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Chain Folding Conformation

The tendency of polymer chains to fold and entangle due to steric hindrance and attractive forces, influencing material properties.
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The statement of the theorem

Let r=(r1,r2,,rN)\mathbf{r} = (\mathbf{r}_1, \mathbf{r}_2, \dots, \mathbf{r}_N) be the set of spatial coordinates defining the conformation of a polymer chain of NN monomers. The equilibrium conformation minimizes the total free energy functional F(r)F(\mathbf{r}): \begin{equation*} F(\mathbf{r}) = E_{internal}(\mathbf{r}) + E_{interaction}(\mathbf{r}) - T S(\mathbf{r}) \end{equation*} The internal energy EinternalE_{internal} includes bond stretching and angle bending potentials, while EinteractionE_{interaction} accounts for non-bonded forces (e.g., Lennard-Jones potential VLJV_{LJ}): \begin{equation*} E_{interaction}(\mathbf{r}) = \sum_{ir0\mathbf{r}_0 is the state that minimizes FF: r0=argminrF(r)\mathbf{r}_0 = \arg\min_{\mathbf{r}} F(\mathbf{r}). The folding tendency is quantified by the free energy difference ΔF=F(r0)F(rrandom)\Delta F = F(\mathbf{r}_0) - F(\mathbf{r}_{random}).