Citation
Griffel, David Henry (1968) The Kinetic Theory of the Solar Wind and its Interaction with the Moon. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/DH61ZQ91. https://resolver.caltech.edu/CaltechETD:etd09202008111601
Abstract
NOTE: Text or symbols not renderable in plain ASCII are indicated by [...]. Abstract is included in .pdf document.
Beyond about .1 A.U. from the sun, fluid mechanics is not a good approximation for the solar wind, because the collision frequency is low. Analysis of the particle dynamics shows that if there are no collisions beyond .1 A.U., then at the earth T[...]/T[...] = 35; this is much greater than is observed. We study the effects of interactions by means of the Boltzmann equation. Solving it with Krook's collision term, we find that the temperature anisotropy observed by the Vela satellite requires each particle to make an average of 2 or 3 collisions between .1 and 1 A.U. The temperature averaged over direction roughly follows an adiabatic law, with γ = 3/2; γ tends to increase with distance. The theory predicts an excess of highvelocity particles, as is observed by Vela, even when the collision frequency is independent of velocity; but to produce an effect as strong as that observed requires a fairly strong velocitydependence of the collision frequency.
We proceed to study the interaction of the wind with the moon, treated as a solid body, with neither magnetic field nor atmosphere, absorbing and neutralizing all incident particles. We construct an exact theory of the boundary layer between such a body and a plasma with a magnetic field parallel to the surface, valid when the plasma has no velocity towards the surface. The thickness of the layer is about two gyroradii, and the magnetic field rises across it according to the equation of pressure balance.
We then consider twodimensional models of the complete windplanet interaction, and show that in any steady twodimensional flow, the plasma velocity must be tangential to the body. Then, using the model of the sheath constructed above, we show that there can be no steady flow at all around a finitely conducting cylinder.
Finally, we consider the magnetic fields induced by the interplanetary field inside the moon, taking account of its rotation. If the applied field is uniform, then in the steady state there is a constant axial field inside the sphere; near the surface there is a complex toroidal field, dying away to zero in the interior if the sphere is spinning rapidly. If the external field is nonuniform, there is a residual toroidal field throughout the sphere. If the diffusion time is longer than the time between reversals of the interplanetary field, then the moon will contain concentric shells of toroidal and axial fields, independently diffusing inwards.
Item Type:  Thesis (Dissertation (Ph.D.)) 

Subject Keywords:  (Physics) 
Degree Grantor:  California Institute of Technology 
Division:  Physics, Mathematics and Astronomy 
Major Option:  Physics 
Thesis Availability:  Public (worldwide access) 
Research Advisor(s): 

Thesis Committee: 

Defense Date:  18 December 1967 
Record Number:  CaltechETD:etd09202008111601 
Persistent URL:  https://resolver.caltech.edu/CaltechETD:etd09202008111601 
DOI:  10.7907/DH61ZQ91 
Default Usage Policy:  No commercial reproduction, distribution, display or performance rights in this work are provided. 
ID Code:  3673 
Collection:  CaltechTHESIS 
Deposited By:  Imported from ETDdb 
Deposited On:  06 Nov 2008 
Last Modified:  02 Apr 2024 17:54 
Thesis Files

PDF (Griffel_dh_1968.pdf)
 Final Version
See Usage Policy. 3MB 
Repository Staff Only: item control page