Polymer and Cell Dynamics: Multiscale Modeling and Numerical by Prof. Dr. Wolfgang Alt, Prof. Dr. Mark Chaplain, Prof. Dr.

Polymer and Cell Dynamics: Multiscale Modeling and Numerical by Prof. Dr. Wolfgang Alt, Prof. Dr. Mark Chaplain, Prof. Dr.

By Prof. Dr. Wolfgang Alt, Prof. Dr. Mark Chaplain, Prof. Dr. Michael Griebel (auth.), Prof. Dr. Wolfgang Alt, Prof. Dr. Mark Chaplain, Prof. Dr. Michael Griebel, Dr. Jürgen Lenz (eds.)

Polymer and mobile dynamics play a huge position in procedures like tumor progress, metastasis, embryogenesis, immune reactions and regeneration. This quantity – in line with a world workshop on numerical simulations of polymer and cellphone dynamics in undesirable Honnef (Germany) in 2000 – offers an summary of the proper mathematical and numerical equipment, their functions and boundaries. The contributions are from the fields of utilized and numerical arithmetic, medical computing, theoretical physics, molecular biophysics, mobilephone and molecular biology in addition to chemical and biomedical engineering. the quantity could be of curiosity to scientists and complex undergraduates within the fields of biotechnology, biomedicine, utilized arithmetic, biomathematics, biophysics and bioinformatics.

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Extra resources for Polymer and Cell Dynamics: Multiscale Modeling and Numerical Simulations

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The first contribution by Rzehak, Arend, Kienle & Zimmermann uses a simplified 'bead-spring' model in order to simulate the dynamics of flexible polymer chains that are tethered at one end and are exposed to an outer hydrodynamic flow. Model beads representing a coarse-grained discretization of the elastic polymer chain are connected by (nonlinear) springs. After adding hydrodynamic interactions (for an approximating steady state) and by regarding a non-overlap condition for the polymer beads, the resulting stochastic multipartic1e system of Langevin type is appropriate to answer the two basic questions of interest: how does the outer flow deform the polymer chains, and, how does their motion alter the flow pattern.

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