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\@writefile{los}{\l@slide {1}{\ignorespaces Molecular models - two particle system}{2}}
\@writefile{los}{\l@slide {2}{\ignorespaces Molecular models - many particle systems}{3}}
\@writefile{los}{\l@slide {3}{\ignorespaces The relation of the microscopic and the macroscopic level}{4}}
\@writefile{los}{\l@slide {4}{\ignorespaces Statistical mechanics}{5}}
\@writefile{los}{\l@slide {5}{\ignorespaces Molecular dynamics simulation}{6}}
\@writefile{los}{\l@slide {6}{\ignorespaces Monte Carlo simulations}{7}}
\@writefile{los}{\l@slide {7}{\ignorespaces Monte Carlo simulations}{8}}
\@writefile{los}{\l@slide {8}{\ignorespaces Monte Carlo simulations}{9}}
\@writefile{los}{\l@slide {9}{\ignorespaces Monte Carlo simulations}{10}}
\@writefile{los}{\l@slide {10}{\ignorespaces Periodic boundary condition}{11}}
\@writefile{los}{\l@slide {11}{\ignorespaces Mixed boundary conditions}{12}}
\@writefile{los}{\l@slide {12}{\ignorespaces Problems with large scale MD simulations}{13}}
\@writefile{los}{\l@slide {13}{\ignorespaces Problems with large scale MD simulations}{14}}
\@writefile{los}{\l@slide {14}{\ignorespaces Continuum models}{15}}
\@writefile{los}{\l@slide {15}{\ignorespaces Macroscopic electrostatics}{16}}
\@writefile{los}{\l@slide {16}{\ignorespaces Variational formalism}{17}}
\@writefile{los}{\l@slide {17}{\ignorespaces Solution of the extremum condition}{18}}
\@writefile{los}{\l@slide {18}{\ignorespaces Point charges as source charges}{19}}
\@writefile{los}{\l@slide {19}{\ignorespaces Sharp dielectric interfaces}{20}}
\@writefile{los}{\l@slide {20}{\ignorespaces The matrix equation}{21}}
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\@writefile{los}{\l@slide {21}{\ignorespaces The matrix equation}{22}}
\@writefile{los}{\l@slide {22}{\ignorespaces Calculation of the integral}{23}}
\@writefile{los}{\l@slide {23}{\ignorespaces Calculation of the energy}{24}}
\@writefile{los}{\l@slide {24}{\ignorespaces Ion is modelled as a hard sphere with a point charge in the center}{25}}
\@writefile{los}{\l@slide {25}{\ignorespaces One flat interface: $\varepsilon _{1} | \varepsilon _{2}$ geometry - ions on the right side}{26}}
\@writefile{los}{\l@slide {26}{\ignorespaces Two flat interfaces: $\varepsilon _{1} | \varepsilon _{2} | \varepsilon _{3}$ geometry - electrical double layer}{27}}
\@writefile{los}{\l@slide {27}{\ignorespaces A dielectric sphere $\varepsilon _{1}=80$ embedded in a dielectric $\varepsilon _{2}=2$}{28}}
\@writefile{los}{\l@slide {28}{\ignorespaces The effective force acting between two charged dielectric spheres}{30}}
\@writefile{los}{\l@slide {29}{\ignorespaces MC simulation for a model calcium channel}{31}}
\@writefile{los}{\l@slide {30}{\ignorespaces MC simulation for a model calcium channel}{32}}
\@writefile{los}{\l@slide {31}{\ignorespaces Preliminary results for inhomogeneous dielectric}{33}}
\@writefile{los}{\l@slide {32}{\ignorespaces Problem of absence of charge neutral bulk}{36}}
\@writefile{los}{\l@slide {33}{\ignorespaces Simulation by imposing Dirichlet or Neumann boundary conditions}{37}}
\@writefile{los}{\l@slide {34}{\ignorespaces Coupling induced and electrode charge calculations}{38}}
\@writefile{los}{\l@slide {35}{\ignorespaces Acknowledgement}{39}}