Session C8 Paper #191 Disclaimer—This paper partially fulfills a writing requirement for first year (freshman) engineering students at the University of Pittsburgh Swanson School of Engineering. This paper is a student, not a professional, paper. This paper is based on publicly available information and may not provide complete analyses of all relevant data. If this paper is used for any purpose other than these authors’ partial fulfillment of a writing requirement for first year (freshman) engineering students at the University of Pittsburgh Swanson School of Engineering, the user does so at his or her own risk. ITER NUCLEAR FUSION REACTOR: TESTING THE VIABILITY OF FUTURE FUSION REACTORS Samuel Schiller, [email protected], Mena 3:00, Daniel Funari, [email protected], Mena 3:00 Abstract—The ITER (International Thermonuclear Experimental Reactor) is the largest Tokamak nuclear fusion reactor. Currently under construction in southern France, the ITER will bring nuclear fusion one step closer to a viable source of energy. Today, 85% of the world’s energy is provided by fossil fuels. While effective at producing and storing large amounts of energy when compared to solar, wind, and hydroelectric power, the environmental impact of fossil fuels is highly detrimental. The need for an extremely efficient, reliable, and environmentally safe source of energy has never been a more crucial topic. The potential for fusion power to solve or alleviate the energy crisis is what makes it so attractive to scientists and engineers alike. However, the current state of fusion technology is not without its problems, both scientific and political. ITER may prove to be the next step in the world of fusion, if it can overcome the issues that have plagued Tokamak fusion reactors in the past. The science behind fission and fusion reactions are explained, including the plasma physics and magnetism behind Tokamaks, as well as what makes the ITER tokamak different than reactors past and what the success of ITER could mean for the world. commercial style reactor as heat generated from the reaction will not be used to make steam and will therefore produce no usable energy. The purpose is instead to allow scientists to experiment with much higher plasma volumes, in conditions closer to future commercial fusion power plants [1]. The hopeful success of the ITER project will break new ground in implementing a safe, efficient, sustainable, and environmentally friendly energy source to supply the needs of the future. THE SCIENCE OF NUCLEAR ENERGY Nuclear energy is founded on the immense energy that is stored in the mass of nuclei. Nuclear fusion is a way to harness that energy, just as we do today with nuclear fission power plants and nuclear weapons. As of 2015, Nuclear fission power makes up about 9% of the United States total energy production (19% commercial), whereas the remaining majority of energy of production is from fossil fuels [2]. While fission power does not produce any CO2 emissions, it does produce radioactive waste, which can be very dangerous and difficult to dispose of. Each year, about 10,000 m3 of “high-level waste” is produced by nuclear power plants worldwide [3], all of which require constant cooling and shielding due to the heat generated. The spent radioactive fuel can produce a considerable amount of heat for about 10 years after use, which must be considered during the disposal process, as stated by the World Nuclear Association [3]. While not harmful, once the decay heat dissipates to safe levels, the radioactivity of certain types of the spent fuel take up to hundreds of thousands of years to fully decay. Theoretically, the operation of nuclear power plants should be quite safe, however, there is always the risk of human error, unpredictable natural disasters, and terrorism, which can lead to a meltdown. In the case of a meltdown, the surrounding land will likely become unfit for life for an extremely long time. For example, the 30 km2 area surrounding the Chernobyl meltdown will still be dangerously radioactive for another 20,000 years [4]. Because of these risks, policy makers remain wary of fission power, despite the clear advantages. Keywords—Nuclear Fusion, Tokamak, Renewable Energy, Nuclear Fission, ITER, Plasma interactions THE ENERGY CRISIS AND ITER As climate change continues to become a more pressing issue, industrialized countries must shift their main energy focus from fossil fuels like coal, to more environmentally friendly and sustainable sources. One of these possible sources is nuclear fusion. Nuclear fusion has been a sough after energy source since the 1930s when it was discovered as the source of the Sun’s energy. However, due to the technical challenges of achieving a controlled and stable fusion