Liquefaction Process Evaluation for Floating LNG. Maya Kusmaya, Trondheim 2014

Similar documents
LEAN LNG PLANTS HEAVY ENDS REMOVAL AND OPTIMUM RECOVERY OF LIGHT HYDROCARBONS FOR REFRIGERANT MAKE-UP

Natural gas liquids recovery from gas turbine fuel

NATURAL GAS LIQUEFACTION TECHNOLOGY FOR FLOATING LNG FACILITIES

The LNG industry has experienced significant. a suitable process

ECONOMICAL OPTIONS FOR RECOVERING NGL / LPG AT LNG RECEIVING TERMINALS

How To Make A High Co 2 Gas Blend

Liquefied Natural Gas (LNG)

HOW THE RIGHT TECHNICAL CHOICES LEAD TO COMMERCIAL SUCCESS

Open Cycle Refrigeration System

SUPERSONIC GAS CONDITIONING - COMMERCIALISATION OF TWISTER TECHNOLOGY

Comparative Economic Investigation Options for Liquefied Petroleum Gas Production from Natural Gas Liquids

DESIGNING MOLECULAR SIEVE DEHYDRATION UNITS TO PREVENT UPSETS IN DOWNSTREAM NGL/LPG RECOVERY PLANTS

Technical Evaluation of C3-MR and Cascade Cycle on Natural Gas Liquefaction Process

PERFORMANCE EVALUATION OF NGCC AND COAL-FIRED STEAM POWER PLANTS WITH INTEGRATED CCS AND ORC SYSTEMS

IBP 2778_10 HIGH EFFICIENCY ON CO2 REMOVAL IN NATURAL GAS WITH UCARSOL SOLVENTS Thiago V. Alonso 1. Abstract. 1. Introduction

Efficiency of Hydrogen Liquefaction Plants

How To Calculate The Performance Of A Refrigerator And Heat Pump

OPTIMAL POLYGEN COOLING CONCEPT FOR ST. OLAVS HOSPITAL IN TRONDHEIM, NORWAY

Natural Gas Developments

UNIT 2 REFRIGERATION CYCLE

Putting a chill on global warming

Optimization of Natural Gas Processing Plants Including Business Aspects

GTI Small-Scale Liquefaction Technology. March 2013

APPLIED THERMODYNAMICS TUTORIAL 1 REVISION OF ISENTROPIC EFFICIENCY ADVANCED STEAM CYCLES

FUNDAMENTALS OF ENGINEERING THERMODYNAMICS

DEVELOPMENT OF A TWIN SCREW EXPRESSOR AS A THROTTLE VALVE REPLACEMENT FOR WATER-COOLED CHILLERS

Dry-out Design Considerations and Practices for Cryogenic Gas Plants

Modelling and Simulation of the Freezing Systems and Heat Pumps Using Unisim Design

Chapter 2 P-H Diagram Refrigeration Cycle Analysis & Refrigerant Flow Diagram

The paper addresses the boil-off in the cryogenic industry and details the specifics of it when applied to vehicle LNG tanks.

Chapter 10: Refrigeration Cycles

The Second Law of Thermodynamics

COMMERCIAL HVAC CHILLER EQUIPMENT. Air-Cooled Chillers

GAS TURBINE INLET AIR CHILLING FOR LNG

Chemical Analysis. Natural Gas Analyzer. A Family of optimized GC Solutions. Gas Chromatography. think forward

Analysis of Ammonia Water (NH3-H2O) Vapor Absorption Refrigeration System based on First Law of Thermodynamics

Facts about gas physical properties

OPTIMAL DESIGN AND OPERATION OF HELIUM REFRIGERATION SYSTEMS *

A Focus on Balance A Novel Approach Taking the Phillips Optimized Cascade LNG Process Into the Future

ALONE. small scale solar cooling device Project No TREN FP7EN Project No TREN/FP7EN/ ALONE. small scale solar cooling device

Turbine Inlet Cooling

Freeport LNG Liquefaction Project

Thermal Coupling Of Cooling and Heating Systems

Water Fired Chiller/Chiller-Heater. WFC-S Series: 10, 20 and 30 RT Cooling

HVAC Systems: Overview

SASO XXXX:2016. (Including the modifications approved in Saudi Council Board No. XXX/2016) LARGE CAPACITY AIR CONDITIONERS

Refrigeration Basics 101. By: Eric Nelson

Sheet 5:Chapter 5 5 1C Name four physical quantities that are conserved and two quantities that are not conserved during a process.

