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Thermodynamic analysis of a water tube boiler operating on
                                                       natural gas with flue gas recirculation and an economiser
                                                          Fraser McGill
                                                          Division of Electronic Engineering, Physics and Renewable Energy, School of Engineering, Physics, and
                                                          Mathematics, University of Dundee, Dundee DD1 4HN, Scotland
  Introduction
  The climate of the planet Earth is changing. To say that the human race is not the only contributor to climate change but that the human race is
  definitely contributing would be a statement that is unanimously accepted. Natural gas is an important fossil fuel with an increasing rate of
  consumption. The increased demand for natural gas is because natural gas burns with less greenhouse gas emissions than other fossil fuels.
  Therefore, through transitions to a more environmentally friendly fuel, natural gas can be the first step.
  As the supply of fossil fuels peak and then reduce, the cost will only ever increase, this coupled with additional climate taxation of fossil fuels will
  drive the market to change their fuel choice or increase their efficiency.

  The idea of thermodynamic analysis has been applied to many combustion related processes with the aim of increasing the efficiency of the fuel use.
  Through an extensive literature search, the thermodynamic analysis of the above named water tube boiler configuration has not currently been
  published, this highlights the individuality of the honours project. The boiler configuration to be analysed is commonly located at industrial
  operations where steam is used as a heat transfer mechanism.


                                                                                    Table 1
                                                            Averaged natural gas composition for Scotland in 2010 [1]
                                                              Carbon                                                                           Neo-         Iso-          N-
                                      %          Nitrogen                    Methane    Ethane       Propane        Iso-butane n-Butane                                                Hexane
                                                              Dioxide                                                                          Pentane      Pentane       Pentane
                                      Average    0.8756       2.4414         88.1825    6.1176       1.7854         0.1772       0.2925        0.00002      0.0467        0.0478       0.0332

                                      Max        1.1468       3.1870         89.4403    7.1864       2.3847         0.2370       0.4362        0.0001       0.0740        0.0776       0.0525

                                      Min        0.7109       1.8239         86.6052    5.3103       1.2087         0.0857       0.1251        0.0000       0.0106        0.0086       0.0037

                                                                                                                                                                                                                                                                              Figure 1
                                                                                                                                                                                                                                                  Boiler tubes, water containing drums and combustion gas path
  Analytical Method
  During a controlled test where the boiler modulation was held at 95%, a ‘snapshot’ of the process variables was captured. The subsequent use of the data began with Psychrometric
  analysis of the combustion air, followed by Stoichiometric combustion analysis specific to the measured gas composition for that day. The initial calculations created the foundation of
  information that allowed for the application of the thermodynamic laws.

  The boiler was deconstructed into manageable control volumes upon which thermodynamic analysis took place, these control volumes are depicted in Figure 2. The analysis used was
  the first law of thermodynamics and the second law of thermodynamics. The second law of thermodynamics allowed for the analysis of Entropy generation in the form of Exergy
  analysis.

  The second law of thermodynamics result can be represented as an Irreversibility per kilogram of steam output or water input and an Irreversibility per kilogram of fuel consumed. Any
  decrease of the Irreversibility will directly translate to an increase in the second law efficiency and indeed the first law efficiency.

                                                                                                                                                                                                                                                         Figure 3
                                                                                                                                                                                                                                 Pressure – Enthalpy diagram for the steam raising process
                                                                                                                                                                                                1000
                  Example of Exergy calculation for substance k relative to reference condition r                                                                                                                                                                                                           ─── Temperature in °C
                                                                                                                                                                                                                                                                                                             ─── Vapour fraction
                                                                                                                                                                                                                                                                                                             ─── Saturated liquid
                                                                                                                                                                                                                                                                                                            ─── Saturated vapour


                            ������������ =                      ������������ ℎ������ − ℎ������ − ������������ ������������ − ������������                                                                                                             100


                                                ������
                                                                                                                                                                                                                                                                                                            Triple point
                                                                                                                                                                                                                                         32.8                                                               Liquid saturation line
                                                                                                                                                                                                                                 33                                                                         21barg saturated liquid
                                                                                                                                                                                                                                                                                                            Feed Pump
                                                                                                                                                                                                                                          20.55
                                                                                                                                                                                                                                                                                                            Economiser
                                                                                                                                                                                                Pressure - bar(a)




