Figure 10.

Dependences of the order parameter of the vector P (a) and density (b) of the given nanocomposites based on ODPA-P3 for the different description of the van der Waals energy in the form of the Lennard–Jones $U_{L-J}\left(r_{ij}\right)$ and Weeks–Chandler–Anderson $W\left(r_{ij}\right)$ potentials; (с) distribution of the orientation angles $\theta$ between the vector P and CNT surface for the Weeks–Chandler–Anderson potential at T = 580 K after the 1-µs simulation.