1 SE/P3-39 Nuclear Fusion as New Energy Option in a Global Single-Regional Energy System Model C. Eherer 1), M. Baumann 1), J. Düweke 2), T. Hamacher 2) 1) Institute for Theoretical and Computational Physics (ITP), Graz University of Technology, Austria 2) Max Planck Institute for Plasma Physics (IPP), Garching, Germany e-mail contact of main author: [email protected] Abstract. Is there a window of opportunity for fusion on the electricity market under “business as usual” conditions, and if not, how do the boundary conditions have to look like to open such a window? This question is addressed within a subtask of the Socio-Economic Research on Fusion (SERF) programme of the European Commission. The most advanced energy-modelling framework, the TIMES model generator developed by the Energy Technology System Analysis Project group of the IEA (ETSAP) has been used to implement a global single-regional partial equilibrium energy model. Within the current activities the potential role of fusion power in various future energy scenarios is studied. The final energy demand projections of the baseline of the investigations are based on IIASA-WEC Scenario B. Under the quite conservative baseline assumptions fusion only enters the model solution with 35 GW in 2100 and it can be observed that coal technologies dominate electricity production in 2100. Scenario variations show that the role of fusion power is strongly affected by the availability of GEN IV fission breeding technologies as energy option and by CO2 emission caps. The former appear to be a major competitor of fusion power while the latter open a window of opportunity for fusion power on the electricity market. An interesting outcome is furthermore that the possible share of fusion electricity is more sensitive to the potential of primary resources like coal, gas and uranium, than to the share of solar and wind power in the system. This indicates that both kinds of technologies, renewables and fusion power, can coexist in future energy systems in case of CO2 emission policies and/or resource scarcity scenarios. It is shown that Endogenous Technological Learning (ETL), a more consistent description of technological progress than mere time series, has an impact on the model results. 1. Introduction Facing the expected growth in energy demand on a global scale during the next decades, whereby especially fast growing economies in the non-OECD part of the world (e.g. China) will have an impact on the situation, the investigation of the technical and economic potential of new energy supply technologies in possible future energy systems is of high interest. Nuclear fusion is one of the promising new energy supply technologies due to its safe operation, nearly inexhaustible resources and its potential for a CO2 emission free production of base load electricity. Fusion reactors are expected to be commercially available for power generation about the middle of the century. Due to their large unit size, they will initially serve as base load option for electricity production. The site for the fusion experiment ITER, which is the next step in fusion research and which might bring the proof of principle for nuclear fusion, is currently under decision. Within a subtask of the Socio-Economic Research on Fusion (SERF) programme of the European Commission the central goal is to identify, whether there is a window of opportunity for fusion on the electricity market under “business as usual” conditions, and if not, how the boundary conditions have to look like to open such a window [1]. The most advanced energy-modelling framework, the TIMES model generator developed by the Energy Technology System Analysis Project group of the IEA (ETSAP, [2]) has been used to implement a global single-regional partial equilibrium energy model at the IPP Garching in co-operation with the ITP Graz [3]. 2 SE/P3-39 Within an EFDA-SERF project task, the ITP Graz studies the potential role of fusion power in a future energy system. The work is done in co-operation with the IPP Garching and is mainly focused on long-term scenario analyses until 2100 with special attention to nuclear fusion and its most likely long-term competitors. Scenarios comprise possible development paths of major driving forces of an energy system. They can be seen as story lines formulated by the modeller or by stakeholders to assess e.g. the impact of energy policies [4]. 