                                                                                                                                                                                                                10                                                                                          Economiser to Boiler
                                                                                                                                                                                                                                                                                                            Boiler

Exergy Analysis                                                                                                                                                                                                                                                                                             Vapour saturation line
                                                                                                                                                                                                                                                                                                            Process
The application of exergy analysis consists of using a combined form of the first law and second law of thermodynamics to                                                                                                                                                                                   D/A Feed pump

establish the performance of a system compared to the theoretical reversible limit. The exergy of a substance is the amount                                                                                         1
                                                                                                                                                                                                                                                                                                            D/A

of work which can be produced by the substance as it comes from an energy state that is higher than a reference condition
to an energy state at the reference conditions. Exergy is not subject to conservation laws and it can be described as being
increased or decreased during a process. The further a process veers from the ideal case, the more of a substance’s exergy is
destroyed. Exergy essentially measures how well energy is transformed and it can give an indication of the performance of
the transformation with respect to the ideal case. [2]                                                                                                                                                     0.1
                                                                                                                                                                                                                        0               500          1000       1500       2000               2500   3000         3500                4000
                                                                                                                                                                                                                                                                           Enthalpy - kJ/kg
In the analysis that has been undertaken, the area of greatest interest with respect to exergy analysis is the combustor
control volume (Control volume 2 in Figure 2). The greatest exergy destruction takes place in the combustor control
volume, therefore, developing a slower reaction with more than one stage will improve the exergy efficiency of combustion.                                                                                                                         Future work
                                                                                                                                                                                                                                                   With reference to Figure 3, a future improvement to the steam
                                                                                                                                                                                                                                                   raising process would be to decrease the pressure that the feed
                                                                                                                                                                                                                                                   water is supplied to the boiler as the additional work currently
                                                                                   Figure 2                                                                                                                                                        provided to the water by the pump serves little use. The feed water
                                                                Control volumes for the thermodynamic analysis                                                                                                                                     pressure need only be at a pressure greater than the steam
                                                                                                                                                                                                                                                   generation pressure. The difference could be as small as 1bar but to
                                                                                                                                                                                                                                                   allow for a factor of safety of 3, this could increase to 3bar of a
                     Air intake                            Combustion                            Boiler heat exchange                   Economiser heat exchange                Flue Gas Recirculation takeoff                                     difference. This would create a yearly saving of 67MWh of
                  mAI + mFGR = mCA                        mCA + mF = mPC                                mPC = mBE                                  mBE = mFG                             mFG - mFGR = mSG                                          electricity.
             mAIhAI + mFGRhFGR = mCAhCA               mCAhCA + mFhF = mPAhPA                     mPChPC = mBEhBE – QBHE                   mBEhBE = mFGhFG – QEHE                    mFGhFG - mFGRhFGR = mSGhSG
                                                                                                  QBHE = QSTM + QHTLS-B                        QEHE = QE + QHTLS-E                                                                                 Further refinement of the thermodynamic model could be achieved
                                                                                                                                                                                                                                                   if there were less assumptions, however this would require
     Air In, AI                      Combustion Air, CA                    Products of Combustion, PC                     Boiler Exhaust, BE                         Flue Gas, FG                                       Stack Gas, SG              intrusive measurements of pressure and temperature with the
                                                                                                                                                                                                                                                   combustion chamber and a shift towards a computer based model.
                        1                                        2                                          3                                         4                                     5
                                                                                                                                                                                                                                                   The novel proposal of thermodynamic analysis of a water tube
                                                                                                                                                                                                                                                   boiler operated on natural gas with flue gas recirculation and an
                                                                                                                                                                                                                                                   economiser is a complicated scenario compounded by daily
                                                                                                                                                                                                                                                   variation in it’s operating conditions. The variables of the operating
                            Flue Gas Recirculation,                  Fuel, F                Steam, STM
                                                                                                                                                             Economiser in,                     Flue Gas Recirculation,                            conditions would constantly create a unique conclusion if the
                                                                                                                     Economiser out, E-OUT                   E-IN                               FGR
                            FGR                                                                                                                                                                                                                    analysis were performed with a timescale of days to weeks. Any
                                                                                                                                                                                                                                                   stable model yielding a replicable result would be required to
                                                                                                                                                                                                                                                   ascertain large data sets over a timescale of months to years. Such a
                                                                                                   Steam generation                              Feedwater preheating                                                                              data set and timescale lends itself well to computer based
                                                                                                  mE-OUT = mSTM - mBLD                               mE-IN = mE-OUT                                                                                modelling.
                                                                                       mSTMhSTM = mE-OUThE-OUT - mBLDhBLD + QSTM           mE-INhE-IN = mE-OUThE-OUT + QEHE




