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. 2016 Nov 30;292(3):955–966. doi: 10.1074/jbc.M116.760371

TABLE 2.

Kinetic parameters extrapolated to 0 m for all FNIII domains studied

FNIII 2C* and FNIII 9C* were fit by a more complex model (Equation 13).

FNII domain kop kcl mop mcl ΔG meq kchem KopL
s−1 s−1 m1 m1 kcal mol1 kcal mol1 m1 m1 s1
2C* 2.7 × 10−4 (1 × 10−5) 4.8 (0.2) 1.1 (0.008) −0.65 (0.01) 5.9 (0.04) −1.1(0.008) 1,700 (2) 3.2 × 10−5 (7 × 10−7)
3C 1.9 × 10−3 (2 × 10−5) 0.55 (0.01) 1.5 (0.007) −0.78 (0.01) 3.4 (0.01) −1.4 (0.006) 2,100 (2)
6C 1.3 × 10−5 (1 × 10−7) 0.14 (0.003) 1.5 (0.002) −0.20 (0.006) 5.6 (0.02) −1.0 (0.002) 2,200 (2)
7 6.9 × 10−5 (4 × 10−7) 1.4 (0.01) 0.95 (0.001) −1.2 (0.002) 5.9 (0.007) −1.3 (0.008) 1,200 (0.3)
9C* 3 × 10−5 (4 × 10−7) 0.015 (0.0003) 1.2 (0.004) −0.53 (0.006) 3.7 (0.01) −1.0 (0.004) 12,000 (40) 2.7 × 10−4 (1 × 10−6)
11C 0.016 (2 × 10−4) 0.06 (0.001) 1.8 (0.02) −0.93 (0.04) 0.78 (0.02) −1.6 (0.001) 1,400 (2)
12C 2.3 × 10−4 (1 × 10−6) 0.3 (0.005) 1.1 (0.003) −1.3 (0.006) 4.3 (0.01) −1.5 (0.003) 3,700 (3)
Irisin 2.1 × 10−3 (1 × 10−5) 1.9 (0.01) 0.72 (0.002) −1.7 (0.004) 4.1 (0.005) −1.4 (0.008) 5,200 (5)
TNfn3 6 × 10−3 (1 × 10−4) 0.72 (0.02) 0.55 (0.008) −2 (0.02) 2.9 (0.02) −1.5 (0.01) 6,200 (6)