2. Methodology 2.1. The TIMES Model Generator The main tool to carry out the present system studies is the “The Integrated MARKAL EFOM System” (TIMES), which is the latest energy modelling framework developed by the Energy Technology System Analysis Project group of the IEA (ETSAP). TIMES is a so called model generator. The modeller provides information about the structure of the energy system, the energy technologies and all the required technical and economic data. Out of these information TIMES generates an economic partial equilibrium model of the energy system in terms of a mathematical programme. In the solution of a TIMES model the quantities and prices of the various commodities of the energy system are in equilibrium, i.e. their prices and quantities in each time period are such that at those prices the suppliers produce exactly the quantities demanded by the consumers [5]. This equilibrium is present at every stage of the energy system from primary energy forms to final energy demands. In reality, demands will reduce or increase compared to a reference case, when prices rise and fall, respectively. TIMES offers the feature to make energy demands price sensitive, by assigning elasticities to them. The demands can thus selfadjust within a certain bandwidth endogenously within the model, allowing a bona fide supply-demand equilibrium. Due to elastic demands, the energy model has the chance to balance welfare losses caused by a more expensive electricity mix with welfare losses caused by demand reductions, leading to an optimal distribution of the two with respect to the net total surplus of the system. In a TIMES model energy technologies are explicitly modelled in detail in terms of technological and economic data, which is a bottom-up description of the energy system. The scope of TIMES models is beyond purely energy related issues. The representation of materials and environmental emissions related to the energy system is possible. Thanks to the explicitness of the representation of technologies and fuels, a TIMES model can be constructed to analyse energy-environmental policies. The energy system in a TIMES model is depicted by flows of energy carriers through energy technologies, modelled by the concept of a Reference Energy System (RES). Energy, material flows and emissions are described by commodities, which are transformed by processes into each other. In this way, the whole path from primary energy to final energy or even energy services can be modelled. TIMES offers a number of advanced modelling features for a sophisticated representation of the energy system (e.g. variable model period lengths, flexible time slices and storage processes, accurate and realistic depiction of cost payments and investments, flexible processes, Endogenous Technological Learning, data decoupled from period definition, age dependent parameters, vintaging, multiple model regions linked by inter-regional trade) [6], [7], [8]. SE/P3-39 3 FIG. I. STRUCTURE OF THE TUG-IPP MODEL. 2.2 The TUG-IPP Global Energy Model The developed global model depicts the energy system starting from extraction of primary energy carriers over conversion, refining and distribution to the various end-use sectors demanding final energy. In addition, a simplified description of the transport sector is included. At the moment, the focus of the model structure lies on the supply side (especially electricity production), while the demand side is viewed at in an aggregated way. Although, the model is single-regional at the present state, the energy demands are split into OECD and non-OECD due to the expected differences in development in these two world regions. Figure I gives an overview of the structure of the TUG-IPP model. The time horizon of the model is the long-term future. It reaches from 1990 to 2100, divided into 12 model periods of 10 years length each. The resolution is annual, no seasonal or even smaller time divisions are made. Past investments existing prior to the model time horizon are accounted for. The set of electricity and central heat production technologies includes a variety of present and future technology types: nuclear fusion power (HCLL, Model AB, [9]), nuclear fission power, coal and gas plants, CO2 sequestrating technologies, hydro power, solar thermal power, photovoltaics, on- and offshore wind turbines, geothermal power from hard dry rock and aquifers, biomass and biogas plants, fuel cell plants. To achieve a more realistic representation of technological diffusion and growth, dynamic growth constraints are being used. Such constraints link the development of a technology in one period with its status in the previous period. In reality, the growth of a technology is dependent on its former development. So, by the use of dynamic growth constraints unrealistic effects (e.g. the taking over of the whole market in one single period, or the alternating use of two technologies) can be prevented, leading to smoother transitions from one technology to another one and smoother transitions between periods. 