reaction, it has yet to become a viable energy source. The International Thermonuclear Experimental Reactor (ITER) will not only be the largest fusion reactor ever built, but will be the first to achieve a positive net energy output. Although ITER will produce more energy than required to keep it running, it will not function as a University of Pittsburgh Swanson School of Engineering 3.31.2017 1 Samuel Schiller Daniel Funari Nuclear Fission This process is identical to all types of power plants which instead use the burning of coal or other fossil fuels, which release harmful amounts of carbon dioxide and other air pollutants, to create the steam. Nuclear fission is the splitting of an atomic nuclei. When a larger unstable atom is split, it will break into 2 smaller isotopes while emitting some neutrons. However, the sum of the remaining parts only makes up about 99.9% of the original mass. The remaining 0.1% is converted into a large amount of energy conforming to Einstein's mass-energy equivalence equation E = mc2. The factor c2—the speed of light squared— is so large, ~9x1016, that even a tiny amount of mass can be converted to a huge amount of energy. In this case, the energy required to split the atom is less than the energy released after fission, resulting in a net energy gain in the form of heat. Just one atom of enriched uranium — uranium containing a higher percentage of U-235 isotopes — will release about 200 MeV (3.2x10-11J) of energy, which on its own is not substantial since it would take about 3.121 billion of these reactions to produce 1 joule of heat energy [5]. However, nuclear power plants use an amount of fuel that far exceeds 3 billion by many orders of magnitude. The result is a huge amount of energy in the form of heat. Just one tonne of enriched uranium has the energy output of up to 20,000 tonnes of black coal or 8.5 million cubic meters of gasoline [6]. Typical power plants use enriched uranium for fuel, which is 3.5%-5% U-235, compared to natural uranium that contains only 0.7% U-235 [6]. To start the reaction, alpha particles are fired at neutron emitting sources (compounds that have beryllium), and a reaction occurs where a neutron is emitted and a nuclide is produced. The high-energy neutrons then collide with the uranium, which is enough to start the fission reaction. Each U-235 isotope can emit up to 3 neutrons, which proceed to start more fission reactions, resulting in a prolonged chain reaction producing immense heat. Much of the U-238 is also consumed in the reaction and turned into Plutonium which also undergoes fission, accounting for a third of the reactor's energy output [6]. The power plant generates electricity, as seen in the Figure 1, by boiling water from the radioactive material. Nuclear Fusion Nuclear fusion is a process that is very similar to fission, but it has greater results depending on what nuclei you fuse. Just as nuclear fission occurs spontaneously yet rarely in nature, so does fusion. In fact, fusion is occurring all the time, just not on Earth. The process of nuclear fusion takes place in the sun (and other stars), and it's what gives the sun its immense energy. While fission is the splitting of two large atoms, fusion, is the combination of two lighter atoms, usually hydrogen and its isotopes (deuterium/tritium). Because of the massive gravity of the sun, all the hydrogen inside becomes super compressed and extremely hot — 15 million degrees Celsius. At this point the hydrogen is no longer gas. The electrons are stripped from the hydrogen isotopes and plasma, a fluid of protons and electrons, is formed. The sun then goes through a process called a proton-proton chain, shown Figure 2, where the immense heat causes two protons to fuse (overcoming the nuclear and electrostatic repelling force), one of which will "capture" an electron, thus cancelling out its charge and creating a neutron. FIGURE 2 [8] Proton-Proton Chain Once fused, the neutron and proton create a deuteron (a deuterium nucleus). That deuteron will fuse with another proton (hence the p-p chain term), making Helium-3. Then two He-3 nuclei will fuse and form unstable beryllium-6, which degenerates into one Helium-4 nuclei and 2 protons. Thus 4 protons are transformed into Helium-4. However, the mass of the resulting Helium nuclei does not equal the mass of the 4 initial protons. The missing mass, just like in fission, is converted into heat energy by E=mc2. Just one of these reactions creates 25 MeV, which is less than the 200 MeV per Figure 1 [7] Power Plant Diagram The steam produced by the boiling water passes through a turbine connected to an electric generator that converts the mechanical energy of the spinning turbine into electricity. 