressure (P2) and temperature (T2) Estimating Efficiency – Rigorous Method The heart of any commercial process flow simulation software is an equation of state. Due to their simplicity and relative accuracy, a cubic EOS such as Soave Redlich-Kwong (SRK) [3] or Peng-Robinson [4] is used. These equations are used to calculate Vapor-Liquid-Equilibria (VLE), enthalpy (h), and entropy (s). With proper binary interaction coefficients, the process simulation results of these two equations are practically the same. Therefore, only the SRK is used in this work. The isentropic efficiency is defined by
Where: ηIsen = Isentropic efficiency
h1 = Suction enthalpy calculated at P1, T1, and composition (zi) h2 = Discharge enthalpy calculated at P2, T2, and composition (zi) h2Isen = Isentropic discharge enthalpy at P2 (or T2), S2Isen =S1, and composition (zi)
= Mass flow rate The computation compressor efficiency or power involves two steps 1. Determination of the ideal or isentropic (reversible and adiabatic) enthalpy change (h2Isen-h1) of the compression process. 2. Determination of the actual enthalpy change (h2-h1). The step-by-step calculation based on an EOS: a. Assume steady state, i.e. b. Assume the feed composition remain unchanged c. Calculate suction enthalpy h1=f(P1, T1, and zi) and entropy s1=f(P1, T1, and zi) by EOS d. Assume isentropic process and set s2Isen = f (P2, T2Isen, zi) = s1 = f (P1, T1, zi). e. Calculate the ideal enthalpy (h2Isen) at discharge condition for known zi, T2 (or P2) and s2Isen. f. Calculate the actual enthalpy (h2) at discharge condition for known zi, T2 and P2. g. Calculate isentropic efficiency by Equation 1: µIsen = (h2Isen – h1)/(h2 – h1)
h. Calculate power by Equation 2: Estimating Efficiency – Shortcut Method The isentropic path exponent (k) or ideal gas heat capacity ratio (k=/CV) can be calculated by the correlation presented in the May 2013 TOTM:
Where: T = Temperature, K (°R) = Gas relative density; ratio of gas molecular weight to air molecular weight A = 0.000272 (0.000151) The actual discharge temperature based on an isentropic path can be estimated by
Solving for the isentropic efficiency,
Similarly, the actual discharge temperature based on a polytropic path can be estimated by
Solving the above equation for the polytropic path coefficient (n):
Similarly, the actual discharge temperature based on a polytropic path can be estimated (ηPoly) by:
The isentropic head is calculated by
Similarly, the polytropic head is calculated by
For an isentropic (reversible and adiabatic) process the power is calculated by
Or for a polytropic process the power is calculated by
Alternatively:
Where: Head = Compressor head, m (ft) Power = Compressor power, kW (HP) R = Universal gas constant, 848 kg-m/(kmol-K) or (1545 ft-lbf/(lbmol-°R)) PS = Standard condition pressure, kPa (psia) P1 = Suction pressure, kPa (psia) P2 = Discharge pressure, kPa (psia) TS = Standard condition temperature, K (°R) T1 = Suction temperature, K (°R) T2 = Discharge temperature, K (°R) qS = Gas volumetric rate at the standard condition, Sm3/d (scf/day) Za = Average gas compressibility factor = (Z1+Z2)/2 Z1 = Gas compressibility factor at the suction condition Z2 = Gas compressibility factor at the discharge condition MW = Gas molecular weight The power calculation should be made per stage of compression and then summed for all stages connected to a single driver.
The step-by-step calculation for shortcut method a. Calculate the isentropic exponent (k) by Equation 3 using the average temperature defined by T = (T1+3T2)/4. This form of average temperature was defined to obtain better match between the rigorous and shortcut method results. b. Calculate the isentropic efficiency (ηIsen) by Equation 5. c. Calculate the polytropic coefficient (n) by Equation 7. d. Calculate the polytropic efficiency (ηPoly) by Equation 8. e. Calculate the isentropic and polytropic heads by Equations 9 and 10, respectively. f. Calculate the required power per stage by either Equation 11 or 12. Case Study A natural gas mixture is compressed using a three-stage centrifugal compressor. The process flow diagram is shown in Figure 1. For each stage, the measured pressure, and temperature are presented in Table 1. The measured feed composition, flowrates, and calculated molecular weight and relative density are presented in Table 2.