4 SE/P3-39 3. Baseline Scenario An energy scenario consists of a set of coherent assumptions about future trajectories of the drivers of an energy system. It describes a possible way in which the future may enfold [4]. Long-term energy models like the TUG-IPP model are explorative tools for the investigation of such possible futures based on contrasted scenarios. In a TIMES model, a scenario consists of different types of inputs: energy demands, primary resource potentials (e.g. coal and lignite, natural gas, crude oil, uranium), a policy setting, and the description of a set of technologies [5]. In the baseline scenario of the TUG-IPP model the final energy demands are based on the projections of IIASA-WEC Scenario B, which are characterised by moderate growth [4]. Recent numbers for primary resource potentials were included ([10], [11], [12], [13], [14]) and the maximum share of electricity generated by wind and solar power was given an upper limit of 30%. In the baseline no policies like emission caps or taxes are assumed and no GEN IV nuclear fission breeding technologies are available. Commercial fusion power plants are assumed to be available in the mid of the century. For investments a discount rate of 5% has been chosen for all model periods. Figure II shows the results for the electricity production mix in the baseline scenario. One can observe that coal technologies without CO2 sequestration dominate electricity production in 2100 (47%). Nuclear fission contributes quite a lot to the electricity mix (up to 33% in 2060). It starts declining about 2070 due to ongoing depletion of the uranium resources available in the baseline. Gas turbines and fuel cells satisfy the peak load demand for electricity (ca. 20% of the demand). Solar power, wind turbines, biomass plants and hydro power produce together 24% of the electricity in 2100, while fission accounts for only 7% of the production. Nevertheless, without any emission policies, the chosen development path favours inexpensive electricity from coal. In the described setting of the baseline, which is chosen quite conservative, fusion power cannot compete as base load option with coal and nuclear power and enters the global energy mix with only 35 GW in 2100. 4. Scenario Variations To investigate the influence of different boundary conditions on the potential of fusion power a number of scenario variations have been carried out and analysed. Compared to the baseline all combinations of the following scenario assumptions have been tested: different cumulative CO2 emission constraints leading to a certain long-term stabilisation level [15], an upper limit on the cumulative amount of CO2 sequestration, different upper limits on the maximum share of solar and wind power, different potentials of primary resources, existence of nuclear fission breeding technologies (Table I). For the analysis of key boundary conditions the total electricity produced from fusion power plants has been compared to the total cumulative production over the whole model horizon. The observations derived from the results of all possible scenario variations (in total 72 variations) can be summarised as follows. SE/P3-39 5 Generated electricity by fuel - baseline 80,000.00 Other 70,000.00 Wind Solar 60,000.00 Electricity [TWh] Hydro Fission 50,000.00 Existing LWR Biomass 40,000.00 Fuel cell Gas + Seq. 30,000.00 Gas Fusion 20,000.00 Coal + Seq. Coal + Lig. 10,000.00 Existing 1990 2000 2010 2020 2030 2040 2050 2060 2070 2080 2090 2100 Model period FIG. II. ELECTRICITY PRODUCTION BY FUEL IN THE BASELINE. TABLE I: SCENARIO VARIATIONS. Assumption Cumulative CO2 emission constraints Maximum amount of cumulative sequestrated CO2 Maximum share of electricity from wind and solar power Amount of primary resources GEN IV Nuclear fission breeding technology Variations 450 ppm / 550ppm / no limit 300 Giga tonnes carbon / no limit 30% / 60% 65% / 100% / 200% (of baseline) yes / no If nuclear fission breeding technologies are available as energy option (at 30% higher investment cost, 50% higher operation and maintenance cost and 100% higher activity costs than LWRs [16]), nuclear fusion power does not enter the electricity mix in any of the scenarios. In the cases where breeder reactors are not available, fusion power can get a market share in 32 of 36 cases. In 24 of these 32 cases CO2 emission constraints are present, confirming the expected impact of emission policies on the role of fusion power. The amount of fusion power is also dependent on the amount of primary resources