Sentence examples for a function of filament from inspiring English sources

Fig. 5 explores the PAIRS coefficient dependence on time-step and the method accuracy as a function of filament length and external force.

We have analyzed our data as a function of filament length.

(A ) Cross correlation curves and corresponding single exponential fits for the data as a function of R ecA filament length of the non-homologous dsDNA interaction with RecA filament changes as a function of filament length.

(I J ) The change in length, Δ L, as a function of time for a filament tether to the surface using VASP at (I ) low (18.2 molecules/μm or 0.1 molecules per micron of filament) or (J ) high (18,200 molecules/μm or 100 molecules per micron of filament) surface density.

(A B ) The change in length, Δ L, as a function of time for a filament tether to the surface using α-actinin at (A ) low (16.7 molecules/μm or 0.1 molecules per micron of filament) or (B ) high (16,700 molecules/μm or 100 molecules per micron of filament) surface densities.

(E F ) The change in length, Δ L, as a function of time for a filament tether to the surface using NEM-myosin at (E ) low (6.8 molecules/μm or 0.04 molecules per micron of filament) or (F ) high (6800 molecules/μm or 40 molecules per micron of filament) surface densities.

(M N ) The change in length, Δ L, as a function of time for a filament tether to the surface using VASP ΔGAB at (M ) low (18.5 molecules/μm or 0.1 molecules per micron of filament) or (N ) high (18,500 molecules/μm or 100 molecules per micron of filament) surface density.

In the absence of filament turnover, the contraction velocity increases as a function of time because an increasing filament density leads to higher stress.

(C ) Δ L as a function of time for single filaments grown on surfaces with different tethering proteins.

Breakdown voltage (VB) for various ratios of argon-nitrogen as a function of pd in the absence of filament.

Measurements of filament elongation as a function of solution viscosity (Drenckhahn and Pollard, 1986) and particle-analysis from cryo-electron microscopy (Narita et al., 2011) suggest the existence of a non-elongating state at the pointed-end.