Chapter 3.4: HVAC & Refrigeration System

How Ground/Water Source Heat Pumps Work

New absorption chillers for high efficient solar cooling systems

NATURAL GAS EXPERIENCE

Industrial Gas Turbines utilization with Associated Gases

Development of a model for the simulation of Organic Rankine Cycles based on group contribution techniques

District heating and district cooling with large centrifugal chiller - heat pumps

APPLIED THERMODYNAMICS. TUTORIAL No.3 GAS TURBINE POWER CYCLES. Revise gas expansions in turbines. Study the Joule cycle with friction.

LNG Storage and Fuel Gas Systems. LNG: Fuel for Shipping, London 15-Feb Carriers & Offshore Units. Jürgen Harperscheidt Sales Manager

AIR CONDITIONING TECHNOLOGY

Typical Cooling Load Profile

POSSIBILITY FOR MECHANICAL VAPOR RE-COMPRESSRION FOR STEAM BASED DRYING PROCESSES

T U R B I N E G A S M E T E R

Environmental and Safety Impacts of HFC Emission Reduction Options for Air Conditioning and Heat Pump Systems

MERCURY REMOVAL FROM NATURAL GAS AND LIQUID STREAMS ABSTRACT. Giacomo Corvini, Julie Stiltner and Keith Clark UOP LLC Houston, Texas, USA

GLOBACON 05 HVAC Systems for Cogen

Evaluation Of Hybrid Air- Cooled Flash/Binary Power Cycle

Commercial refrigeration has been in the environmental. Refrigerant. as a. Basics Considerations PART 1:

Natural Gas. Natural Gas... p. 57 to 59. fin-house f Training... p. 61

Silicagel-water adsorption cooling prototype system for mobile air conditioning

CHAPTER 7 THE SECOND LAW OF THERMODYNAMICS. Blank

2B.1 Chilled-Water Return (and Supply) Temperature B.3 Cooling-Water Supply Temperature / Flow

Daikin Altherma hybrid heat pump. The natural combination

COMMERCIAL HVAC EQUIPMENT. Condensers and Cooling Towers

Dry Gas Seals for LNG Compressors

Natural Gas Dehydrator Optimization

FULL ELECTRICAL LNG PLANTS: HIGHEST AVAILABILITY AND ENERGY EFFICIENCY THROUGH OVERALL SYSTEM DESIGN

HIGH PERFORMANCE CHILLED WATER SYSTEMS. EarthWise HVAC. EarthWise HVAC High Performance CHW Plants

LG Electronics AE Company, Commercial Air Conditioning

Torino Nord. Cogeneration Plant. The gas turbine. The steam generator. The Torino Nord cogeneration plant produces electricity and heat for district

News in Data Center Cooling

HEAT RECOVERY FROM CHILLED WATER SYSTEMS. Applications for Heat Reclaim Chillers

Passing the Baton Cleanly

Building Energy Systems. - HVAC: Heating, Distribution -

Advances in Membrane Materials Provide New Solutions in the Gas Business

LNG BUNKERING LNG AS A SHIP S FUEL GREEN SHIP TECHNOLOGY, OSLO 23-MAR Carriers & Offshore Units. Jürgen Harperscheidt Sales Manager

HIGH-EFFICIENCY CO 2 HEAT PUMP WATER HEATER SYSTEMS FOR RESIDENTIAL AND NON-RESIDENTIAL BUILDINGS

Module 5: Combustion Technology. Lecture 34: Calculation of calorific value of fuels

