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. 2020 Jun 22;117(27):15632–15641. doi: 10.1073/pnas.1916343117

Table 4.

Optical trap step kinetics and step displacement fit parameters

Step kinetics Step sizes
Motor [MgATP] Load, pN A1 k1, s−1 A2 k2, s−1 Aback μback, nm Aforward μforward, nm
KIF3AA 1 mM 1 pN hindering 1.0 18 0.04 −7.1 ± 4.8 0.96 8.7 ± 2.9
KIF3AA 1 mM 1 pN assisting 1.0 24 0.12 −11 ± 6.4 0.88 11 ± 5.5
KIF3CC 1 mM 1 pN hindering 0.61 6.6 0.39 0.6 0.39 −6.7 ± 5.2 0.61 7.8 ± 4.4
KIF3CC 1 mM 1 pN assisting 0.78 18 0.22 2.2 0.20 −9.8 ± 5.1 0.80 11 ± 7.5
KIF3AC 10 μM 1 pN hindering 1.0 5.9 0.35 −5.0 ± 7.2 0.65 7.8 ± 2.9
KIF3AC 1 mM 1 pN hindering 0.96 11 0.04 2.4 0.21 −7.4 ± 5.0 0.79 9.2 ± 4.5
KIF3AC 1 mM 1 pN assisting 0.88 24 0.12 2.7 0.27 −9.4 ± 7.4 0.73 11 ± 7.3

Dwell time distributions were fit by either a single exponential function or the sum of two exponential functions to determine step kinetics. Single exponential fit equation: y=k1ek1t and sum of two exponential functions fit equation: y=Ak1ek1t+(1A)k2ek2t, where the amplitude A is reported as A1 and (1 – A) is reported as A2. Amplitude and rate parameters are shown. Justification of a second exponential was determined by the log-likelihood ratio test. For KIF3CC, P < 1 × 10−16 at 1-pN hindering load, and P < 1 × 10−16 at 1-pN assisting load. For KIF3AC, P < 1 × 10−16 at 1-pN hindering load, and P < 1 × 10−16 at 1-pN assisting load. Step-size distributions were fit by the sum of two Gaussian distributions. Relative amplitudes are reported; step sizes are reported as means ± σ of the fit curve, where σ indicates the width of Gaussian peak and not uncertainty in peak position.