Acknowledgements
Supervisor: Dr R.A. Gibson
Special thanks are extended to Gerry Bannister of Michelin Tyre Company
                                                                                                                                                                                     References
                                                                                                                                                                                     [1] National Grid daily calorific values (2010).
                                                                                                                                                                                     [2] M.A. Rosen, I.Dincer, M.Kanoglu Energy Policy. 36, 128-137 (2008).

Degree Programme: BSci Renewable Energy

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Thermodynamic analysis of a water tube boiler operating on natural gas with flue gas recirculation and an economiser

  • 1. Thermodynamic analysis of a water tube boiler operating on natural gas with flue gas recirculation and an economiser Fraser McGill Division of Electronic Engineering, Physics and Renewable Energy, School of Engineering, Physics, and Mathematics, University of Dundee, Dundee DD1 4HN, Scotland Introduction The climate of the planet Earth is changing. To say that the human race is not the only contributor to climate change but that the human race is definitely contributing would be a statement that is unanimously accepted. Natural gas is an important fossil fuel with an increasing rate of consumption. The increased demand for natural gas is because natural gas burns with less greenhouse gas emissions than other fossil fuels. Therefore, through transitions to a more environmentally friendly fuel, natural gas can be the first step. As the supply of fossil fuels peak and then reduce, the cost will only ever increase, this coupled with additional climate taxation of fossil fuels will drive the market to change their fuel choice or increase their efficiency. The idea of thermodynamic analysis has been applied to many combustion related processes with the aim of increasing the efficiency of the fuel use. Through an extensive literature search, the thermodynamic analysis of the above named water tube boiler configuration has not currently been published, this highlights the individuality of the honours project. The boiler configuration to be analysed is commonly located at industrial operations where steam is used as a heat transfer mechanism. Table 1 Averaged natural gas composition for Scotland in 2010 [1] Carbon Neo- Iso- N- % Nitrogen Methane Ethane Propane Iso-butane n-Butane Hexane Dioxide Pentane Pentane Pentane Average 0.8756 2.4414 88.1825 6.1176 1.7854 0.1772 0.2925 0.00002 0.0467 0.0478 0.0332 Max 1.1468 3.1870 89.4403 7.1864 2.3847 0.2370 0.4362 0.0001 0.0740 0.0776 0.0525 Min 0.7109 1.8239 86.6052 5.3103 1.2087 0.0857 0.1251 0.0000 0.0106 0.0086 0.0037 Figure 1 Boiler tubes, water containing drums and combustion gas path Analytical Method During a controlled test where the boiler modulation was held at 95%, a ‘snapshot’ of the process variables was captured. The subsequent use of the data began with Psychrometric analysis of the combustion air, followed by Stoichiometric combustion analysis specific to the measured gas composition for that day. The initial calculations created the foundation of information that allowed for the application of the thermodynamic laws. The boiler was deconstructed into manageable control volumes upon which thermodynamic analysis took place, these control volumes are depicted in Figure 2. The analysis used was the first law of thermodynamics and the second law of thermodynamics. The second law of thermodynamics allowed for the analysis of Entropy generation in the form of Exergy analysis. The second law of thermodynamics result can be represented as an Irreversibility per kilogram of steam output or water input and an Irreversibility per kilogram of fuel consumed. Any decrease of the Irreversibility will directly translate to an increase in the second law efficiency and indeed the first law