. Author manuscript; available in PMC: 2022 Mar 1.

Published in final edited form as: Acta Biomater. 2020 Dec 28;122:263–277. doi: 10.1016/j.actbio.2020.12.043

Table II:

Thermodynamic free energy functions for mechanical deformation of P22, HAdV, and HSV shells, calculated using the values of FNS model parameters (from Table I): free energies for Hertzian deformation $Δ G_{H}$ , bending deformation $Δ G_{b}$ , and plastic deformation $Δ G_{p}$ , obtained with Eqs. (12), and the free energy for particle fracture $Δ G_{f}$ . The values of $Δ G_{f}$ obtained using Eq. (15) and by performing the numerical integration of the average experimental FX-spectra are separated by the slash.

Particle	Thermodynamic state functions
Particle	$Δ G_{H}$ , MJ/mol	$Δ G_{b}$ , MJ/mol	$Δ G_{p}$ , MJ/mol	$Δ G_{f}$ , MJ/mol
P22 Procapsid	0.03	0.92	0.57	1.52/1.45
P22 Expanded	0.07	1.11	1.02	2.22/2.3
HAdV weak	0.40	2.00	3.30	5.70/5.90
HAdV strong	1.20	5.10	8.80	14.8/14.4
HSV	0.71	4.90	6.89	12.8/12.4