and the maximum shares of wind and solar power, while the limit on cumulative sequestrated CO2 has no impact. Furthermore, it can be seen, that the amount of resources has a higher impact on the share of fusion power than an imposed upper limit on the share of wind and solar power. The maximum share of cumulative electricity production that can be reached by fusion power in scenarios without fission breeding technologies is 14.3%. Figure III shows the results for generated electricity in case of an energy scenario containing cumulative CO2 emission constraints leading to a long-term stabilisation level of 550 ppm [15]. Furthermore, it is assumed that no GEN IV breeders are available and high shares of solar and wind power (60%) are allowed. In this scenario fusion power can get a considerable market share of 9.6% of the cumulative electricity production over the model time horizon. Fission fades out due to depletion of uranium. SE/P3-39 6 Fusion Energy Scenario - Generated electricity by fuel 550ppm, unlimited sequestration, up to 60% wind and solar, no GEN IV fission breeder 80,000.00 Other 70,000.00 Wind Solar Electricity [TWh] 60,000.00 Hydro Fission 50,000.00 Existing LWR Biomass 40,000.00 Fuel cell Gas + Seq. 30,000.00 Gas Fusion 20,000.00 Coal + Seq. Coal + Lig. 10,000.00 Existing 1990 2000 2010 2020 2030 2040 2050 2060 2070 2080 2090 2100 Model period FIG. III. ENERGY SCENARIO WITH CO2 EMISSION CONSTRAINTS. In 2100 fusion power (31%) and coal technologies with CO2 sequestration (9%) account for 40% of electricity production. Hydro, solar, wind and geothermal power take 40% of the market. The demanded peak load (20%) is produced by heron turbine fuel cell plants. 5. Impact of Endogenous Technological Learning (ETL) In long-term energy models, one of the important issues is to describe the future development of the technological progress. Among the parameters that are important for the characterisation of a technology are the specific investment costs [17]. Some years ago, in energy models the cost development was considered as being a function of time, i.e. a technology becomes cheaper with elapsing time, also if it is not used. The progress of a technology was an exogenous assumption, though based on historic experiences. This sometimes led to unreasonable results, especially in perfect foresight models. In these models, a technology was chosen because of its competitive price in model periods at the end of the time horizon, without being in use before. Historical experience has shown that the progress of a technology is related to the knowledge accumulated through the construction or use of this technology [18], [19]. Thus, it has become more common to treat the technological progress of a technology in an energy system model in an endogenous way. In the TIMES model generator technological learning is endogenised by linking the specific investment costs of a technology to its cumulative installed capacity via the Experience Curve concept [20], [21]. This feature has been applied to the electricity producing technologies and the impact on the baseline and selected scenarios was investigated. To study the impact of ETL on the scenario results, three different scenarios were analysed, the baseline scenario and two scenarios with a considerable share of electricity generated by fusion power. The results show that the endogenous description of the specific cost development has a significant impact. The main benefit is gained by technologies based on solar power, especially PV cells which can enter already the baseline scenario with a high market share (in terms of generated electricity). Also wind power and biomass plants can increase their market share. In all scenarios, the total amount of generated electricity increased, and the cost of electricity decreased. 7 SE/P3-39 The increased electricity production of these technologies compensates the production by some other technologies. Coal power plants have the biggest decrease in production, but also the production of fusion power plants declines. For example, the small share of fusion in the baseline scenario vanishes completely. In the case of high CO2 emission constraints (450 ppm), the share of cumulative fusion power drops from 12% to 9%, whereas the in case of 550 ppm it drops from 10% to only 3%. Nevertheless, a major drawback of ETL is the tremendous increase of computer resources if one wants to include more than a few (5-10) learning technologies in an energy model. This is also the reason, why at the moment not all 72 scenario variations presented in section 4 could be investigated with ETL. 6. Conclusion/Outlook Under the quite conservative