2 Samuel Schiller Daniel Funari U-235 fission reaction. However, per nucleon, fusion produces about 7 times as much energy than fission Fission and fusion are opposing processes, and the reason both release a net heat energy gain, is dependent on what types of nuclei are being fused/split. If Uranium-235 underwent fusion, there would be a net heat loss, as would occur if helium underwent fission. This is because the binding energy of uranium-235 is higher than the sum of the binding energies of the smaller atoms that would fuse. On the other hand, the binding energy for helium is lower than the binding energies of its parts. The proton-proton chain process described above is the fusion process in sun and other stars, but unfortunately, that same reaction cannot be recreated on earth due to the lack of immense gravitational pressure. In the sun, two protons are turned into neutrons, a reaction that would take far too long to complete. To obtain the neutrons, two isotopes of hydrogen, are used which already contain the necessary neutrons. Deuterium has one neutron and tritium has two. This D-T (Deuterium-Tritium) reaction will yield about 17 MeV of energy, a He-4 particle, and a single neutron (4/5 of that energy is in the neutron). Then, that neutron is absorbed by a heat blanket lining the reaction chamber (which is cooled by water) and converted into electricity via conventional steam technology. However, since tritium does not occur naturally in nature, it would have to be bred in the reactor by bombarding lithium with neutrons. Nuclear fusion has many benefits over fission. While uranium is an exhaustible resource, hydrogen is limitless since it is the most abundant element in the universe. Also, fission creates radioactive byproducts, while fusion only produces helium, high energy neutrons which can be easily contained and present no radiation exposure risk, and tritium which is recycled and reused in the reactor. There is, in addition, no risk of a meltdown with fusion, since the reaction stops when there is insufficient energy. Even if the containment system fails, the worst that can happen is a fire, which can be solved by conventional fire safety methods. Yet while the advantages are clear, fission is a developed technology that is currently being implemented across the world. Fusion, on the other hand, is experimental, and while successful fusion reactions have been created, none have produced a net heat gain, and these experimental reactors are only able to function in short bursts [10][11]. Containing 150 Million Degree Plasma The first and most obvious challenge is the incredibly high temperatures needed for the fusion reaction to take place. The fusion of deuterium and tritium requires temperatures upward of 150 million degrees Celsius [12]. The sun, which burns at approximately 15 million degrees, is only able to sustain its fusion due to the immense pressure inside its core. The approximately 150-million-degree plasma that fusion requires would instantly vaporize and destroy any surface that it touched. Scientists overcame this difficulty with the use of magnetic confinement, which uses a series of magnets to levitate the plasma inside of the reactor [12]. Even with magnetic confinement however, the inner walls of current and future reactors will over time become damaged by the frequent exposure to the hot plasma. The tiles lining the reactor walls will need recurrent replacement to ensure no damage occurs to vital components of the reactor. Structural Challenges Current fusion reactors do not operate continuously and instead function in long pulses. In addition to this intense heat, the reactor, throughout its lifetime will be subjected to thousands of these magnetic pulses, putting an extreme amount of stress onto the structure of the reactor. The structure must be able to withstand these pulses in combination with the weakening of the metals caused by the extreme heat. According to a 2001 journal article about plasma material interactions (PMIs) from the Institute of Physics, the energy exposed to the wall, “can be high enough to melt and vaporize the surface material rapidly” [13]. In addition to the weakening of reactor walls due to heat, exposure to the plasma has other degrading effects, mainly erosion and hydrogen trapping. Erosion of the reactor walls is due to many processes, but mainly by a process called sputtering [13]. Sputtering occurs when atoms in a material become energized to the point of overcoming their binding energy, and are then ejected from the surface. This process effectively determines the life of the plasma facing components (PFCs) [13]. The repeated ejection of atoms not only produces PFC erosion but causes impurities which cool the plasma core, possibly affecting the fusion reactions. The plasma also causes an accumulation