Problem 80
Question
How are the fusion reactions that are the basis for power production in the tokamak described in Section 19.9 different from those that power our Sun?
Step-by-Step Solution
Verified Answer
Answer: The key differences between the fusion reactions in the Sun and a tokamak are:
1. Fuel components: the Sun's fusion reaction primarily involves hydrogen nuclei (protons), while a tokamak uses deuterium and tritium nuclei as fuel.
2. Reaction mechanism: the Sun's fusion process is based on the proton-proton chain, while the tokamak's fusion process is based on the D-T fusion reaction.
3. Temperature and pressure requirements: the Sun's core requires temperatures of around 15 million degrees Celsius for fusion, while a tokamak needs temperatures of around 100-150 million degrees Celsius.
1Step 1: Understand fusion reactions in the Sun
The Sun primarily generates its energy through a process called nuclear fusion. In the Sun's core, the fusion process involves combining four hydrogen nuclei (protons) to form one helium nucleus (two protons and two neutrons) with the release of two positrons and two neutrinos. This process is known as the proton-proton chain.
2Step 2: Understand fusion reactions in the tokamak
A tokamak is a device designed to achieve nuclear fusion for power production on Earth. In a tokamak, fusion occurs when two isotopes of hydrogen, deuterium (D), and tritium (T), are heated to extremely high temperatures and high pressure to form a plasma. Under these conditions, the D and T nuclei combine to form a helium nucleus (two protons and two neutrons) and a high-energy neutron. This is called the D-T fusion reaction.
3Step 3: Compare the key differences between the fusion reactions in the Sun and tokamak
1. Fuel components: In the Sun, the fusion reaction primarily involves hydrogen nuclei (protons). In a tokamak, the reaction involves deuterium and tritium nuclei as fuel.
2. Reaction mechanism: The Sun's fusion process is based on the proton-proton chain, while the tokamak's fusion process is based on the D-T fusion reaction.
3. Temperature and pressure requirements: To initiate fusion, the Sun's core needs temperatures of around 15 million degrees Celsius. On the other hand, to initiate fusion in a tokamak, temperatures of around 100-150 million degrees Celsius are required. This is because the D-T fusion reaction has a higher energy barrier compared to the proton-proton chain.
By highlighting these key differences, we can conclude that the fusion reactions powering the Sun and a tokamak are fundamentally different in terms of their fuel components, reaction mechanisms, and temperature and pressure requirements.
Key Concepts
Tokamak FusionProton-Proton ChainD-T Fusion ReactionSolar Energy Processes
Tokamak Fusion
Imagine a device so powerful it attempts to replicate the energy generation process of the stars right here on Earth—that's the tokamak fusion reactor. In simple terms, tokamak fusion is about forcing atomic nuclei to combine, an event that only naturally occurs under intense pressure and heat like in the core of stars.
Tokamaks are donut-shaped containers designed to control a plasma—a superheated, charged gas of fusion fuel. The tokamak's strong magnetic fields keep this plasma stable and heated to extremes. The deuterium-tritium (D-T) fusion process used in tokamaks yields an enormous amount of energy from just a little fuel, a key advantage for sustainable power generation.
However, reaching the right conditions for D-T fusion is a high-tech challenge. The required temperatures soar above 100 million degrees Celsius, much hotter than the Sun's core, to overcome the strong force that normally keeps atomic nuclei apart. Once achieved, the nuclei can collide with enough energy to fuse, releasing energy as a result.
Tokamaks are donut-shaped containers designed to control a plasma—a superheated, charged gas of fusion fuel. The tokamak's strong magnetic fields keep this plasma stable and heated to extremes. The deuterium-tritium (D-T) fusion process used in tokamaks yields an enormous amount of energy from just a little fuel, a key advantage for sustainable power generation.
However, reaching the right conditions for D-T fusion is a high-tech challenge. The required temperatures soar above 100 million degrees Celsius, much hotter than the Sun's core, to overcome the strong force that normally keeps atomic nuclei apart. Once achieved, the nuclei can collide with enough energy to fuse, releasing energy as a result.
Proton-Proton Chain
The proton-proton chain is a sequence of nuclear reactions that convert hydrogen into helium, the primary energy source of the Sun and other stars like it. This process takes place in the star's core, where pressures and temperatures are extreme, yet much lower than those required for tokamak fusion.
