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Lipid aggregation can be well explained by the mutual repulsion of water and the
hydrocarbon chain that forms the hydrophobic tail of lipid amphiphiles.
Furthermore, Van-der-Waals interactions between the unpolar tails might be
important for micelle formation. Both repulsion and Van-der-Waals forces can be
expressed by pairwise potentials between the involved particles. The most common
potential function has been introduced by Lennard and Jones and reads ![]() ![]() Given the potentials of all particles, we use Netwon dynamics to model their motion. In addition, friction and thermic noise describe the medium in which particles move. This leads to an ordinary second order differential equation for each particle:
![]() whereby xi, vi denote position and velocity of particle i, mi its mass and Ui the potential with respect to the positions of other particles. γ is the friction coefficient of the medium, ξσ is a Gaussian distributed random vector. Particle motion is calculated by a stepwidth adaptive Euler approximation. In order to explore the kinetics of chemical reactions, the tool allows the user to define arbitry particles and reactions between them. After each timestep, reaction probabilities are determined for all pairs of reactants within a predefined critical range. These probabilities depend on particle distances as well as the distance of eventually present catalysts. If a reaction occurs, reactants are exchanged by products.
The program offers both visual and numerical output. The user can choose
analyses to perform from a wide palette of different observables like potential
and kinetic energy, particle numbers, micelle size distributions, a.s.o. |
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By introducing a metabolism in the system, we are able to study growth and splitting processes of micelles with respect to the underlying physics. The metabolism we explore uses precursers that can form either new lipids or catalysts. The catalyst enhances both its own creation and the creation of lipids. Both lipids and catalysts degrade to waste particles with a fixed, but small reaction rate. ![]() We start simulations with a small micelle that is charged with some catalyst and exposed to a solution of precursors. While time passes, precursors diffuse into the micelle and are transformed into new lipids and catalysts leading to micelle growth. When reaching a certain threshold size, micelles may become unstable and finally split. One of our aims is to study the impact of the underlying physics on this micelle division. |
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As pointed out by David W. Deamer and Daniel Segré catalytic lipids (so-called lipozymes) might have played an important role for the emergence of early life. If one defines life as a set of chemical reactions which is able to undergo natural selection, then the most simple organisms to imagine whould probably be micelles consisting of auto- and self-catalytic lipozymes only.
In these simulations we will explore the interplay of different lipozymes, that construct a catalytic network. We will study the relation between the structure of the catalytic network and the composition of micelles that will emerge. Using the detailed approach of molecular dynamics for these examinations allows the study of spatial patterns in the resulting dynamics. |