of hydrogen deposits, mainly tritium, which also weaken the PFCs. The deposited tritium must be removed regularly to ensure proper function and prevent further wall damage and plasma impurity [13]. Having to contain such a high-energy source as fusing plasma causes immense structural integrity challenges. CHALLENGES FOR FUSION POWER Fusion power is the most ideal energy source. It’s able to create an enormous amount of energy from a limited amount a fuel, like nuclear fission, while producing no long lasting radioactive waste or other toxins released into the environment. Being such an ideal source, it has many challenges. Cost and Availability The most important challenge affecting the rate of fusion research is development cost. Modern fusion reactors require billions in funding and can take more than a decade to construct. The ITER reactor is projected to cost well over $18 3 Samuel Schiller Daniel Funari billion [14]. Therefore, ITER required funding by multiple countries to sustain its cost. Although fusion research and construction requires billions in funding, the low cost of the electricity it produces “force fusion power towards base-load supply” [13]. A base load energy source is used continuously to supply the minimum daily energy needed. A fusion plant must have very minimal down time to sustain this supply need, which while easily reached by fission, “will be a stretch for any planned fusion power station” [13]. The practicality of sustained energy generation in Tokamak style reactors will be one of the main question to be answered by the ITER project. production accounted for 37% of the total 2015 CO2 emissions in the US [16]. Under this definition, fusion power is incredibly sustainable. In research conducted at the University of Tokyo, early fusion reactors in total would produce around 43.9g of CO2 for every kWh of energy produced, with modifications that could lower this value to only 22.5g for future reactors, which is on par with fission and hydroelectric power [17]. In addition, fusion produces a much greater amount of energy compared to these sources. However, economic sustainability is as much an issue. As stated previously, fusion reactors require decades of construction time and billions of dollars in funding, which makes fusion less economically viable in the near future. Future reactors would need to be much cheaper than the ITER. Another important factor is the abundance of fusion fuel. Hydrogen-1 and deuterium are easily extracted from water and heavy water and do not pose any supply difficulty. However, tritium must be produced from lithium. While reserves contain an abundant supply of lithium, the use of its us in batteries has been exponentially increasing which could pose a supply risk for fusion power [18]. From research conducted at the Max Planck Institute for Plasma Physics, seawater theoretically contains enough lithium to supply “2,760 power plants for 23 million years” [18]. Although this is only theoretically, the scale of this value ensures that consuming the Earth’s lithium supply is not an issue for fusion power, especially with the continuing research into non-lithium batteries. While fusion power is extremely environmentally friendly, it is still questionable whether it will be economically sustainable. Production of Dangerous Materials The argument for fusion power is that it can produce power on the scale of fission power without the waste or possibility of a meltdown. While all radioactive isotopes involved in the fusion process have short half-lives, ensuring power plants will not expose damaging amounts of long lived radioactivity to the surrounding environments, skeptics claim that dangers may arise in the large-scale adaptation of fusion energy [15]. The two components of the fusion process that this danger arises from are tritium, one of the two hydrogen isotopes fused, and high-energy neutrons. Even though tritium has many industrial uses, it is radioactive and is also an essential component in boosted fission weapons which increase the explosive yield of fission weapons by adding a small fusion reaction triggered by the fission explosion. However enriched uranium and other nuclear materials are needed in addition to the tritium to develop fission boosted weapons. Should nuclear weapon growth become a more concerning issue, international restrictions may be placed on tritium availability, which could dramatically affect nuclear fusion research. The other concerning product of fusion reactions is the release of high-energy neutrons [15]. When these neutrons strike “depleted uranium”, they bind to some nuclei and transform parts of the uranium into fissile isotopes that can be used in nuclear weapons. According to a 2008 report by the Institute of Physics on