baseline assumptions fusion only marginally enters the model solution in 2100 (35 GW) and it can be observed that coal and gas technologies account for a large part of the electricity production in 2100. Scenario variations show that the role of fusion power is strongly affected by the availability of GEN IV fission breeding technologies as energy option and by CO2 emission caps. The former appear to be a major competitor of fusion power while the latter open a window of opportunity for fusion power on the electricity market. An interesting outcome is furthermore that the possible share of fusion electricity is more sensitive to the potential of primary resources like coal, gas and uranium, than to the share of solar and wind power in the system. This indicates that both kinds of technologies, renewables and fusion power, can coexist in future energy systems in case of CO2 emission policies and/or resource scarcity scenarios. For instance, in case of CO2 emission constraints leading to a long-term stabilisation level of 550 ppm in the atmosphere, fusion power is able to produce 31% of the electricity in 2100, while another 40% are produced by solar, wind, hydro and geothermal power. It was shown that Endogenous Technological Learning (ETL), a more consistent description of technological progress than mere time series, can have an impact on the model results. The application of ETL imposes high needs on computer resources, even in case of just a few learning technologies, thus at the moment its application is limited. In the next phase of the activities, more in depth analyses and informative results will be obtained making use of the new long-term 15-regions global energy model, which was developed under EFDA contract and has been released in October 2004 [5], [22]. The TUGIPP model will be used and maintained further for quick checks, comparisons and exploration of modelling features that are only applicable in smaller models because of computer resources. 7. Acknowledgements Besides the Austrian EURATOM Association and EFDA, we especially would like to thank the Friedrich Schiedel Foundation for Energy Technology and the Austrian Ministry of Science (BM:BWK) for their significant support of this research project. 8. Disclaimer This work, supported by the European Communities under the Contract of Association between EURATOM and the Austrian Academy of Sciences, was carried out within the SE/P3-39 8 framework of the European Fusion Development Agreement. The views and opinions expressed herein do not necessarily reflect those of the European Commission. Appendix 1: References [1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] [19] [20] [21] [22] EFDA-STAC, Fusion Technology work programme 2005, 2004. ETSAP homepage, http://www.etsap.org, referenced in November 2004. Eherer, C., Baumann, M., Long-Term Technology Based Modelling with TIMES, Interim Report, EFDA/SERF sub task TW3-TWE-FESA/A, Garching, June 2004 Nakicenovic, N., Grübler, A., and McDonald A., Global Energy Perspectives, Cambridge University Press, Cambridge, UK, 1998. Haurie, A., Kanudia, A., Loulou, R., van Regemorter, D., and Vaillantcourt, K., The EFDA World Model. Draft Final Report prepared for EFDA, ORDECSYS, HALOA/KANORS and KUL, 2004. TIMES, The "New" ETSAP E3 MODEL System Documentation, Working Paper, The IEA-ETSAP TIMES Working Group, 2000. Mäkelä, J., Development of an Energy System Model of the Nordic Electricity Production System, Master Thesis, Helsinki, 2000. Eherer, Ch., Fusion as a new energy technology in a long-term TIMES model of the energy system, Friedrich Schiedel project, project report, Graz-Garching, 2004. Ward, D.J., Baumann, M., Report on the first assessment of an HCLL plant model, Culham, March 2004. BGR, Reserven, Ressourcen und Verfügbarkeit von Energierohstoffen 2002, Rohstoffwirtschaftliche Länderstudien Heft XXVIII, Bundesanstalt für Geowissenschaften und Rohstoffe, Hannover 2003. Erdmann, G., Wirtschaftliche Vorraussetzung der energetischen Nutzung von Biomasse, TU Berlin, 1998. Fischer, G., Schrattenholzer, L., Global Bioenergy Potentials through 2050, Biomass & Bioenergy 20, pages 151-159, 2001. Kaltschmitt, M, Hartmann, H., Energie aus Biomasse – Grundlagen, Techniken, Verfahren, Springer Verlag, Berlin-Heidelberg, 2001. Lako, P., Eder, H., de Noord, M., Reisinger, H., Hydropower Development with a Focus on Asia and Western Europe, Overview in the framework VLEEM 2, ECN report C—03-027, Netherlands, 2003. IPCC, Special Report on Emissions Scenarios, Nakicenovic and Swart (eds)., Cambridge University Press, 2000. Mooz, W.E., Siegel, S., A Comparison of the Capital Costs of Light Water Reactor and Liquid