Advanced Process Integration for Low Grade Heat Recovery

A car air-conditioning system based on an absorption refrigeration cycle using energy from exhaust gas of an internal combustion engine

David Mezzacappa, P.E. SCS Engineers Contractor to U.S. EPA on LMOP

Research on the Air Conditioning Water Heater System

Energy savings in commercial refrigeration. Low pressure control

ADVANCED CONTROL TECHNIQUE OF CENTRIFUGAL COMPRESSOR FOR COMPLEX GAS COMPRESSION PROCESSES

The Second Law of Thermodynamics

DESIGN CHALLENGES AND OPERATIONAL EXPERIENCE OF A MEGA MED SEAWATER DESALINATION PLANT IN TIANJIN

Heat Recovery In Retail Refrigeration

CURBING THE COST OF DATA CENTER COOLING. Charles B. Kensky, PE, LEED AP BD+C, CEA Executive Vice President Bala Consulting Engineers

OUTCOME 2 INTERNAL COMBUSTION ENGINE PERFORMANCE. TUTORIAL No. 5 PERFORMANCE CHARACTERISTICS

Comparison of Spherical and Membrane Large LNG. Carriers in Terms of Cargo Handling

SOLAR-POWERED COOLING, DEHUMIDIFICATION AND AIR CONDITIONING

Transcription:

Liquefaction Process Evaluation for Floating LNG Maya Kusmaya, Trondheim 2014

Outline Introduction Expander processes for natural gas liquefaction Proposed process schemes for FLNG Basis for process evaluation and comparison Result and discussion 2

Introduction Background A challenge to find the optimal liquefaction process technology for use in offshore environment Growing interest to apply expander-based liquefaction processes for FLNG A challenge to get objective comparison between the various technology efficiencies Objective To do a comparative evaluation of several expanderbased processes for FLNG on a identical basis focusing on capacity, efficiency, integration into energy system, complexity, and hydrocarbon inventory Scope of work Literature study, establishment of a identical evaluation basis, HYSYS model development, case studies and systematic comparative analysis of performance data resulted from HYSYS 3

A typical expansion-based liquefaction processes Natural Gas N2 N2 Compressor Natural Gas N2 N2 Cycle Compressor Natural Gas N2 N2 CO2 N2 N2 N2 N2 Warm Compander N2 N2 N2 Compander Flash gas N2 N2 Cold Compander Flash gas N2 N2 Flash gas Natural Gas/LNG Low Pressure N2 Medium Pressure N2 High Pressure N2 LNG Natural Gas/LNG Low Pressure N2 Medium Pressure N2 High Pressure N2 LNG Natural Gas/LNG Low Pressure N2 Medium Pressure N2 High Pressure N2 CO2 refrigerant LNG Single Expansion Double Expansion Double Expansion + Precooling Efficiency and Capacity Improvement 4

The Cooling Curves Single Expansion Double Expansion Double Expansion + Precooling Efficiency and Capacity Improvement 5

Proposed Expander Process Schemes for Floating LNG Process A Based on US Patent 2010/0122551 A1 N2 expander-based process with two pressure levels and three expander temperatures Natural Gas N2 N2 Compressor N2 N2 ARS (LiBr/water) is used for precooling system MCHE The LiBr process driven by gas turbine waste heat and provides cooling of feed gas, N2 loop and gas turbine air intakes. Flash gas SCHE N2 N2 N2 N2 ARS : Absorption Refrigeration System LNG Natural Gas/LNG Nitrogen 6

Proposed Expander Process Schemes for Floating LNG Process B Based on US Patent 5,768,912 a CO 2 precooled dual nitrogen expander liquefaction process the CO2 cooling is also used for gas turbine air intake cooling. 7

Proposed Expander Process Schemes for Floating LNG Process C Process C with precooling Based on US Patent 6,412,302 CH4 Compressor CH4 CH4 CH4 CH4 Compander Natural Gas Flash gas LNG N2 Compressor N2 N2 N2 N2 Compander Natural Gas/LNG Methane Nitrogen 8