nuclear fusion, a reactor with this intent would require “special engineering of the tokamak, including additional cooling, shielding and a reprocessing capability” [15]. These additional features would be easily noticed and regulations “should be sufficient to prevent illicit production of any fissile materials” [15]. This reprocessing ability however, is beneficial as it creates fuel for use in fission power plants. Although there are many safeguards in place to prevent illicit production of fissionable materials, should fusion energy become widely adopted, increased regulations and monitoring may be necessary. TOKAMAK STYLE REACTOR The most developed reactor design currently is the tokamak reactor. While tokamaks vary in shapes and sizes, the general design remains unchanged. A tokamak reactor contains the plasma by means of a toroidal shaped reaction chamber. Using magnetic fields, the plasma is able to be confined and controlled within the torus [10]. Plasma Confinement For an earth bound fusion reaction to take place, the deuterium and tritium must be heated to extreme temperatures of around 150 million degrees Celsius (10 times hotter than the sun). Once the fuel reaches this temperature, there is then the problem of containing it. Because proton plasma at 150 million degrees Celsius is completely ionized and is electrically charged, it can be manipulated by magnetism. The plasma creates its own magnetic field due to its high volume of charged particles, and is thus affected by the magnetic field. This is done with 3 sets of magnetic coils in most cases, sometimes with 4. Around the torus, there are several vertical coils called the toroidal coils that induce a current in the plasma which goes around in a circle (following the path of the doughnut-shaped chamber). Also around the torus, there Economic and Environmental Impact When discussing the sustainability of a certain technology, people mainly think about its environmental impact. This is understandable considering that energy 4 Samuel Schiller Daniel Funari are a series of horizontal coils that surround the reaction chamber [10]. These coils, called the poloidal coils, induce a current in the plasma that goes in circles perpendicular to the toroidal induced current. Along with the poloidal coils shown in Figure 3, there is also a central solenoid coil that induces a field like that of the poloidal coils [10]. also increases, which causes even more heat by fusion and kinetic energy. While higher power magnets induce more current, they also compress the plasma further, which increases the collision frequency and plasma pressure, which in turn increases temperature. There are issues with induced current plasma fusion however. In order to induce a current, the reactor must be run by a giant transformer, which intrinsically operates in a pulsed manner, thus the plasma can only exist and be contained for short bursts. When the transformer is recharging, the plasma ceases [19]. The run time of tokamak reactors could possibly be prolonged by use of a complex plasma mechanic called the bootstrap current [20]. Due to the lack of uniformity in the magnetic field, the motion of the plasma is not symmetrical. This leads to a residual current that is not induced [20]. This problem can also be alleviated using other heating methods [15]. One way to heat the plasma is through neutral beam heating [19]. With this method, beams of neutral particles that are not affected by the magnetic field are fired into the plasma/fuel in order to heat it. To accomplish this, isotopes of hydrogen, deuterium, hydrogen-1, or tritium, are accelerated through a high voltage, into a neutralizer section (such as a gas cloud), where they gain electrons to become neutral [19]. Once neutral, the particles still have a high remaining velocity as they enter the reaction chamber to collide with the plasma, thus increasing the plasma's overall speed and heat. Another way is through radio-frequency heating [19]. In this process, high frequency electromagnetic waves are generated outside the torus that match the resonance of the particles in the plasma. The energy in the waves can then be added to the energy in the plasma, increasing its overall heat. Once fusion occurs, the heat from the expelled neutrons collides with the walls of the reactor chamber, which is cooled by water. Then the fusion part of the process is over and electricity is generated through conventional steam technology. For a net energy gain to occur, the heat energy generated must exceed the energy required start and sustain the reaction. Unfortunately, no reactor has been able to accomplish this so far, rendering all current fission reactors purely experimental. The current largest tokamak reactor is the Joint European Torus (JET), which has a major radius of 3 meters with a plasma volume of 100 m3, and was able to generate 16 MW of power for a few seconds. The JET reactor only produces about 64% of the 24 MW input energy [21]. Figure 3 [15] Tokamak Magnet Set-Up These coils essentially make up a giant transformer, where the plasma acts as a secondary winding. The result is a helical shaped current that spins around the in the toroid. This motion of the plasma keeps it in the center of the chamber cross sections, away from any chamber walls. In some tokamaks, there are also helical coils surrounding the chamber, which assist further in the motion/confinement of the plasma. Because all the electrons are separated from the protons in the plasma, there is a two-way motion going on in the torus. While the positive charges circle one way, the stripped electrons rotate the other way [15]. The plasma inside the torus ends ups moving rapidly, with current tokamaks reaching speeds upward of 100 km/s. These extreme speeds increase the number of collisions and in turn, the number of fusion reactions [19]. Plasma Heating Containing super-heated plasma is just one of the challenges associated with fusion reactors. Heating the fuel to the required temperature, and keeping it there, is done in a combination of many different ways. One way is by magnetism/ohmic heating, which is also the same process confining the plasma [10]. When a such a high-energy current is induced in the fuel/plasma, it increases the amount of resistance per second the current must go through. This results in a great amount of induced heat. Unfortunately, as the heat of the plasma increases, its resistance decreases, thus reducing the heating effect. The magnetic coils heat the plasma in other ways as well. Due to the high speeds at which the plasma is moving from the induced current, the number of collisions ITER: FIRST ENERGY PRODUCING FUSION REACTOR ITER is will be the first reactor that will have a Q-value above 1. The Q-value is the ratio of output energy to input energy. With the Q-value estimated to be around 10, ITER will produce 500 MW of heat from an input of only 50 MW [1]. The reactor, as the name states, is purely experimental, as it will not actually generate usable energy from the produced heat. However, the knowledge of much higher plasma volume 5 Samuel Schiller Daniel Funari interactions will pave the way for reactors that will. History and Construction The ITER project was first proposed in 1985 by the Soviet Union. The idea was to create an international effort to develop nuclear fusion as viable energy source. The following year the United States reached an agreement with the European Union, Japan, and the Soviet Union to collaborate on a design for a large international fusion reactor [21]. The design process began midway through 1988 with the Conceptual Design Activities (CDA) in Germany which through 1990, in addition to designing the reactor, performed an environmental impact analysis, developed site requirements, estimated the cost, and outlined the schedule for the engineering, design, and operation [21]. Two years after the completion of the CDA, the Engineering Design Activities (ERA) began which carried on through 2001. After completing the initial design in 1998, the ERA was extended three years to implement further cost cutting measures. During this ERA extension period the US withdrew, although temporarily, due to concerns about the projected cost. In 2005, the ITER members officially agreed to construct ITER in Cadarache, France. The ITER agreement was signed in November of 2006 and construction began only two months later [20]. Construction of the reactor building however, did not begin until August of 2010. Initially, during the CDA, the estimated cost and schedule was laid out. According to the official CDA report, ITER was estimated to be completed by 2003, with only $4.9 Billion in construction costs [14]. Although this was only an initial estimation, the cost continually rose. Currently, the estimated cost is around the scope of $18 Billion. When construction began in 2010, the ITER schedule planned for the first plasma operation in 2019, with the first D-T plasma occurring in 2027. In an ITER Council meeting in November of last year, the schedule was unanimously delayed again, projecting initial plasma in 2025, and D-T operation in 2035 [22]. While it is too early to tell if this updated schedule will hold up, managing members claim ITER has remained on schedule, and on budget throughout 2016, increasing global confidence in ITER’s success. Figure 4 [21] ITER Size Comparison ITER is planned to have a 500 MW energy output and a 300500 second run time, compared to JET's output of 16 MW and run time of 60 seconds. The DEMO reactor, which is