Much of the research on controlled fusion focuses on the problem of how to contain the reacting material. Magnetic fields appear to be the most promising mode of containment. Why is containment such a problem? Why must one resort to magnetic fields for containment?

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Containment is a problem in controlled fusion research due to the need to control highly reactive plasma at extreme temperatures and pressures, which no solid material can withstand. Magnetic fields offer a promising solution for containment, as they confine and control the motion of the charged particles within the plasma without direct contact with the reactor walls. This minimizes the risk of damage to materials and allows for continuous control of plasma conditions. Popular magnetic confinement methods include tokamaks and stellarators, which researchers are actively working on to improve and achieve practical controlled fusion on Earth.

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01

Introduction to Controlled Fusion

Controlled fusion is the process of combining light atomic nuclei at extremely high temperatures and pressures to release energy in the form of heat and light, similar to the process that occurs in the sun. The main challenge in achieving controlled fusion on Earth is to confine and control the highly reactive plasma, which is composed of ions and electrons, as the atoms in the plasma react with one another, producing nuclear fusion products and enormous amounts of energy.
02

Problem of Containment

One of the biggest challenges in controlled fusion research is containing the reacting plasma. The plasma needs to be at an extremely high temperature (millions of degrees Celsius) and pressure for fusion reactions to occur. At these temperatures, no solid material can withstand direct contact with the plasma, and the extreme pressure requires a robust containment system to prevent the plasma from escaping or coming into contact with the reactor walls.
03

Advantages of Magnetic Fields

Plasma, being an ionized gas, is composed of charged particles that respond to electric and magnetic fields. Magnetic fields can be used to confine and control the motion of the charged particles within the plasma. The use of magnetic fields for containment has several advantages, such as: 1. Because the plasma does not come into direct contact with the reactor walls, it minimizes the risk of damage to the materials and maintains the integrity of the containment system. 2. Magnetic fields can be adjusted and controlled to create various configurations that help in stabilizing the plasma and maintaining the necessary conditions for controlled fusion to occur. 3. The use of magnetic fields allows for the continuous containment and control of the plasma, as opposed to other methods that might require shutting down the reactions for maintenance or repair.
04

Magnetic Confinement Fusion Methods

Some popular magnetic confinement fusion methods include: 1. Tokamak: A toroidal (doughnut-shaped) device in which magnetic fields are generated by a combination of externally applied magnets and the current-driven plasma itself. These magnetic fields provide confinement and stabilization of the plasma. 2. Stellarator: A specialized twisting, toroidal device in which magnetic fields are generated solely by externally applied magnets. These fields are created to maintain precise control over the plasma and its confinement without relying on plasma currents. In conclusion, containment is a significant problem in controlled fusion research because of the need to control highly reactive plasma at extreme temperatures and pressures. Magnetic fields offer a promising method for containment due to their ability to confine charged particles without direct contact with the reactor walls, adjustability, and capacity for continuous control of the plasma. Researchers are actively working on improving magnetic confinement fusion methods, such as tokamaks and stellarators, to achieve practical and sustainable controlled fusion on Earth.

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Most popular questions from this chapter

Calculate the amount of energy released per gram of hydrogen nuclei reacted for the following reaction. The atomic masses are $_{1}^{1} \mathrm{H}, \quad 1.00782\( u; \)_{1}^{2} \mathrm{H}, \quad 2.01410 \quad \mathrm{u} ;$ and an electron, \(5.4858 \times 10^{-4}\) u. (Hint: Think carefully about how to account for the electron mass.) $$ _{1}^{1} \mathrm{H}+_{1}^{1} \mathrm{H} \longrightarrow_{1}^{2} \mathrm{H}+_{+1}^{0} \mathrm{e} $$

Write an equation describing the radioactive decay of each of the following nuclides. (The particle produced is shown in parentheses, except for electron capture, where an electron is a reactant.) a.\(_{1}^{3} \mathrm{H}(\beta)\) b. \(_{3}^{8} \operatorname{Li}(\beta \text { followed by } \alpha)\) c. \(\quad_{4}^{7}\) Be (electron capture) d. \(_{5}^{8} \mathrm{B}(\text { positron })\)

The number of radioactive nuclides in a sample decays from $1.00 \times 10^{20}\( to \)2.50 \times 10^{19}$ in 10.0 minutes. What is the half-life of this radioactive species?

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