. 2017 Dec 1;13(12):e1005866. doi: 10.1371/journal.pcbi.1005866

Table 4. Quantifying the wall velocities $v_{w}^{i j}$ from our fits of $L_{s}^{i j}$ by using $L_{s}^{i j} = D_{w} / (v_{w}^{i j})^{2}$ and an independently measured D_w which was constant between experiments.

The uncertainty in $v_{w}^{i j}$ from the fit $L_{s}^{i j}$ was calculated via error propagation.

Strain i	Strain j	$L_{s}^{i j} (m m)$ : fitting F_ij	$v_{w}^{i j}$ : from fit $L_{s}^{i j}$	$v_{w}^{i j}$ : tracking sectors
eYFP/eCFP	mCherry	13 ± 3	(9 ± 1) × 10⁻²	(6 ± 2) × 10⁻²
Black	mCherry	25 ± 7	(6 ± 1) × 10⁻²	(6 ± 2) × 10⁻²
eYFP/eCFP	Black	70 ± 20	(3.8 ± 0.7) × 10⁻²	Undetectable

Table 4. Quantifying the wall velocities vwij from our fits of Lsij by using Lsij=Dw/(vwij)2 and an independently measured Dw which was constant between experiments.