also shown in Figure 4, will be expanded on later and is the succession to the ITER project. The vacuum vessel where the reaction takes place will be made from 5200 tonnes of stainless steel. Lining the wall of the chamber will be the blanket. The blanket (covering 600 m2) will be responsible for absorbing most the heat from the plasma. The ITER team has chosen beryllium as the element to cover the first blanket wall for its high heat resistant qualities, with stainless steel and copper as the secondary walls. The blanket will be hit by the high-energy neutrons from the fusion reaction, absorbing their heat energy. ITER will be the first reactor to utilize active water cooling, where water is pumped around the blanket constantly to remove massive amounts of heat. The blanket is planned to be made up of 440 modules, each weighing 4.6 tonnes. ITER will also be the first reactor to be designed for deuterium and tritium reactions. In the blanket, there will be 6 dedicated ports that will be open for a lithium layer that will breed tritium once a high-speed neutron collides with it. While not fully designed to accommodate entirely self-sufficient tritium breeding, ITER will be able to accommodate tritium breeding testing that will give us the research necessary for future reactors [1]. The magnets that will heat and confine the plasma will have a stored energy of 51 Gigajoules, and a combined magnetic field of 30.8 T (Tesla). The magnetic coils are made of niobium-tin, which is superconductive at 4 degrees Kelvin. By use of cryogenically cooled helium, the 10000 tonnes of coil will be cooled to 4 K, thus reducing the power needed to operate the coils and optimizing the net energy gain from the reaction. The cryogenic helium will be cooled in a series of helium refrigerators in a separate building, with a total helium supply of 25 tonnes. Niobium-tin is extremely expensive, and ITER demands 100,000 km of it for the coils, an amount which has taken 9 suppliers 7 years to manufacture. To put in perspective, during coil production the 15 tonne/year production rate increased to 100, just for ITER. Surrounding What Makes ITER Different Much of what makes ITER different is simply the scale at which all the components have been ramped up. ITER boasts multiple record breaking scientific endeavors, such as having the some of the largest vacuum systems, superconducting magnetic coil, and cryogenic systems ever built. The primary systems alone will weigh 23,000 tonnes. The ITER tokamak will be the largest Tokamak ever built, with a chamber radius of 6.2 meters and a plasma volume of 840 m3. As seen in Figure 4 demonstrating ITER’s size, the planned capabilities of ITER far exceed the current capabilities of any of its predecessors. 6 Samuel Schiller Daniel Funari the torus, there will be 18 “D”-shaped toroidal magnets, each weighing 310 tonnes (for a total of 5,580 tonnes). ITER installed the first of these magnets in January of this year. The toroidal magnets will store 41 GJ, and generate 11.8 T of magnetic field. There will also be 6 poloidal magnets, the largest with a diameter of 24 meters and a weight of 400 tonnes, storing 4 GJ and generating a magnetic field of 6 T. The largest magnet will be the central solenoid, standing at 13 meters tall and 4 meters wide (1000 tonnes), storing 6.4 GJ and emitting a field of 13 T. The solenoid will induce a current of 15 MA in the plasma, making it the backbone of the entire magnet system. All of these systems will be housed in an enormous 16,000 m3 vacuum chamber that stands 30 meters high that will evaporate and prevent any inside moisture [1][19]. As the plasma develops, fuel will be injected at 400 PA m3/s, an entire order of magnitude higher than any existing fuel injecting system. In order to meet the initial heat required for fusion to occur, ITER will utilize 3 external heating systems. The first one, two neutral beam injectors, will fire deuterium isotopes at 4 times the speed of any existing neutral beam injector. However, this makes using positive ions very difficult to neutralize prior to entering the reactor. Instead of using positive ions, ITER will fire negative ions into the plasma since the extra electron that makes it negative is loosely bound. Secondly there will be 2 external electromagnetic wave heaters, one that emits waves at a frequency resonant to that of the ions, and one that emits waves with a resonance to that of electrons (170 GHz). The waves will increase the energy of the ions/electrons, which will in turn increase the heat of the system [15][19][24]. FUSION’S FUTURE A world powered by fusion power is not imminent. There still much more research needed to determine the viability of nuclear fusion as a source of energy. With the initial operation of ITER