Figure 1. Process flow diagram for a 3-stage compression Table 1. Measured temperature and pressure for the three stages of compression
Table 2. Gas analysis and flow rate for the three stages of compression
* Calculated Results and Discussions The process flow diagram shown in Figure 1 was simulated by ProMax software [5] to perform the rigorous calculations using the SRK EOS. The program calculated polytropic and isentropic efficiencies, heads, and compression power. The program also calculated the isentropic path exponent (k), and polytropic path exponent (n). These calculated results are presented in Table 2 for all three stages under SRK headingings. The calculations performed by ProMax are very similar to the step-by-step of a through h described in the rigorous section. Table 2 also presents the shortcut caculation results for the corresponding values under the shortcut heading. The shortcut calculations are based on the step-by-step of a through f described in the shortcut method section. The error percent between the rigrous method and the shortcut methods for each stage are presented in Table 2, too. Table 2 indicates that excellent agreements are obtained for stages 1 and 2. However, larger deviations are obseved for the isetropic and polytropic exponents of stage 3 due to high pressure operation which deviated too far from ideal gas state conditions. Table 3. Summary of the rigorous and shortcut calculated results
Conclusions Table 2 indicates that there are good agreements between the shortcut and the rigorous results. The differences between the rigorous and shortcut method results for facilities calculations and planning purposes are negligible. For stage 3, due to high-pressure operation and deviating too far from the ideal gas state condition, a larger error is observed for the isentropic exponent (k). The calculated isentropic exponent (k) in the ProMax [5] is not the ideal gas state heat capacity (/CV) ratio. It is the value of the isentropic exponent that is required to yield an isentropic path from inlet to outlet. Its value is calculated as an integration of that path. Thus it is somewhat of an “average” value representing the true isentropic path. For ideal gases, the value would be equal (/CV) ratio. This error in ‘k’ also illustrates the importance of specifying which correlation is to be used when ordering a performance test (ie, refer to ASME PTC-10 for additional details), so that client and vendor are on the same agreement moving forwards with regard to molecular weight (MW) and k for the test fluid. For further detail refer to reference [6] and August and September 2010 TOTMs [7, 8]. It may also be worth noting that when trending ‘n’ and the polytropic efficiency to evaluate machine condition, the relative accuracy of measurement instrument/equipment (temperature and pressure transducers) and mapping of compressor performance to the original performance curve (actual gas volume flow rate vs speed), introduces many potential erroneous sources into this daily evaluation. Note that the accuracy of the shortcut methods is dependent on the values of k and n. The definition of average temperature in the shortcut method was adjusted to obtain a better match between the isentropic path exponent (k) calculated by rigorous method. To learn more about similar cases and how to minimize operational problems, we suggest attending our G4 (Gas Conditioning and Processing), PF4 (Oil Production and Processing Facilities), ME46 (Compressor Systems–Mechanical Design and Specifications) and ME44 (Fundamentals of Pump and Compressors Systems), courses. PetroSkills offers consulting expertise on this subject and many others. For more information about these services, visit our website at http://petroskills.com/consulting, or email us at [email protected]. Dr. Mahmood Moshfeghian Reference:
1. Maddox, R. N. and L. L. Lilly, “Gas conditioning and processing, Volume 3: Advanced Techniques and Applications,” John M. Campbell and Company, 2nd Ed., Norman, Oklahoma, USA, 1990. 2. Campbell, J.M., Gas Conditioning and Processing, Volume 2: The Equipment Modules, 9th Edition, 2nd Printing, Editors Hubbard, R. and Snow–McGregor, K., Campbell Petroleum Series, Norman, Oklahoma, 2014. 3. Soave, G., Chem. Eng. Sci., Vol. 27, pp. 1197-1203, 1972. 4. Peng, D. Y., and Robinson, D. B., Ind. Eng. Chem. Fundam., Vol. 15, p. 59, 1976. 5. ProMax 3.2, Bryan Research and Engineering, Inc, Bryan, Texas, 2014. 6. ASME PTC-10, “Performance test Code on Compressors and Exhausters”, 1997. 7. Honeywell, J. “Important Aspects of Centrifugal Compressor Testing-Part 1”, Tip of the Month, August 2010 8. Honeywell, J. “Important Aspects of Centrifugal Compressor Testing-Part 2”, Tip of the Month, September 2010 Did you enjoy this post? Do you have a question? Leave us a Comment below! Want to read more articles like this? Subscribe to our RSS Feed or visit the Tip of the Month Archives for past articles. Posted on July 1, 2015 at 12:00 am 11 comments Categories: Gas Processing, Mechanical, Pipeline, Process Facilities Recieve new post updates: Entries (RSS) Recieve follow up comments updates: RSS 2.0
Written by Dr. Mahmood Moshfeghian DR. MAHMOOD MOSHFEGHIAN is a Senior Technical Advisor and Senior Instructor. He is the author of most Tips of the Month and develops technical software for PetroSkills. He has 40 years teaching experience in universities as well as for oil and gas industries. Dr. Moshfeghian ed JMC in 1990 as a part time consultant and then as full time instructor/consultant in 2005. Moshfeghian was Professor of Chemical Engineering at Shiraz University. Dr. Moshfeghian is a senior member of AIChE and has published more than 125 technical papers on thermodynamic properties and Process Engineering. Dr. Moshfeghian has presented invited papers in international conferences. He is a member of the Editorial Board for the International Journal of Oil, Gas, and Coal Technology and a member of the GPSA Technical Committee Group F. He holds B.S. (74), M.S. (75) and and PhD (78) degrees in Chemical Engineering, all from Oklahoma State University. View all posts by: Dr. Mahmood Moshfeghian « Previous post Next Post »
11 responses to “How to Estimate Compressor Efficiency?” 1. Paul says: August 31, 2015 at 7:11 am
thanks for the article, I would also mention that rigorous methods (based on interpolated values such as ASME PTC-10 or numerical integration pin->pout such as Huntington etc.) consider non-contant values for properties from pin->pout, these variations may originate large errors (see the example provided in Huntington’s paper), finally, a procedure can also consider phase equilibria, I know Prode Properties (see http://www.prode.com/docs/pppman.pdf) which includes both Huntington and a proprietary method for solving a polytropic stage with phase equilibria, when there is a change of phase it is difficult to evaluate and adopt a value for efficiency in different conditions… Reply 2.
Francis says: December 28, 2015 at 9:30 am Please may I know the equation seven. I cannot find the formula for calculating the polytropic path exponent(n). Please can u write the formula for calculating polytropic path exponent Reply o
Laurent says: February 25, 2016 at 8:37 am There is an obvious mistake in (7) when you inverse (6). Reply
Dr. Mahmood Moshfeghian says: February 27, 2016 at 9:54 am Laurent: You are correct, both temperature and pressure ratios should have been ln(T2/T1) and ln(P2/P1). Thanks. Reply
3.
Daniel says: April 22, 2016 at 3:51 am Hello, used these equations with preos… did not work, gave me an efficiency of 4000… Reply
4. Ray Fang says: April 25, 2016 at 9:32 pm us to learn about CAE350 CAE350 compressor analyzing system is a low cost portable system to test the capacity,power efficiency and unit air consumption of the compressor with [email protected] to know more
Reply 5.
Panos says: June 17, 2016 at 4:19 pm Here is the link of a new article, which describes the rigorous calculation of the polytropic efficiency based on thermodynamics of real gases. A comparison with data shown on this website (!) can also be found, under: http://www.degruyter.com/view/j/tjj.ahead-of-print/tjj-2016-0029/tjj-2016-0029.xml?format=INT Reply o
Arif says: November 2, 2016 at 12:55 pm Panos, the link does not work Reply
o
Arif says: November 2, 2016 at 12:56 pm Panos, nothing works as the link Reply
6.