Evaluation and Comparison Basis Simulation scope Feed gas Site conditions Drivers Cryogenic HX Component efficiency LNG product The pretreating units are out of the scope Covers the process of the treated feed gas to LNG product Same condition (60 bar, 22 o C) Medium gas (91% of methane) 27 o C of air temperature 17 o C of cooling water temperature 5 o C min temperature approach of cooling water cooled HX GT GE LM6000 At 27 o C air GT gives 35 MW 3 o C min temperature approach 85 bar max pressure Compressor polytropic efficiency of 78% The compander polytropic efficiency was assumed of 73% for the compressor and 83% for the expander Same condition (1.38 bar, -149 o C) At LNG spec 9

Result & Discussion 10

Key Parameter Cycle Process A Process B Basic Process C CO 2 precooled Cycle compression power, MW 35 35 35 35 Precooling power, MW - 1.3-1.4 Precooling heat duty 1, MW 10 - - - Total power, MW 35 36.3 35 36.4 LNG production, MTPA 0.83 0.83 0.82 0.91 Specific power, kwh/ton LNG 336 347 339 315 Compander size the biggest in a single train, MW 9.83 13.23 11.45 8.53 11

LNG Production, MTPA Production and Efficiency Comparison 5.00 4.50 4.00 3.50 3.00 2.50 2.00 1.50 1.00 0.50 0.00 Process A Process B Process C Process C + precool DMR 100% 90% 80% 70% 60% 50% 40% 30% 20% 10% 0% Production (MTPA) Relative process efficiency (%) Note: At the same given power about 140 MW (4 GE LM6000) for liquefaction and precooling cycle 12

Specific power, kwh/ton LNG Specific Power Comparison 360 340 320 300 280 260 240 220 200 Process A Process B Process C Process C + precool DMR 13

Effect of Cooling Water Temperature on Production 110% 100% 90% 80% 70% 60% Low temperature Base case High temperature Process A Process B Process C DMR All processes give higher production at lower temperature with the same given power (more efficient) since less power required for rejecting the heat into a colder sink (ambient) It is influencing more for DMR since the refrigerant condensation pressure depends on cooling water temperature The condensation of refrigerant typically rejects a large part of the energy removed from the natural gas to make LNG thus the variation of the pressure gives significant effect to the power consumption 14

Effect of Cooling Water Temperature on the Relative Production to the DMR 100% Low temperature Base case High temperature 90% 80% 70% 60% Process A Process B Process C DMR Each case was compared to the DMR and represented as a percentage of the corresponding DMR production (100% = production for each DMR case) The difference in production between expanders vs DMR at the same cooling temperature is smaller at high cooling temperature and vice versa. High ambient temperature (e.g. tropical) reduces the advantage of the DMR over the expanders in term of efficiency 15

Cooling Water System Cycle Process A Process B Without precooling Process C With CO 2 precooling DMR Cooling water flow, m 3 /h - For precooling cycle per train - Total per train - Total in a 3 MTPA plant 1710 5,448 21,792 336 4,434 17,736-4,371 17,484 418 4,181 16,724-13,180 13,180 In/Out =17 o C/30 o C A higher specific power of the process give a higher need for CW Process A is the highest as a consequence of introducing a large amount of heat into the precooling (ARS) Process A need a chilled water loop in addition to CW system for the precooling 16

Train Configuration and Equipment Count 17 Cycle Process C Process Process Without With CO A B 2 precooling precooling DMR Number of train per 3 MTPA plant 2 4 4 4 1 The key equipment count per train: - Compressors 6 2 4 4 6 - Pumps 0 0 0 0 1 - Compander 6 2 2 2 - - Heat exchanger (CWHE/PFHE) 4 (2/2) 1 (-/1) 1 (-/1) 1 (-/1) 2 (2/-) - Separators 1 1 2 2 4 - Water cooled exchanger 8 3 6 6 6 Total equipment per train Common precooling: 25 YES 9 YES 15 NO 15 YES 19 NO - Compressors - 2-2 - - Separator - - - 1 - - Heat exchanger - 1-1 - - Water cooled exchanger 6 2-2 - - ARS package (@ 7 MW) 8 - - - - - Chilled water pump (plus back up) 2 - - - - - HRSG unit (additional) 2 - - - - Total equipment per plant 50 + 18 Note: numbers are indicative based on the equipment units shown in the HYSYS simulation and did not consider the size and the duty of the units which may result in several units in parallel in actual plant. 36 + 5 60 60 + 6 19

