. 2009 Nov 4;4(11):e7756. doi: 10.1371/journal.pone.0007756

Table 1. Polymer statistics of filaments adsorbed to different supports^a.

interaction	surface	s/L_P ^b	<s> [nm]	L_P(cos(Θ)) [nm]	<Θ⁴>/<Θ²>²	L_P(Θ²) [nm]	L_P(R²) [nm]	counts
Weak	glass	2–4	2620	990	2.9–3.1	980	1110	173
weak	glass	3–6	3630	1090	2.8–3.4	1100	1050	56
strong	mica	0.6–1.5	1020	336	2.5–2.7	350	445	55
strong	mica	2–4	2670	310	2.7–3.5	290	370	57
strong	mica	3–6	4050	330	3.2–4.3	180	320	57

For each support, we have computed the apparent persistence lengths from equations 4 to 8. The mean errors were less than 5% for all calculated persistence lengths.

Range of the selected length s of the filaments divided by the persistence length L_P (Assumption: full equilibrated).

Table 1. Polymer statistics of filaments adsorbed to different supportsa.

Table 1. Polymer statistics of filaments adsorbed to different supports^a.