scholarly journals Remarks on the Motility and Thermotactic Response of Fibroblasts

1983 ◽  
Vol 36 (5) ◽  
pp. 707
Author(s):  
WC Parkinson

The motion of mouse L cells (fibroblast) in vitro is studied by means of time-lapse photography. In particular, the response of the cells to a temperature gradient of7� 22�Ccm-1 is studied for several temperatures from 32� 6�C to 39� 7�C. Three measures of the thermotactic response are used: (1) the motility, defined in terms of the mean-square displacement of an ensemble of cells, (2) the displacement of the centre of gravity of an ensemble of cells versus time, and (3) the distribution in the number of cells in an ensemble moving up the gradient compared with the number moving down the gradient. There is no evidence of a thermotactic response as determined by these three measures. The variance in the data can be understood in terms of statistical fluctuations.

Fluids ◽  
2021 ◽  
Vol 6 (3) ◽  
pp. 111
Author(s):  
Leonid M. Ivanov ◽  
Collins A. Collins ◽  
Tetyana Margolina

Using discrete wavelets, a novel technique is developed to estimate turbulent diffusion coefficients and power exponents from single Lagrangian particle trajectories. The technique differs from the classical approach (Davis (1991)’s technique) because averaging over a statistical ensemble of the mean square displacement (<X2>) is replaced by averaging along a single Lagrangian trajectory X(t) = {X(t), Y(t)}. Metzler et al. (2014) have demonstrated that for an ergodic (for example, normal diffusion) flow, the mean square displacement is <X2> = limT→∞τX2(T,s), where τX2 (T, s) = 1/(T − s) ∫0T−s(X(t+Δt) − X(t))2 dt, T and s are observational and lag times but for weak non-ergodic (such as super-diffusion and sub-diffusion) flows <X2> = limT→∞≪τX2(T,s)≫, where ≪…≫ is some additional averaging. Numerical calculations for surface drifters in the Black Sea and isobaric RAFOS floats deployed at mid depths in the California Current system demonstrated that the reconstructed diffusion coefficients were smaller than those calculated by Davis (1991)’s technique. This difference is caused by the choice of the Lagrangian mean. The technique proposed here is applied to the analysis of Lagrangian motions in the Black Sea (horizontal diffusion coefficients varied from 105 to 106 cm2/s) and for the sub-diffusion of two RAFOS floats in the California Current system where power exponents varied from 0.65 to 0.72. RAFOS float motions were found to be strongly non-ergodic and non-Gaussian.


1991 ◽  
Vol 46 (7) ◽  
pp. 616-620 ◽  
Author(s):  
Junko Habasaki

MD simulation has been performed to learn the microscopic mechanism of diffusion of ions in the Li2SiO3 system. The motion of lithium ions can be explained by the trapping model, where lithium is trapped in the polyhedron and moves with fluctuation of the coordination number. The mean square displacement of lithium was found to correlate well with the net changes in coordination number.


1994 ◽  
Vol 08 (24) ◽  
pp. 3411-3422 ◽  
Author(s):  
W. SCHOMMERS

The effect of premelting is of particular interest in connection with the theory of melting. In this paper, we discuss the structural and dynamical properties of the surfaces of semi-infinite crystals as well as of nano-clusters, which show the effect of premelting. The investigations are based on molecular-dynamics calculations: different models are used for the systematic study of the effect of premelting. In particular, the behaviour of the following functions have been studied: pair correlation function, generalized phonon density of states, and the mean-square displacement as a function of time. The calculations have been done for krypton since for this substance a reliable interaction potential is available.


2018 ◽  
Vol 32 (19) ◽  
pp. 1850210
Author(s):  
Chun-Yang Wang ◽  
Zhao-Peng Sun ◽  
Ming Qin ◽  
Yu-Qing Xu ◽  
Shu-Qin Lv ◽  
...  

We report, in this paper, a recent study on the dynamical mechanism of Brownian particles diffusing in the fractional damping environment, where several important quantities such as the mean square displacement (MSD) and mean square velocity are calculated for dynamical analysis. A particular type of backward motion is found in the diffusion process. The reason of it is analyzed intrinsically by comparing with the diffusion in various dissipative environments. Results show that the diffusion in the fractional damping environment obeys the Langevin dynamics which is quite different form what is expected.


1977 ◽  
Vol 44 (3) ◽  
pp. 487-491 ◽  
Author(s):  
S. F. Masri ◽  
F. Udwadia

The transient mean-square displacement, slope, and relative motion of a viscously damped shear beam subjected to correlated random boundary excitation is presented. The effects of various system parameters including the spectral characteristics of the excitation, the delay time between the beam support motion, and the beam damping have been investigated. Marked amplifications in the mean-square response are shown to occur for certain dimensionless time delays.


2019 ◽  
Vol 2019 ◽  
pp. 1-5
Author(s):  
Long Shi

In this work, a generalization of continuous time random walk is considered, where the waiting times among the subsequent jumps are power-law correlated with kernel function M(t)=tρ(ρ>-1). In a continuum limit, the correlated continuous time random walk converges in distribution a subordinated process. The mean square displacement of the proposed process is computed, which is of the form 〈x2(t)〉∝tH=t1/(1+ρ+1/α). The anomy exponent H varies from α to α/(1+α) when -1<ρ<0 and from α/(1+α) to 0 when ρ>0. The generalized diffusion equation of the process is also derived, which has a unified form for the above two cases.


Author(s):  
Ali Khalili Golmankhaneh ◽  
Saleh Ashrafi ◽  
Dumitru Baleanu ◽  
Arran Fernandez

AbstractIn this paper, we have investigated the Langevin and Brownian equations on fractal time sets using Fα-calculus and shown that the mean square displacement is not varied linearly with time. We have also generalized the classical method of deriving the Fokker–Planck equation in order to obtain the Fokker–Planck equation on fractal time sets.


1964 ◽  
Vol 206 (1) ◽  
pp. 83-88 ◽  
Author(s):  
S. O. Raab ◽  
J. W. Athens ◽  
O. P. Haab ◽  
D. R. Boggs ◽  
H. Ashenbrucker ◽  
...  

Dog granulocytes were labeled in vitro with radioactive diisopropylfluorophosphate (DFP32) and then returned to the circulation of the donor. Granulocytes were separated from whole blood by utilizing hexadimethrine bromide as the sedimenting agent and saponin as a lysing agent. The labeled granulocytes disappeared from the circulation in an exponential fashion with a mean (±1 sd) half-time disappearance of 5.6 ± 0.95 hr. The size of the total blood granulocyte ( TBGP), circulating granulocyte ( CGP), and marginal granulocyte ( MGP) pools, and the granulocyte turnover rate ( GTR) were measured in 31 normal, unanesthetized dogs. The mean values ± 1 sd, expressed as number of cells x107/kg body wt., were as follows: TBGP, 102 ± 34.8; CGP, 54 ± 20.7; MGP, 48 ± 23.4; and GTR, 305 ± 111.5 cells/kg day. The values observed in anesthetized and in unanesthetized, splenectomized dogs were not significantly different from the above values.


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