Norman Day says: September 7, 2016 at 3:21 pm Please calculate or estimate overall efficiency of the following AIR 5.4 bore 6.5 stroke 1800-2400 RPM mechanical valves from a Caterpillar 3406 Diesel engine Reply
7.
Norman Day says: September 7, 2016 at 3:25 pm Please calculate or estimate overall efficiency of; AIR BORE 5.4 INCHES STROKE 6.5 INCHES 1800-2400 RPM Mechanical valves Caterpillar 3406 Diesel Engine is 85% practical? Reply
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How to Estimate Compressor Efficiency? In the November 2011 tip of the month (TOTM) we presented the compressor calculations of a case study. We compared the rigorous method results with the values from the shortcut methods. The rigorous method was based on an equation of state like the Soave-Redlich-Kwong (SRK) for calculating the required enthalpies and entropies. The enthalpies and entropies are used to determine the power requirement and the discharge temperatures. The results indicated that the accuracy of the shortcut method is sensitive to the value of ideal gas state heat capacity ratio, k. From a calculation viewpoint alone, the power calculation is particularly sensitive to the specification of mass flow rate, suction temperature and pressure, and discharge temperature and pressure. A compressor is going to operate under varying values of the variables affecting its performance. Thus the most difficult part of a compressor calculation is specification of a reasonable range for each variable and not the calculation itself. Reference [1] emphasizes that using a single value for each variable is not the correct way to evaluate a compression system. Normally, the thermodynamic calculations are performed for an ideal (reversible) process. The results of a reversible process are then adapted to the real world through the use of a thermodynamic efficiency. In the compression process there are three ideal processes that can be visualized: 1) an isothermal process (PV1=C1), 2) an isentropic process (PVk=C2) and 3) a polytropic process (PVn=C3). Any one of these processes can be used suitably as a basis for evaluating compression power requirements by either hand or computer calculation. The isothermal process, however, is seldom used as a basis because the normal industrial compression process is not even approximately carried out at constant temperature. Note that Dresser Rand is doing quite a lot of work with “Near constant temperature” compression especially for CO2compression from vent stacks. For detail refere to: http://www.nist.gov/pml/high_megawatt//6_1-Approved-Moore.pdf In this TOTM, we will demonstrate how to determine the efficiency of a compressor from measured flow rate, composition, suction and discharge temperatures and pressures. A rigorous calculation based on an equation of state and a shortcut method are considered and the results are compared. Compress Efficiency Compressor efficiencies vary with compressor type, size, and throughput. They can only be determined (afterward) by a compressor test, although compressor manufacturers can usually provide good estimates. For planning purposes, reference [2] suggests the following values for the overall efficiencies: Table 1. Overall Compressor Efficiencies [2]
Compressor Type
Efficiency, η
Centrifugal
0.70 – 0.85
High Speed Reciprocating0.72 – 0.85
Low Speed Reciprocating 0.75 – 0.90
Rotary Screw
0.65 – 0.75
Reference [2] indicates that these overall efficiencies include gas friction within the compressor, the mechanical losses (bearings, seals, gear-box, etc.), and gear-box losses. The mechanical efficiency varies with compressor size and type, but 95% is a useful planning number. When calculating the compressor head and discharge temperature the efficiency used will be isentropic or polytropic (isentropic efficiency is sometimes called adiabatic efficiency). Adding 3-4 % efficiency (mechanical losses) to the overall efficiencies in Table 1 will generally give a good estimate of the thermodynamic efficiency [2]. To evaluate the performance of an existing compressor, the objective is to calculate the compressor efficiency (η) and power requirement. Known and measured properties are: a. Standard condition gas volume flow rate (qS) or gas mass rate () b. Gas composition (zi) c. Suction pressure (P1) and temperature (T1) d. Discharge pressure (P2) and temperature (T2) Estimating Efficiency – Rigorous Method The heart of any commercial process flow simulation software is an equation of state. Due to their simplicity and relative accuracy, a cubic EOS such as Soave Redlich-Kwong (SRK) [3] or Peng-Robinson [4] is used. These equations are used to calculate Vapor-Liquid-Equilibria (VLE), enthalpy (h), and entropy (s). With proper binary interaction coefficients, the process simulation results of these two equations are practically the same. Therefore, only the SRK is used in this work. The isentropic efficiency is defined by