The chain starts with two protons, or hydrogen nuclei, colliding and fusing to create a heavy hydrogen isotope called deuterium. During these reactions, positrons and neutrinos are emitted, and a signature burst of energy is released in the form of gamma rays. This process is a marvel of nature's ability to create energy and happens over billions of years in the stable environment of a star's core.
While there are several steps in a full proton-proton chain, the overall effect is the mass conversion of hydrogen into helium with a release of energy, according to Einstein's famous equation, E=mc^2, where a small amount of mass is transformed into a significant amount of energy.
The chain starts with two protons, or hydrogen nuclei, colliding and fusing to create a heavy hydrogen isotope called deuterium. During these reactions, positrons and neutrinos are emitted, and a signature burst of energy is released in the form of gamma rays. This process is a marvel of nature's ability to create energy and happens over billions of years in the stable environment of a star's core.
While there are several steps in a full proton-proton chain, the overall effect is the mass conversion of hydrogen into helium with a release of energy, according to Einstein's famous equation, E=mc^2, where a small amount of mass is transformed into a significant amount of energy.
D-T Fusion Reaction
The D-T fusion reaction is a specific type of nuclear fusion process and the cornerstone of tokamak reactor design. To understand this, let's look at its fuel first: Deuterium (D), an isotope of hydrogen with an additional neutron, and Tritium (T), an isotope with two additional neutrons.
When deuterium and tritium nuclei are heated and brought close enough to each other, they fuse. This fusion generates a neutron with substantial kinetic energy and a helium-4 nucleus. The neutron flies away and can be captured to generate heat, which, in turn, can be used to produce electricity. The D-T reaction is particularly attractive for fusion power because it has a lower energetic barrier compared to other fusion reactions, making it easier to achieve on Earth.
The challenge here is the creation of a self-sustaining cycle where the energy output from fusion heats new fuel, maintains plasma temperature, and generates electricity—all while containing and controlling this process safely.
When deuterium and tritium nuclei are heated and brought close enough to each other, they fuse. This fusion generates a neutron with substantial kinetic energy and a helium-4 nucleus. The neutron flies away and can be captured to generate heat, which, in turn, can be used to produce electricity. The D-T reaction is particularly attractive for fusion power because it has a lower energetic barrier compared to other fusion reactions, making it easier to achieve on Earth.
The challenge here is the creation of a self-sustaining cycle where the energy output from fusion heats new fuel, maintains plasma temperature, and generates electricity—all while containing and controlling this process safely.
Solar Energy Processes
The Sun, our closest star, is a natural fusion reactor providing light and warmth integral to life on Earth. The solar energy processes involve converting hydrogen into helium deep within the Sun's core, a sequence sustained over billions of years which reflects a delicate balance between gravitational forces and nuclear energy.
In the heart of the Sun, the density and temperature are just right for nuclear fusion to occur through the proton-proton chain. This transforms mass into energy as described by Einstein's principle, resulting in the sunlight that reaches us. Solar energy not only supports life but also drives the weather systems and climate patterns on our planet.
Moreover, human technology harnesses solar energy through photovoltaic cells, directly converting sunlight into electricity. This use of solar energy is a distant cousin to the fusion processes that power stars but shows human ingenuity in tapping into the power of the cosmos.
In the heart of the Sun, the density and temperature are just right for nuclear fusion to occur through the proton-proton chain. This transforms mass into energy as described by Einstein's principle, resulting in the sunlight that reaches us. Solar energy not only supports life but also drives the weather systems and climate patterns on our planet.
Moreover, human technology harnesses solar energy through photovoltaic cells, directly converting sunlight into electricity. This use of solar energy is a distant cousin to the fusion processes that power stars but shows human ingenuity in tapping into the power of the cosmos.
Other exercises in this chapter
Problem 78
For each of the following fission reactions, determine the identity of the unknown nuclide: a. \(^{235} \mathrm{U}+_{0}^{1} \mathrm{n} \rightarrow^{147} \mathrm
View solution Problem 79
In what ways are the fusion reactions that formed \(\alpha\) particles during primordial nucleosynthesis different from those that fuel our Sun today?
View solution Problem 82
All of the following fusion reactions produce \(^{32}\) S. Calculate the energy released in each reaction from the masses of the isotopes: \(^{4} \mathrm{He}(4.
View solution Problem 83
How much energy is released per nucleus of tritium produced during the following reactions? a. \(_{0}^{1} n+\frac{6}{3} L i \rightarrow \frac{4}{2} H e+\frac{3}
View solution