Complexity The number of equipment units indicates complexity of the facilities. Process A is more complex and Process B is the simplest Even though the DMR has less number of equipment, the DMR is still considered more complex particularly if operational complexity when the plant start up/shut down and or dealing with feed gas condition changes are taken into account 18

Footprint and weight Footprint is a function of equipment count and dimension The actual volume flow indicating how large the suction piping needs to be and it may represent facility dimension Mass and actual volume flow rate of refrigerants into LP compressor inlets: Cycle Process C Process Process Without With CO A B 2 precooling precooling DMR Refrigerant flow, ton/h 1412 1062 706 (C1+N 2 ) 891 (C1 + N 2 ) 2227 Actual volume flow at compressor suction 1 ): Niche processes is the smallest - in m 3 /s 10.5 11.9 8.7 (C1) 6.4 (C1) 25.1 - in m 3 /h 37,800 42,840 31,320 (C1) 23,040 (C1) 90,360 Weight of a topside processing facility is a function of number of equipment, thickness and the material use, including structural material The process with higher number of equipment and operates at higher pressure will be heavier Process A is considered as the heaviest and having the largest footprint 19

Hydrocarbon inventory All the expander-based processes evaluated use of a safe non-flammable refrigerant, i.e. nitrogen, or a minimum use gaseous methane as in Process C The expander-based processes are therefore ideal for FLNG where a small hydrocarbon inventory is preferable from a safety point of view. 20

Motion Except the basic Process C, all the expander based processes subjected to two-phase operation in their precooling system They are all subjected to the vessel motion to some extent. 21

Comparison Summary Criteria Process A Process B Basic Process C Precooled Process efficiency Medium Low Medium High Complexity/Equipment count High Low Medium Medium Footprint High Medium Low Medium Weight High Low Medium Medium Safety High Medium Low Low Sensitivity to motion Medium Medium Low Medium Note: The process, which is considered the most suited for a certain criteria, is highlighted (bold letter) 22

23

FLNG Overview Combining advance technology in land-based LNG and offshore FPSO Used for monetizing stranded offshore natural gas No FLNG currently exist Has different requirement compared to land-based LNG i.e. safety, simplicity, motion, low weight and small footprint (ExxonMobile, 2013) 24

Absorption Refrigeration System 25

Evaluation and Comparison Basis The same set of conditions were applied to the proposed process schemes: Simulation scope Feed gas condition and composition Site conditions (air/cooling water temperature) Drivers (gas turbines) Heat exchanger sizing (min temperature approach) Component efficiency (compressor polytrophic eff.) LNG product condition (i.e. end flash vapor quantity) 26

Simulation scope Fuel gas for GT CO2-free and dried Feed Gas 1 NGL Recovery C5+ NGL/LPG 2 Treated Feed Gas (C5+ and BTX-free) Liquefaction Cycle 1) The pretreating units, i.e. CO 2 removal, dehydration, mercury removal, are out of the scope of the simulation in this study. The feed gas is processed, sweet and dry natural gas coming from the pretreating units at the upstream. 2) NGL/LPG extracted in NGL recovery unit (modeled as turboexpander unit) is fully re-injected into LNG feed stream (assumes that no LPG production and no make up refrigerant required). The NGL/LPG extraction is only for removing BTX components in the feed gas stream. Those aromatic components are assumed to leave the LNG feed stream in the condensate (C5+) product. 3) Lean gas leaving the NGL recovery unit enters into the liquefaction circuit at the same temperature/pressure condition as when it enters the NGL recovery unit (it is recompressed by the booster and cooled by cooling water). 4) The proposed expander-based liquefaction process schemes and the APCI DMR were simulated in this thesis for analysis and comparison. 5) The LNG condition is set to provide constant end flash vapor quantity. The nitrogen content is assumed to be moderate and does not necessitate the implementation of a dedicated nitrogen rejection unit. 3 4 5 LNG 27