Where: ηIsen = Isentropic efficiency
h1 = Suction enthalpy calculated at P1, T1, and composition (zi) h2 = Discharge enthalpy calculated at P2, T2, and composition (zi) h2Isen = Isentropic discharge enthalpy at P2 (or T2), S2Isen =S1, and composition (zi)
= Mass flow rate The computation compressor efficiency or power involves two steps 1. Determination of the ideal or isentropic (reversible and adiabatic) enthalpy change (h2Isen-h1) of the compression process. 2. Determination of the actual enthalpy change (h2-h1). The step-by-step calculation based on an EOS: a. Assume steady state, i.e. b. Assume the feed composition remain unchanged c. Calculate suction enthalpy h1=f(P1, T1, and zi) and entropy s1=f(P1, T1, and zi) by EOS d. Assume isentropic process and set s2Isen = f (P2, T2Isen, zi) = s1 = f (P1, T1, zi). e. Calculate the ideal enthalpy (h2Isen) at discharge condition for known zi, T2 (or P2) and s2Isen. f. Calculate the actual enthalpy (h2) at discharge condition for known zi, T2 and P2. g. Calculate isentropic efficiency by Equation 1: µIsen = (h2Isen – h1)/(h2 – h1)
h. Calculate power by Equation 2: Estimating Efficiency – Shortcut Method The isentropic path exponent (k) or ideal gas heat capacity ratio (k=/CV) can be calculated by the correlation presented in the May 2013 TOTM:
Where: T = Temperature, K (°R) = Gas relative density; ratio of gas molecular weight to air molecular weight A = 0.000272 (0.000151) The actual discharge temperature based on an isentropic path can be estimated by
Solving for the isentropic efficiency,
Similarly, the actual discharge temperature based on a polytropic path can be estimated by
Solving the above equation for the polytropic path coefficient (n):
Similarly, the actual discharge temperature based on a polytropic path can be estimated (ηPoly) by:
The isentropic head is calculated by
Similarly, the polytropic head is calculated by
For an isentropic (reversible and adiabatic) process the power is calculated by
Or for a polytropic process the power is calculated by
Alternatively:
Where: Head = Compressor head, m (ft) Power = Compressor power, kW (HP) R = Universal gas constant, 848 kg-m/(kmol-K) or (1545 ft-lbf/(lbmol-°R)) PS = Standard condition pressure, kPa (psia) P1 = Suction pressure, kPa (psia) P2 = Discharge pressure, kPa (psia) TS = Standard condition temperature, K (°R) T1 = Suction temperature, K (°R) T2 = Discharge temperature, K (°R) qS = Gas volumetric rate at the standard condition, Sm3/d (scf/day) Za = Average gas compressibility factor = (Z1+Z2)/2 Z1 = Gas compressibility factor at the suction condition Z2 = Gas compressibility factor at the discharge condition MW = Gas molecular weight The power calculation should be made per stage of compression and then summed for all stages connected to a single driver.
The step-by-step calculation for shortcut method a. Calculate the isentropic exponent (k) by Equation 3 using the average temperature defined by T = (T1+3T2)/4. This form of average temperature was defined to obtain better match between the rigorous and shortcut method results. b. Calculate the isentropic efficiency (ηIsen) by Equation 5. c. Calculate the polytropic coefficient (n) by Equation 7. d. Calculate the polytropic efficiency (ηPoly) by Equation 8. e. Calculate the isentropic and polytropic heads by Equations 9 and 10, respectively. f. Calculate the required power per stage by either Equation 11 or 12. Case Study A natural gas mixture is compressed using a three-stage centrifugal compressor. The process flow diagram is shown in Figure 1. For each stage, the measured pressure, and temperature are presented in Table 1. The measured feed composition, flowrates, and calculated molecular weight and relative density are presented in Table 2.
