THESIS
2018
xii, 58 pages : illustrations (some color) ; 30 cm
Abstract
We systematically studied the potential landscapes of colloidal diffusion systems using
the Markov State Model. The potential landscapes includes simulated 1D, 2D, periodical
and random potentials, and experimental 2D periodical and random potentials. Robust
Perron clustering analysis (PCCA+) identified potential traps successfully. The height
of the energy barrier between traps was obtained from the transition rate matrix. The
distribution of the height of energy barriers agreed well with that from the Boltzmann
distribution of a direct population probability histogram. We were able to evaluate the
barrier height with reasonable accuracy without sampling the trajectory at the peak of the
barrier directly.
The free diffusion of proteins on live cell membranes is modulated by th...[
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We systematically studied the potential landscapes of colloidal diffusion systems using
the Markov State Model. The potential landscapes includes simulated 1D, 2D, periodical
and random potentials, and experimental 2D periodical and random potentials. Robust
Perron clustering analysis (PCCA+) identified potential traps successfully. The height
of the energy barrier between traps was obtained from the transition rate matrix. The
distribution of the height of energy barriers agreed well with that from the Boltzmann
distribution of a direct population probability histogram. We were able to evaluate the
barrier height with reasonable accuracy without sampling the trajectory at the peak of the
barrier directly.
The free diffusion of proteins on live cell membranes is modulated by the local cellular
context both inside and outside the cell. We used an extra-cellular pattern of microgrooves
to control the spatial distribution of adhesion complexes on the basal membrane of muscle
cells, and evaluated the effects of this topographic patterning on the diffusion dynamics
of AChRs. Along the microgroove direction (the x direction), the motion is the same
as the anomalous diffusion without the pattern, which can be explained by the dynamic
heterogeneity of the diffusion coefficient. In the direction perpendicular to the microgrooves
( the y direction), the motion is hindered and can be modeled as a diffusion with non-constant
diffusion coefficient over a 1D periodical potential. This diffusion guided along
the y direction is caused by the distribution of integrins.
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