Feed Gas Condition Properties Pressure Temperature Feed Gas Stream 60 bar abs 22 o C Composition Component Composition (in %-mole) Nitrogen 1.00 Methane 91.00 Ethane 4.90 Propane 1.70 i-butane 0.35 n-butane 0.40 i-pentane 0.15 n-pentane 0.15 n-hexane 0.13 n-heptane 0.10 n-octane 0.04 n-nonane 0.01 n-decane 0.01 CO 2 0.00 H 2 O 0.00 Benzene 0.03 Toluene 0.02 m-xylene 0.01 28

Cooling Water Temperature The temperature was assumed at 17 o C and it is a closedcircuit cooled by sea water at 14 o C. A 5 o C cooling water cooled exchanger temperature approach was assumed meaning that the compressed refrigerant and feed gas was cooled to 22 o C by using the cooling water. 29

The Driver (Gas Turbine) Gas turbines (GT) used as mechanical driver of main refrigerant compressors and electrical power generation considered are General Electric (GE) LM6000 models ISO rated power (MW) TIT ( o C) Exhaust ( o C) Air flow (kg/s) Pressure ratio Efficiency (%LHV) 42.9 1260 456 124 30 41.7 Air temperature was assumed at 27 oc 30

Heat Exchanger Sizing A minimum temperature approach of 3 o C in the cryogenic heat exchangers was assumed The refrigerant pressure of expander-based processes was limited to 85 bar 31

Component Efficiency Compressors used in the simulation were assumed centrifugal type that has moderate polytropic efficiency of 78% The compander polytropic efficiency was based on GE (Byrne and Mariotti 2010), it was assumed of 73% for the compressor and 83% for the expander 32

Production and Product Quality The intended LNG production is about 3 MTPA with 330 days in a year for the plant availability. LNG product was assumed at -149 o C at the exit of cryogenic heat exchanger and was expanded in end flash column to pressure of 1.38 bar before going to the storage tanks. By this condition, the end flash vapor generated is about 8%-mass of LNG product and nitrogen content is within the LNG specification. It was assumed that the end flash gas from a single expander process train covers fuel needed for a gas turbine LNG Quality Parameters LNG Nitrogen, %-mole < 1 C5+, %-mole < 0.1 BTX, ppm 10 33

HYSYS Model Development Methodology 1. The literature review on the patents and publications of each proposed process scheme was used as basis information for model development 2. Peng-Robinson EOS was used for calculation of thermodynamic properties 3. A steady state mode calculation 4. Optimizing by varying refrigerant flow rate to obtain the selected assumption of minimum approach in LNG heat exchangers. 5. The production was determined based on the given gas turbine power as a mechanical driver for the refrigerant compressors. 6. The key parameters recorded after optimization was LNG production, UA value of LNG heat exchangers, refrigerant flow rates and specific power. 34

DMR process as basis for comparison This is a modification on an established HYSYS model from Statoil, which was adopted by the author during his previous work on the specialization project 35

HYSYS Model Development DMR Process 36

HYSYS Model Development Process A 37

HYSYS Model Development Process B 38

HYSYS Model Development Process C 39

HYSYS Model Development Process C + precooling 40

HYSYS Model Development NGL Extraction Unit 41

Sensitivity Analysis Effect of feed gas composition Effect of treated feed gas pressure Effect of refrigerant pressure Effect of gas turbine intake air cooling Effect of cooling water temperature (heat rejection) 42