Figure 1. Process flow diagram for a 3-stage compression Table 1. Measured temperature and pressure for the three stages of compression
Table 2. Gas analysis and flow rate for the three stages of compression
* Calculated Results and Discussions The process flow diagram shown in Figure 1 was simulated by ProMax software [5] to perform the rigorous calculations using the SRK EOS. The program calculated polytropic and isentropic efficiencies, heads, and compression power. The program also calculated the isentropic path exponent (k), and polytropic path exponent (n). These calculated results are presented in Table 2 for all three stages under SRK headingings. The calculations performed by ProMax are very similar to the step-by-step of a through h described in the rigorous section. Table 2 also presents the shortcut caculation results for the corresponding values under the shortcut heading. The shortcut calculations are based on the step-by-step of a through f described in the shortcut method section. The error percent between the rigrous method and the shortcut methods for each stage are presented in Table 2, too. Table 2 indicates that excellent agreements are obtained for stages 1 and 2. However, larger deviations are obseved for the isetropic and polytropic exponents of stage 3 due to high pressure operation which deviated too far from ideal gas state conditions. Table 3. Summary of the rigorous and shortcut calculated results
Conclusions Table 2 indicates that there are good agreements between the shortcut and the rigorous results. The differences between the rigorous and shortcut method results for facilities calculations and planning purposes are negligible. For stage 3, due to high-pressure operation and deviating too far from the ideal gas state condition, a larger error is observed for the isentropic exponent (k). The calculated isentropic exponent (k) in the ProMax [5] is not the ideal gas state heat capacity (/CV) ratio. It is the value of the isentropic exponent that is required to yield an isentropic path from inlet to outlet. Its value is calculated as an integration of that path. Thus it is somewhat of an “average” value representing the true isentropic path. For ideal gases, the value would be equal (/CV) ratio. This error in ‘k’ also illustrates the importance of specifying which correlation is to be used when ordering a performance test (ie, refer to ASME PTC-10 for additional details), so that client and vendor are on the same agreement moving forwards with regard to molecular weight (MW) and k for the test fluid. For further detail refer to reference [6] and August and September 2010 TOTMs [7, 8]. It may also be worth noting that when trending ‘n’ and the polytropic efficiency to evaluate machine condition, the relative accuracy of measurement instrument/equipment (temperature and pressure transducers) and mapping of compressor performance to the original performance curve (actual gas volume flow rate vs speed), introduces many potential erroneous sources into this daily evaluation. Note that the accuracy of the shortcut methods is dependent on the values of k and n. The definition of average temperature in the shortcut method was adjusted to obtain a better match between the isentropic path exponent (k) calculated by rigorous method. To learn more about similar cases and how to minimize operational problems, we suggest attending our G4 (Gas Conditioning and Processing), PF4 (Oil Production and Processing Facilities), ME46 (Compressor Systems–Mechanical Design and Specifications) and ME44 (Fundamentals of Pump and Compressors Systems), courses. PetroSkills offers consulting expertise on this subject and many others. For more information about these services, visit our website at http://petroskills.com/consulting, or email us at [email protected]. Dr. Mahmood Moshfeghian Reference:
