Spin Polarization Effect on Ignition Access Condition for D-T and D-<sup>3</sup>He Tokamak Fusion Reactors

Mitarai, O.; Hasuyama, H.; Wakuta, Y.

doi:10.13182/fst92-a29720

Cited by 11 publications

(7 citation statements)

References 25 publications

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“…Also, as was discussed earlier, solar system-class operation presupposed propellant and fuel supply availability in the hydrogen and helium-rich outer planet atmospheres and satellites, mitigating supply issues surrounding 3 He. D 3 He fuel with a spin vector polarized parallel to the magnetic field was used to capitalize on the up-to 50% enhancement in fusion reactivity cross section, 24,25 tremendously improving the charged output power. The methods of creating and utilizing polarized fuel have been developed through theory (DT and D 3 He) and experiment (DT) 24,25 .…”

Section: Plasma Modeling and Characteristicsmentioning

confidence: 99%

“…D 3 He fuel with a spin vector polarized parallel to the magnetic field was used to capitalize on the up-to 50% enhancement in fusion reactivity cross section, 24,25 tremendously improving the charged output power. The methods of creating and utilizing polarized fuel have been developed through theory (DT and D 3 He) and experiment (DT) 24,25 . Although much work remains on maintaining fuel polarization, it is well known that ionization and atomic collision processes cannot result in depolarization 25 .…”

Section: Plasma Modeling and Characteristicsmentioning

confidence: 99%

“…The methods of creating and utilizing polarized fuel have been developed through theory (DT and D 3 He) and experiment (DT) 24,25 . Although much work remains on maintaining fuel polarization, it is well known that ionization and atomic collision processes cannot result in depolarization 25 . However, there are potentially significant design impacts to the first wall and fuel injection that will be discussed later.…”

Section: Plasma Modeling and Characteristicsmentioning

confidence: 99%

“…37,40 In a related issue, beryllium could have a detrimental effect on spin-polarized fuel. It has been suggested from today's research reactors that recycling of fuel off a metallic first wall surface could cause significant depolarization 25 . This issue must be resolved should the effect is verified.…”

Section: First Wallmentioning

confidence: 99%

“…It is thought that injecting such pellets during ignited, high temperature operation will be very difficult. 25 An earlier conceptual design study of a mirror reactor propulsion concept suggested a two-stage mechanical (centrifugal) and electromagnetic railgun injector be used for D 3 He pellets. 93 This study and others have suggested a potential approach involving frozen light metal shelled (lithium deuteride) pellets encapsulating 3 He fluid.…”

Section: Fuel Injector and Tankagementioning

confidence: 99%

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Section: Plasma Modeling and Characteristicsmentioning

confidence: 99%

Section: Plasma Modeling and Characteristicsmentioning

confidence: 99%

Section: Plasma Modeling and Characteristicsmentioning

confidence: 99%

Section: First Wallmentioning

confidence: 99%

Section: Fuel Injector and Tankagementioning

confidence: 99%

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D-3He tokamak reactor with inductive a.c. and unidirectional current operation

Mitarai

1995

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Velocity distribution functions and reactivity of D–T fusion plasma with spin-polarized fuel

Takahashi

Nakao

2001

Fusion Engineering and Design

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In 1982, Kulsrud et aI . have examined the possibility of spin-polarized fusion and found that the depolarization rate of polarized fusion fuels is very small compared to the reaction rates in the case that the mechanisms of depolarization such as the binary collisions, the fl uctuation of magnetic field and the inhomogeneity of the field are taken into account [l]. In the present paper, we have made the kinetic model with velocity distributions indexed by the magnetic quantum numbers for spin-polarized fusion plasmas and investigated the effect of depolarization of the polarized fuels on the thermonuclear reactivity for D-T fusion plasma.Since the spin quantum number of deuteron D is unity, the magnetic quantum number of D, mo, has the values of 1, 0 and -1. Deuterons D in an unpolarized plasma equally exist in the three spin states. Thus the probabilities of the existence in each spin states become 1/3. The probabilities for polarized particles, however, should not be identical among three spin states. Therefore, the ordinary distribution function of D, i.e., fo(v), will be described by the expression:where the superscript +, 0 and -represent the magnetic quantum number for mo=l, 0 and -1, respectively. Similary to D, the distribution function of T is also classable by the spin states. Since the spin quantum number of T is 1/2, the magnetic quantum numbers of Tare 1/2 and -1/2. Thus the distribution function of T should be classified as ITCV) = IT+(V)+ IT-(V)where the superscript + and -represent mT=1/2 and l11T=-1/2 . Here, we consider the transition of the spin states of polarized particles in fusion plasmas. Particles supplied into a plasma are assumed to be perfectly polarized in states mo=land mT=1/2. We are able to consider the fuel particle loss due to the D-T fusion reaction. The particle and the energy loss are expressed by using the confinement time dependent on the velocity of particles. The model equation is given by:The first term of R. H . S. represents the Coulomb collision term . The second term describes the particle loss from unit volume in velocity space due to the heat conduction. The third and fourth term, i. e., 5,7 (v )and L; (v), indicate the source and the loss of a species particles in real space due to the particle injection, the nuclear reaction and the convection of particles, respectively. 376Since the fusion reaction cross-sections are different depending on the spin states of D and T, it is neccesary to modify the description of the fusion reactivity. When deuterons with the magnetic quantum number A react with tritons which have /1, the thermonuclear reactivity ( The thermonuclear reactivity for a polarized plasma with no depolarization is 1.5 times as large as the one for unpolarized plasma. Due to the depolarization mechanisms in the plasma the reactivity decreases to some extent. We will calculate the decrement of the reactivity 17 defined as respectively. In all cases, when bB is smaller than 10.5 T, the polarization and the alignment are kept unity. On the other hand, the ...

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Spin Polarization Effect on Ignition Access Condition for D-T and D-³He Tokamak Fusion Reactors

Cited by 11 publications

References 25 publications

Realizing "2001: A Space Odyssey": Piloted Spherical Torus Nuclear Fusion Propulsion

Realizing "2001: A Space Odyssey": Piloted Spherical Torus Nuclear Fusion Propulsion

D-3He tokamak reactor with inductive a.c. and unidirectional current operation

Velocity distribution functions and reactivity of D–T fusion plasma with spin-polarized fuel

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Spin Polarization Effect on Ignition Access Condition for D-T and D-3He Tokamak Fusion Reactors

Cited by 11 publications

References 25 publications

Realizing "2001: A Space Odyssey": Piloted Spherical Torus Nuclear Fusion Propulsion

Realizing "2001: A Space Odyssey": Piloted Spherical Torus Nuclear Fusion Propulsion

D-3He tokamak reactor with inductive a.c. and unidirectional current operation

Velocity distribution functions and reactivity of D–T fusion plasma with spin-polarized fuel

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Product

Resources

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Spin Polarization Effect on Ignition Access Condition for D-T and D-³He Tokamak Fusion Reactors