LNG production (MTPA) Effect of Feed Gas Composition A study case with lean feed gas was performed Production of all processes drops at the same given power (lower efficiency) The lean gas has a lower condensation temperature i.e. larger temperature lift thus higher work requirement 5.00 4.50 4.00 3.50 3.00 2.50 2.00 1.50 1.00 0.50 0.00 Process A Process B Process C Process C + precool DMR Base Case Production Lean Gas Case Production Drop from base case (%) 96.0% 95.0% 94.0% 93.0% 92.0% 91.0% 90.0% 43

LNG production (MTPA) Effect of Feed Gas Composition (cont.) 5.00 4.50 4.00 3.50 3.00 2.50 2.00 1.50 1.00 0.50 0.00 Base Case Production Lean Gas Case Production Drop from base case (%) 96.0% 95.0% 94.0% 93.0% 92.0% 91.0% 90.0% The process C without precooling tends to suffer more than the other processes (production drops about 9% from its base case) The production drops is due to the feed gas is also the basis for refrigerant in one of the circuits i.e. the methane rich refrigerant circuit. Using a leaner feed gas for the refrigerant increases the specific compression power since the gas has a higher compressibility (z) and a lower molecular weight (M) 44

Production, MTPA Effect of treated feed gas pressure Pressure was varied to the limit that the main HX still withstand How the pressure effects to the efficiency in a T-S diagram For all processes, higher pressure increases the efficiency At higher pressure, the min work and heat load to liquefy the gas is reduced 4.75 4.50 4.25 4.00 3.75 3.50 3.25 3.00 2.75 2.50 60 70 80 90 Pressure, bar DMR Process A Process B Process C 45

Specific power, kwh/ton LNG Effect of refrigerant pressure The refrigerant pressure was limited up to a practical limit of the cryogenic heat exchangers, which is in this study limited to 85 bar 400 380 360 340 320 300 280 260 240 220 200 Process A 55 bar 85 bar Process B 46

Effect of gas turbine intake air cooling Lower air temperature higher gas turbine power output The production capacity for all processes potentially increases over 15% when the precooling system is utilized to cool gas turbine air intake. Cycle Process A Process B Process C+ CO 2 precooling Total power (MW) 4 x 45 4 x 45 1 4 x 45 1 LNG production (MTPA) 4.2 2 4.1 3 4.5 % increased in production 97% 95% 105% Compander size (MW) 12.6 16.3 10.5 47

MW Integration into Energy System Power and Heat Balance (correspond to the Process A only since it requires larger amount of heat to drive its precooling) 250 240 230 220 210 200 190 180 170 160 150 Total heat required Total power required 3.3 3.5 3.7 3.9 LNG Production Heat produced from 6 GTs 48

System Pressure (kpa) COP Effect of Cooling Water Temperature to the ARS system used as Precooling in Process A ater line at the left and crystallization line at the right. A typical cycle and points are shown in Fig. 31. Condenser Refrigerant Solution 8 16 12 11 7 Desorber (generator) 15 3 4 Solution Heat Exchanger 2 5 Throttling Valve Pump Throttling Valve 9 1 6 13 Concentrated Solution Evaporator Absorber Vulnerable to 10 crystallization 18 17 14 Fig. 30. Diagram of single-effect air-cooled absorption chiller 1.00 0.95 0.90 0.85 0.80 0.75 0.70 0.65 0.60 0.55 0.50 20 22 24 26 28 30 Cooling Water temperature ( o C) 15 10 5 2 1 49 The COP of the system is lower at higher cooling water temperature 8 To provide the same amount of cooling duty from this system, increased in heat supply to the system is required. There will be not enough waste heat to provide Crystallization curve that requirement. And at higher cooling water temperature, crystallization of the solution in the ARS is more likely occurs 9 1 6 0.5 0 20 40 60 80 100 120 Tempe tu e C 3 4 Fig. 31. The Dühring P-T chart of absorption cycle

MW Effect of Cooling Water Temperature to the Process A Heat Balance 220 200 180 Total heat requirement Total heat supply 160 140 120 100 10 15 20 25 30 Cooling Water temperature (oc) 50