1. Maddox, R. N. and L. L. Lilly, “Gas conditioning and processing, Volume 3: Advanced Techniques and Applications,” John M. Campbell and Company, 2nd Ed., Norman, Oklahoma, USA, 1990. 2. Campbell, J.M., Gas Conditioning and Processing, Volume 2: The Equipment Modules, 9th Edition, 2nd Printing, Editors Hubbard, R. and Snow–McGregor, K., Campbell Petroleum Series, Norman, Oklahoma, 2014. 3. Soave, G., Chem. Eng. Sci., Vol. 27, pp. 1197-1203, 1972. 4. Peng, D. Y., and Robinson, D. B., Ind. Eng. Chem. Fundam., Vol. 15, p. 59, 1976. 5. ProMax 3.2, Bryan Research and Engineering, Inc, Bryan, Texas, 2014. 6. ASME PTC-10, “Performance test Code on Compressors and Exhausters”, 1997. 7. Honeywell, J. “Important Aspects of Centrifugal Compressor Testing-Part 1”, Tip of the Month, August 2010 8. Honeywell, J. “Important Aspects of Centrifugal Compressor Testing-Part 2”, Tip of the Month, September 2010 Did you enjoy this post? Do you have a question? Leave us a Comment below! Want to read more articles like this? Subscribe to our RSS Feed or visit the Tip of the Month Archives for past articles. Posted on July 1, 2015 at 12:00 am 11 comments Categories: Gas Processing, Mechanical, Pipeline, Process Facilities Recieve new post updates: Entries (RSS) Recieve follow up comments updates: RSS 2.0
Written by Dr. Mahmood Moshfeghian DR. MAHMOOD MOSHFEGHIAN is a Senior Technical Advisor and Senior Instructor. He is the author of most Tips of the Month and develops technical software for PetroSkills. He has 40 years teaching experience in universities as well as for oil and gas industries. Dr. Moshfeghian ed JMC in 1990 as a part time consultant and then as full time instructor/consultant in 2005. Moshfeghian was Professor of Chemical Engineering at Shiraz University. Dr. Moshfeghian is a senior member of AIChE and has published more than 125 technical papers on thermodynamic properties and Process Engineering. Dr. Moshfeghian has presented invited papers in international conferences. He is a member of the Editorial Board for the International Journal of Oil, Gas, and Coal Technology and a member of the GPSA Technical Committee Group F. He holds B.S. (74), M.S. (75) and and PhD (78) degrees in Chemical Engineering, all from Oklahoma State University. View all posts by: Dr. Mahmood Moshfeghian « Previous post Next Post »
11 responses to “How to Estimate Compressor Efficiency?” 1. Paul says: August 31, 2015 at 7:11 am
thanks for the article, I would also mention that rigorous methods (based on interpolated values such as ASME PTC-10 or numerical integration pin->pout such as Huntington etc.) consider non-contant values for properties from pin->pout, these variations may originate large errors (see the example provided in Huntington’s paper), finally, a procedure can also consider phase equilibria, I know Prode Properties (see http://www.prode.com/docs/pppman.pdf) which includes both Huntington and a proprietary method for solving a polytropic stage with phase equilibria, when there is a change of phase it is difficult to evaluate and adopt a value for efficiency in different conditions… Reply 2.
Francis says: December 28, 2015 at 9:30 am Please may I know the equation seven. I cannot find the formula for calculating the polytropic path exponent(n). Please can u write the formula for calculating polytropic path exponent Reply o
Laurent says: February 25, 2016 at 8:37 am There is an obvious mistake in (7) when you inverse (6). Reply
Dr. Mahmood Moshfeghian says: February 27, 2016 at 9:54 am Laurent: You are correct, both temperature and pressure ratios should have been ln(T2/T1) and ln(P2/P1). Thanks. Reply
3.
Daniel says: April 22, 2016 at 3:51 am Hello, used these equations with preos… did not work, gave me an efficiency of 4000… Reply
4. Ray Fang says: April 25, 2016 at 9:32 pm us to learn about CAE350 CAE350 compressor analyzing system is a low cost portable system to test the capacity,power efficiency and unit air consumption of the compressor with [email protected] to know more
Reply 5.
Panos says: June 17, 2016 at 4:19 pm Here is the link of a new article, which describes the rigorous calculation of the polytropic efficiency based on thermodynamics of real gases. A comparison with data shown on this website (!) can also be found, under: http://www.degruyter.com/view/j/tjj.ahead-of-print/tjj-2016-0029/tjj-2016-0029.xml?format=INT Reply o
Arif says: November 2, 2016 at 12:55 pm Panos, the link does not work Reply
o
Arif says: November 2, 2016 at 12:56 pm Panos, nothing works as the link Reply
6.
Norman Day says: September 7, 2016 at 3:21 pm Please calculate or estimate overall efficiency of the following AIR 5.4 bore 6.5 stroke 1800-2400 RPM mechanical valves from a Caterpillar 3406 Diesel engine Reply
7.
Norman Day says: September 7, 2016 at 3:25 pm Please calculate or estimate overall efficiency of; AIR BORE 5.4 INCHES STROKE 6.5 INCHES 1800-2400 RPM Mechanical valves Caterpillar 3406 Diesel Engine is 85% practical? Reply
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