efficiency. Figure 3 Pressure – Enthalpy diagram for the steam raising process 1000 Example of Exergy calculation for substance k relative to reference condition r ─── Temperature in °C ─── Vapour fraction ─── Saturated liquid ─── Saturated vapour ������������ = ������������ ℎ������ − ℎ������ − ������������ ������������ − ������������ 100 ������ Triple point 32.8 Liquid saturation line 33 21barg saturated liquid Feed Pump 20.55 Economiser Pressure - bar(a) 10 Economiser to Boiler Boiler Exergy Analysis Vapour saturation line Process The application of exergy analysis consists of using a combined form of the first law and second law of thermodynamics to D/A Feed pump establish the performance of a system compared to the theoretical reversible limit. The exergy of a substance is the amount 1 D/A of work which can be produced by the substance as it comes from an energy state that is higher than a reference condition to an energy state at the reference conditions. Exergy is not subject to conservation laws and it can be described as being increased or decreased during a process. The further a process veers from the ideal case, the more of a substance’s exergy is destroyed. Exergy essentially measures how well energy is transformed and it can give an indication of the performance of the transformation with respect to the ideal case. [2] 0.1 0 500 1000 1500 2000 2500 3000 3500 4000 Enthalpy - kJ/kg In the analysis that has been undertaken, the area of greatest interest with respect to exergy analysis is the combustor control volume (Control volume 2 in Figure 2). The greatest exergy destruction takes place in the combustor control volume, therefore, developing a slower reaction with more than one stage will improve the exergy efficiency of combustion. Future work With reference to Figure 3, a future improvement to the steam raising process would be to decrease the pressure that the feed water is supplied to the boiler as the additional work currently Figure 2 provided to the water by the pump serves little use. The feed water Control volumes for the thermodynamic analysis pressure need only be at a pressure greater than the steam generation pressure. The difference could be as small as 1bar but to allow for a factor of safety of 3, this could increase to 3bar of a Air intake Combustion Boiler heat exchange Economiser heat exchange Flue Gas Recirculation takeoff difference. This would create a yearly saving of 67MWh of mAI + mFGR = mCA mCA + mF = mPC mPC = mBE mBE = mFG mFG - mFGR = mSG electricity. mAIhAI + mFGRhFGR = mCAhCA mCAhCA + mFhF = mPAhPA mPChPC = mBEhBE – QBHE mBEhBE = mFGhFG – QEHE mFGhFG - mFGRhFGR = mSGhSG QBHE = QSTM + QHTLS-B QEHE = QE + QHTLS-E Further refinement of the thermodynamic model could be achieved if there were less assumptions, however this would require Air In, AI Combustion Air, CA Products of Combustion, PC Boiler Exhaust, BE Flue Gas, FG Stack Gas, SG intrusive measurements of pressure and temperature with the combustion chamber and a shift towards a computer based model. 1 2 3 4 5 The novel proposal of thermodynamic analysis of a water tube boiler operated on natural gas with flue gas recirculation and an economiser is a complicated scenario compounded by daily variation in it’s operating conditions. The variables of the operating Flue Gas Recirculation, Fuel, F Steam, STM Economiser in, Flue Gas Recirculation, conditions would constantly create a unique conclusion if the Economiser out, E-OUT E-IN FGR FGR analysis were performed with a timescale of days to weeks. Any stable model yielding a replicable result would be required to ascertain large data sets over a timescale of months to years. Such a Steam generation Feedwater preheating data set and timescale lends itself well to computer based mE-OUT = mSTM - mBLD mE-IN = mE-OUT modelling. mSTMhSTM = mE-OUThE-OUT - mBLDhBLD + QSTM mE-INhE-IN = mE-OUThE-OUT + QEHE Acknowledgements Supervisor: Dr R.A. Gibson Special thanks are extended to Gerry Bannister of Michelin Tyre Company References [1] National Grid daily calorific values (2010). [2] M.A. Rosen, I.Dincer, M.Kanoglu Energy Policy. 36, 128-137 (2008). Degree Programme: BSci Renewable Energy