Impulse response function for Brownian motion

نویسندگان

چکیده

Motivated from the central role of mean-square displacement and its second time-derivative -- that is velocity autocorrelation function $\left\langle v(0)v(t)\right\rangle=\frac{1}{2} \frac{\mathrm{d}^{2} \left\langle \Delta r^{2} (t)\right\rangle}{\mathrm{d}t^{2}} $ in description Brownian motion, we revisit physical meaning first particles. By employing a rheological analogue for show $\frac{\mathrm{d}\left\langle (t) \right\rangle}{\mathrm{d}t}$ microspheres with mass $m$ radius $R$ immersed any linear, isotropic viscoelastic material identical to $\frac{N K_B T}{3 \pi R}h(t)$, where $h(t)$ impulse response network parallel connection linear an inerter distributed inertance $m_R=\frac{m}{6 R}$. The $h(t)=\frac{3\pi R}{N T}\frac{\mathrm{d}\left\langle material-inerter derived this paper at stress-strain level essentially $\chi(t)=\frac{h(t)}{6\pi R}$ particles expressed force-displacement by Nishi \textit{et al.} (2018). derive time-derivatives described Maxwell element connected dashpot which captures high-frequency viscous behavior motion such fluid-like soft matter function, maintains finite constant value long term.

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ژورنال

عنوان ژورنال: Soft Matter

سال: 2021

ISSN: ['1744-683X', '1744-6848']

DOI: https://doi.org/10.1039/d1sm00380a