Metal Fast Breeder Reactor Power Plants, Prepared for the U.S. Arms Control and Disarmament Agency, R-2441-ACDA, The Rand Corporation, 1979. Bareto, L., Technological Learning In Energy Optimisation Models And Deployment Of Emerging Technologies, Dissertation, ETH Zürich, 2001. Dutton, J., Thomas, A., Academy of Management Review – Treating Progress Functions as a Managerial Opportunity, Academy of Management Review Vol. 9, No.2, 235-247, 1984. Argote, L., Epple, D., Learning Curves in Manufacturing, Science Vol. 247, Febr. 1990. Wene, C., Experience Curves for Energy Technology Policy, IEA, Paris, 2000. Neij, L., et.al., Experience Curves - A Tool for Energy Policy Assessment, Lund, 2003. Lechon, Y., Cabal, H., Varela, M., Saez, R., Eherer, C., Baumann, M., Düweke, J., Hamacher, T., Tosato, G.C., A Global Energy Model with Fusion, contribution submitted to the SOFT conference, Venice, Italy, 2004. Nuclear Fusion as a New Energy Option in a Global SingleRegional Energy System Model C. Eherer1, M. Baumann1, J. Düweke2, T. Hamacher2 1 Institute for Theoretical and Computational Physics (ITP), Graz University of Technology, Petersgasse 16/II, 8010 Graz, Austria 2 Max Planck Institute for Plasma Physics (IPP), Boltzmannstr. 2, 85748 Garching, Germany Introduction Introduction Baseline Baseline Scenario Scenario (cont.) (cont.) Socio-Economic Socio-Economic Research Research on on Fusion Fusion (EFDA) (EFDA) Investigation Investigation of of potential potential role role of of fusion fusion power power in in future future energy energy scenarios scenarios Identifying Identifying boundary boundary conditions conditions for for fusion fusion 900.00 Consistent Consistent description description of of specific specific cost cost development development 800.00 700.00 Transport fuels Final energy [EJ] 600.00 Methodology Methodology Endogenous Endogenous Technological Technological Learning (ETL) Learning (ETL) Final energy demands - baseline Generated electricity by fuel - with ETL - baseline Residential electricity Residential heat 500.00 80,000.00 Commercial electricity 400.00 Commercial heat Other 70,000.00 Industrial electricty 300.00 Wind Industrial heat Solar 60,000.00 200.00 Electricity [TWh] Hydro 1990 2000 2010 2020 2030 2040 2050 2060 2070 2080 2090 2100 Model period Fission 50,000.00 Existing LWR Biomass 40,000.00 Fuel cell Gas + Seq. 30,000.00 Gas Fusion 20,000.00 Coal + Seq. Coal + Lig. Primary energy - baseline 10,000.00 1,600.00 Existing 1990 1,400.00 2000 2010 2020 2030 2040 2050 2060 2070 2080 2090 2100 Model period Wind energy Uranium 1,200.00 Solar energy Natural gas 1,000.00 Energy [EJ] The The Integrated Integrated MARKAL MARKAL EFOM EFOM System System (TIMES) (TIMES) Energy Energy Technology Technology System System Analysis Analysis Project Project (ETSAP) (ETSAP) of of the the IEA IEA Model Model generator generator Partial Partial equilibrium equilibrium (supply-demand) (supply-demand) Total Total surplus surplus maximisation maximisation Multi-period, Multi-period, perfect perfect foresight foresight Technology-rich Technology-rich bottom-up bottom-up description description of of the the energy energy system system Energy flows, materials, emissions Energy flows, materials, emissions Analysis Analysis of of energy-environmental energy-environmental policies policies Advanced Advanced features features 100.00 Fusion Scenario 1 - Generated electricity by fuel - with ETL Lignite Hydro energy 80,000.00 Coal 800.00 Geoth. heat (deep) Other 70,000.00 Geoth. heat (aquifer) 600.00 Wind Deuterium + Lithium ¾ ¾ Price Price sensitive sensitive demands demands ¾ ¾ Flexible Flexible technology technologydescription description ¾ ¾ Endogenous EndogenousTechnological TechnologicalLearning Learning Solar 60,000.00 Crude oil 400.00 Hydro Biomass (wood + res.) 200.00 1990 2000 2010 2020 2030 2040 2050 2060 2070 2080 2090 2100 Model period Electricity [TWh] Biomass (energy crops) Fission 50,000.00 Existing LWR Biomass 40,000.00 Fuel cell Gas + Seq. 30,000.00 Gas Fusion 20,000.00 The -IPP Model TUG The TUGTUG-IPP Model 2030 2040 2050 2060 2070 2080 2090 2100 Model period Hydro ¾ ¾ Split: Split:OECD, OECD,Non-OECD Non-OECD Biomass 80,000.00 Fuel cell Gas + Seq. 30,000.00 Wind om .E lc om . .H ea t d. Elc . In d. H e R e at s. Elc . R es .H Tra eat ns po rt 1990 2000 2010 2020 2030 2040 2050 2060 2070 2080 2090 2100 Model period Fusion Fusion in in Energy Energy Scenarios Scenarios Fusion Scenario 1 - Generated electricity by fuel 450ppm, unlimited sequestration, up to 60% wind and solar, no GEN IV fission breeder 90,000.00 CO2 Other 80,000.00 Wind Transport 70,000.00 Solar Electricity [TWh] Hydro 60,000.00 Fission