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. 2003 Nov 14;100(24):13934–13939. doi: 10.1073/pnas.2232868100

Table 1. Some basic properties of the eight simulations.

System Tm, K v, 300 K w, 300 K ΔH, kcal/mol ΔS, cal/mol per K ΔCv, cal/mol per K
A21 in TIP3P (parm94) 361 (14) 0.30 (0.02) 1.68 (0.04) -0.23 (0.21) 0.20 (0.5) -10.9 (1.6)
Fs in TIP3P (parm94) 393 (20) 0.27 (0.05) 2.12 (0.18) -0.72 (0.13) -0.9 (0.4) -4.0 (1.1)
A21 in TIP3P(parm-mod) 258 0.059 (0.006) 1.12 (0.01) -0.58 (0.06) -1.7 (0.2) 0.2 (1.0)
Fs in TIP3P (parm-mod) 342 (8) 0.13 (0.03) 1.67 (0.10) -0.88 (0.15) -2.0 (0.5) 1.2 (1.3)
A21 in GB/SA (parm94) 399 (6) 0.89 (0.02) 3.25 (0.03) -1.39 (0.01) -2.36 (0.03) 0.0 (0.1)
Fs in GB/SA (parm94) 380 (5) 0.79 (0.02) 2.20 (0.03) -0.47 (0.01) -0.02 (0.04) -4.2 (0.3)
A21 in GB/SA (parm-mod) 432 (3) 1.63 (0.08) 4.63 (0.16) -1.48 (0.01) -0.02 (0.04) -4.2 (0.3)
Fs in Gb/SA (parm-mod) 431 (2) 1.57 (0.07) 4.03 (0.12) -1.23 (0.02) -1.56 (0.04) -4.5 (0.02)

Tm is the denaturation temperature measured as the temperature at which half of the possible native α-helical hydrogen bonds are formed. v is the Lifson—Roig helix nucleation parameter at 300 K (smaller values indicate a large nucleation penalty). w is the Lifson—Roig helix propagation parameter at 300 K. ΔH, ΔS, and ΔCv are the energy, entropy, and heat capacity changes, respectively, for helix formation on a per-residue basis found by fitting the variation of w with temperature as described in Methods.