🗊Презентация Physics of fusion power. Collisions / Transport (Lecture 14)

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Physics of fusion power. Collisions / Transport (Lecture 14), слайд №1Physics of fusion power. Collisions / Transport (Lecture 14), слайд №2Physics of fusion power. Collisions / Transport (Lecture 14), слайд №3Physics of fusion power. Collisions / Transport (Lecture 14), слайд №4Physics of fusion power. Collisions / Transport (Lecture 14), слайд №5Physics of fusion power. Collisions / Transport (Lecture 14), слайд №6Physics of fusion power. Collisions / Transport (Lecture 14), слайд №7Physics of fusion power. Collisions / Transport (Lecture 14), слайд №8
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Слайд 1


Physics of fusion power Lecture 14: Collisions / Transport
Описание слайда:
Physics of fusion power Lecture 14: Collisions / Transport

Слайд 2


Collisions Coulomb interaction between electrons and ions leads to the scattering of particles -> Collisions Interaction occurs only within the Debye sphere The angle of deflection depends on how close the particles are approaching each other.
Описание слайда:
Collisions Coulomb interaction between electrons and ions leads to the scattering of particles -> Collisions Interaction occurs only within the Debye sphere The angle of deflection depends on how close the particles are approaching each other.

Слайд 3


Small / Large angle scattering Deflection depends on how close the particles approach each other For a given time a particle moving through the plasma will collide with all particles in a cylinder For large angle scattering collisions the distance must be small and so is the radius of the cylinder For small angle scattering collisions the radius is much larger It turns out that small angle scattering collisions dominate
Описание слайда:
Small / Large angle scattering Deflection depends on how close the particles approach each other For a given time a particle moving through the plasma will collide with all particles in a cylinder For large angle scattering collisions the distance must be small and so is the radius of the cylinder For small angle scattering collisions the radius is much larger It turns out that small angle scattering collisions dominate

Слайд 4


Many body problem The plasma has some 1022 particles. No description is possible that allows for the determination of position and velocity of all these particles Only averaged quantities can be described. The evolution of the averaged velocity is however influenced by a microscopic process : the collisions Each collision can have a different outcome depending on the unknown initial conditions
Описание слайда:
Many body problem The plasma has some 1022 particles. No description is possible that allows for the determination of position and velocity of all these particles Only averaged quantities can be described. The evolution of the averaged velocity is however influenced by a microscopic process : the collisions Each collision can have a different outcome depending on the unknown initial conditions

Слайд 5


Diffusion of the velocity direction
Описание слайда:
Diffusion of the velocity direction

Слайд 6


Diffusion of the velocity Diffusion coefficient Define a function that determines the number of particles moving in a direction given by the angle  Collisions lead to a diffusion in the angle described by
Описание слайда:
Diffusion of the velocity Diffusion coefficient Define a function that determines the number of particles moving in a direction given by the angle  Collisions lead to a diffusion in the angle described by

Слайд 7


Transport in a homogeneous magnetic field Particles undergo scattering. The diffusion coefficient Typical step size is the Larmor radius, typical time the collision frequency
Описание слайда:
Transport in a homogeneous magnetic field Particles undergo scattering. The diffusion coefficient Typical step size is the Larmor radius, typical time the collision frequency

Слайд 8


Transport in a homogeneous magnetic field Typical values for a reactor The particles satisfy a diffusion equation
Описание слайда:
Transport in a homogeneous magnetic field Typical values for a reactor The particles satisfy a diffusion equation

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