Existing LWR 50,000.00 Biomass Fuel cell 40,000.00 Gas + Seq. Gas 30,000.00 Fusion 20,000.00 Coal + Seq. Coal + Lig. Final energy demands for OECD and Non-OECD 10,000.00 Existing 1990 2000 2010 2020 2030 2040 2050 2060 2070 2080 2090 2100 Model period Baseline Baseline Scenario Scenario Conservative Conservative assumptions assumptions on on potential potential of of wind wind and and solar solar power power (30% (30% of of generated generated electricity) electricity) Dynamic Dynamic growth growth constraints constraints for for all all sectors sectors emission caps caps and/or and/or taxes taxes No No CO CO22 emission Discount Discount rate: rate: 5% 5% Fusion Scenario 2 - Generated electricity by fuel 550ppm, unlimited sequestration, up to 60% wind and solar, no GEN IV fission breeder 80,000.00 Other 70,000.00 Wind Solar 60,000.00 Electricity [TWh] ¾ ¾ Geothermal, Geothermal,biomass, biomass,hydropower hydropower Gas + Seq. Gas Coal + Seq. Existing 1990 2000 2010 2020 2030 2040 2050 2060 2070 2080 2090 2100 Model period Share Shareof of cumulative cumulativefusion fusionpower: power: CO2 Based Based on on IIASA-WEC IIASA-WEC Scenario Scenario BB final final energy energy projections projections Resource Resource constraints constraints (fossils, (fossils, uranium) uranium) Limited Limited potentials potentials according according to to literature literature Fuel cell Coal + Lig. Electricity & Heat Production Demand side Biomass 30,000.00 Fusion ¾¾ Scenario Scenario1: 1:13.7% 13.7%(from (from1990 1990on), on),19.6% 19.6%(from (from2050 2050on) on) ¾¾ Scenario Scenario2: 2:9.6% 9.6%(from (from1990 1990on), on),13.6% 13.6%(from (from2050 2050on) on) Sectoral Heating Existing LWR 40,000.00 10,000.00 Grids CO2 Fission 50,000.00 20,000.00 Sectoral Elc. Dem. Electrolysis Hydro Electricity [TWh] Existing Solar 60,000.00 Coal + Seq. 10,000.00 CO2 Refining & Conversion Other 70,000.00 Gas Coal + Lig. In C C ic ity He Ele at ctr icit y t ctr Ele H ea Fu els ew ab R en Existing LWR 40,000.00 Fusion Dynamic Dynamic growth growth constraints constraints Price Price sensitive sensitive energy energy demands demands Endogenous Technological Endogenous Technological Learning Learning (ETL) (ETL) Supply side Fusion Scenario 2 - Generated electricity by fuel - with ETL Fission 50,000.00 20,000.00 rg y y 2020 Solar 60,000.00 En e rg 2010 Wind le En e 2000 Other 70,000.00 Global Global MARKAL/TIMES MARKAL/TIMES energy energy model model Long-term Long-term (1990-2100, (1990-2100, 12 12 periods) periods) Single Single world world region region Final Final energy energy demands demands ¾ ¾ Refining, Refining,conversion, conversion,sectoral sectoralheat heatproduction, production, basic basic grids, grids, transport transport Pri m ary Existing 1990 Focus Focus on on supply supply side side (electricity (electricity sector) sector) Other Other sectors sectors 10,000.00 80,000.00 Electricity [TWh] Coal + Seq. Coal + Lig. Generated electricity - baseline Baseline Baseline ¾ ¾ Coal, Coal, gas gasand andnuclear nucleartechnologies technologies account accountfor foraa large large part partof ofthe theelectricity electricityproduction production ¾ Only a small fraction of fusion in 2100 (35 GW) ¾ Only a small fraction of fusion in 2100 (35 GW) Role Role of of fusion fusion is is affected affected by by ¾ ¾ Availability Availabilityof of GEN GENIV IVfission fissionbreeding breedingtechnologies technologies at ataacertain certaincost cost level level ¾ Cumulative CO emission constraints ¾ Cumulative CO22 emission constraints Resource Resource potentials potentials affect affect fusion fusion more more than than share share of of solar solar and and wind wind power power ETL ETL as as aa consistent consistent description description of of progress progress has has an an impact impact The new EFDA-TIMES energy model The new EFDA-TIMES energy model ¾ ¾ 15 15 world world regions regions ¾ ¾ Trade Tradebetween between regions regions ¾ ¾ Soft-link Soft-linkto tomacroeconomic macroeconomicframework framework (general (general equilibrium equilibriummodel modelGEM-E3) GEM-E3) Hydro Fission 50,000.00 Existing LWR Biomass 40,000.00 Fuel cell Gas + Seq. 30,000.00 Gas Acknowledgements Acknowledgements Fusion 20,000.00 Coal + Seq. Coal + Lig. 10,000.00 Existing 1990 Conclusions/Outlook Conclusions/Outlook 2000 2010 2020 2030 2040 2050 Model period 2060 2070 2080 2090 2100 Friedrich Friedrich Schiedel Schiedel Foundation Foundation for for Energy Energy Technology, Technology, Austria Austria Austrian Ministry of Science Austrian Ministry of Science OEAW-EURATOM OEAW-EURATOM Association Association
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