Worm-like chain (O'Brien) ========================================================= A second worm-like chain implementation, :class:`~afrc.polymer_models.wlc2.WormLikeChain2`, using the closed form of O'Brien et al. (2009). It is conceptually equivalent to the :doc:`Zhou model ` but is numerically better behaved at large contour lengths and additionally provides a closed-form radius of gyration. Mathematical formalism --------------------------------------------------------- With contour length :math:`L_c = N b` and :math:`\alpha = 3 L_c / (4 L_p)`, the end-to-end distribution is .. math:: P(r) = \frac{4\pi C_1\, r^2}{L_c \left(1 - (r/L_c)^2\right)^{9/2}} \exp\!\left( -\frac{3 L_c}{4 L_p \left(1 - (r/L_c)^2\right)} \right), where the normalisation constant is .. math:: C_1 = \left[ \pi^{3/2} e^{-\alpha} \alpha^{-3/2} \left( 1 + 3\alpha^{-1} + \tfrac{15}{4}\alpha^{-2} \right) \right]^{-1}. The :math:`\left(1 - (r/L_c)^2\right)` factors enforce finite extensibility (:math:`r < L_c`). The radius of gyration is given in closed form (with :math:`C_2 = 1/(2 L_p)`): .. math:: \langle R_g^2 \rangle = \frac{L_c}{6 C_2} + \frac{1}{4 C_2^2} + \frac{1}{4 C_2^3 L_c} - \frac{1 - e^{-L_c/L_p}}{8 C_2^4 L_c^2}, and :meth:`get_mean_radius_of_gyration` returns :math:`\sqrt{\langle R_g^2 \rangle}`. Parameters --------------------------------------------------------- .. list-table:: :header-rows: 1 :widths: 20 15 65 * - Parameter - Default - Meaning and typical values * - ``lp`` - 3.0 Å - Persistence length (chain stiffness). As for the Zhou model, 3-5 Å is typical for unfolded polypeptides; larger values give a stiffer, more extended chain. * - ``aa_size`` - 3.8 Å - Segment length :math:`b` (Cα-Cα distance); sets the contour length :math:`L_c = N b`. The constructor additionally requires the sequence to be at least as long as the persistence length (:math:`N \ge L_p`); otherwise a ``WLC2Exception`` is raised. **What to expect for a protein.** Results closely track the Zhou model for typical disordered-protein parameters, with the practical advantages of numerical stability for long chains and a directly available :math:`R_g`. Citations --------------------------------------------------------- 1. O'Brien, E. P., Morrison, G., Brooks, B. R., & Thirumalai, D. (2009). How accurate are polymer models in the analysis of Förster resonance energy transfer experiments on proteins? *The Journal of Chemical Physics*, 130(12), 124903. 2. Rubinstein, M., & Colby, R. H. (2003). *Polymer Physics*. Oxford University Press.