less than ten years away, a world powered by fusion may be a reality within the century. Should ITER construction and operation remain on track, multiple DEMO reactors could then be constructed around the world, producing gigawatts of clean, sustainable, and inexhaustible energy, ending the need for environmentally damaging energy sources like coal, oil, and natural gas. SOURCES [1] “What Will ITER Do” ITER. n.d. Accessed 01.27.2017. https://www.iter.org/sci/Goals [2] "Nuclear Power in the USA." Nuclear Power in the USA. World Nuclear Association, 23 Mar. 2017. Web. 29 Mar. 2017. http://www.world-nuclear.org/informationlibrary/country-profiles/countries-t-z/usa-nuclearpower.aspx [3]“Radioactive Waste Management.” World Nuclear Association. 10.2016. Accessed 02.24.2017. http://www.world-nuclear.org/information-library/nuclearfuel-cycle/nuclear-wastes/radioactive-wastemanagement.aspx [4]“Chernobyl Accident 1986.” World Nuclear Association. 09.2016. Accessed 2.24.2017. http://www.worldnuclear.org/information-library/safety-and-security/safetyof-plants/chernobyl-accident.aspx [5]“Nuclear Fission.” Nuclear-Energy. 4.21.2014. Accessed 02.26.2017. https://nuclear-energy.net/what-is-nuclearenergy/nuclear-fission [6]“The Nuclear Fuel Cycle.” World Nuclear Association. 06.2016. Accessed 2.26.2017. http://www.worldnuclear.org/information-library/nuclear-fuelcycle/introduction/nuclear-fuel-cycle-overview.aspx [7]“Fission Reactor Diagram.” Union of Concerned Scientists. N.d. Accessed 2.27.2017. http://www.ucsusa.org/nuclear-power/nuclear-powertechnology/how-nuclear-power-works#.WLBEkTsrJPY [8]"The Proton-Proton Cycle." The Proton-Proton Cycle. N.p., n.d. Web. 25 Mar. 2017. http://cseligman.com/text/sun/ppcycle.htm [9]“Energy from Nuclear Fusion.” Emc2-Explained. N.d. Accessed 2.28.2017. http://www.emc2explained.info/Emc2/Fusion.htm#.WLUrffI8bjY [10] J. Ongena. "Nuclear fusion and its large potential for the future world energy supply." NUKLEONIKA. Vol. 61, No. 4. 4.19.2016. [11]F. Cain. “Fusion in the Sun.” Universe Today. After ITER: “DEMO” Depending on ITER’s success, the next step in the world of fusion will be the DEMO reactors. DEMO will be the “demonstration” prototype reactors for the world of commercial nuclear fusion power. While ITER's purpose is to demonstrate the safety and possibility of net energy and tritium breeding, DEMO's purpose will be to demonstrate the economic efficiency of fusion. While ITER uses tritium mostly from the global deposit, DEMO will breed 100% of its tritium on site. Other goals of DEMO include continuous operation, a Q-value between 30 and 50 compared to ITER’s Q-value of 10, and a focus on energy collection rather than diagnostics [24]. While DEMO is far down the road (too early to estimate its completion date), currently there are other reactor designs in development alongside ITER, that could also hold promise. Spherical tokamaks change the way the plasma behaves, increasing energy output at a lower cost. The stellarator reactor is a similarly shaped reactor that operates without the need for an induced plasma current by twisting the plasma, allowing prolonged periods of operation compared to tokamaks [20]. 7 Samuel Schiller Daniel Funari 12.24.2015. 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Xanthopoulos. “Stellarator and tokamak plasmas: a comparison.” IOP Science - Plasma Physics and Controlled Fusion, vol. 54, no. 12, 2012. “The History of Nuclear Energy.” U.S. Department of Energy. N.d. pp. 5-21. Accessed 2.24.2017. https://energy.gov/sites/prod/files/The%20History%20of%2 0Nuclear%20Energy_0.pdf P. Mollard. "Star power: Troubled ITER nuclear fusion project seeks new path." Phys.org - News and Articles on Science and Technology. 5.22.2015. Accessed 1.26.2017. https://phys.org/news/2015-05-star-power-iter-nuclearfusion.html “Physics of Uranium and Nuclear Energy.” World Nuclear Association. 09.2016. Accessed 2.26.2017. http://www.world-nuclear.org/information-library/nuclearfuel-cycle/introduction/physics-of-nuclear-energy.aspx J. Sanchez. "Nuclear fusion as a massive, clean, and inexhaustible energy source for the second half of the century: brief history, status, and perspective." Energy Science & Engineering. Vol. 2, No. 4. 9.26.2014. M. Ulrickson. Presentation on plasma material interactions. GCEP Fusion Workshop. 5.2.2006. https://gcep.stanford.edu/pdfs/qa4ScQIicxkve2pX9D7Yg/ulrickson_fusion_05_06.pdf ACKNOWLEDGMENTS We would like to thank our co-chair, Danielle Broderick, for continually taking time out of her busy schedule to help us with this project ADDITIONAL SOURCES J. N. Bahcall. “How the Sun Shines.” Nobelprize.org. 6.29.2000. Accessed 2.26.2017. http://www.nobelprize.org/nobel_prizes/themes/physics/fusi 8
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