<?xml version="1.0" encoding="UTF-8"?>
<rss xmlns:dc="http://purl.org/dc/elements/1.1/" version="2.0">
<channel>
<title>Publications</title>
<link>http://hdl.handle.net/1721.1/18155</link>
<description/>
<pubDate>Sun, 26 May 2013 02:41:12 GMT</pubDate>
<dc:date>2013-05-26T02:41:12Z</dc:date>
<item>
<title>A Mechanistic Model of the Actin Cycle</title>
<link>http://hdl.handle.net/1721.1/26696</link>
<description>A Mechanistic Model of the Actin Cycle
Bindschadler, M.; Osborn, E. A.; Dewey, C. F. Jr; McGrath, J. L.
We have derived a broad, deterministic model of the steady-state actin cycle that includes its major regulatory&#13;
mechanisms. Ours is the first model to solve the complete nucleotide profile within filaments, a feature that determines the&#13;
dynamics and geometry of actin networks at the leading edges of motile cells, and one that has challenged investigators&#13;
developing models to interpret steady-state experiments. We arrived at the nucleotide profile through analytic and numerical&#13;
approaches that completely agree. Our model reproduces behaviors seen in numerous experiments with purified proteins, but&#13;
allows a detailed inspection of the concentrations and fluxes that might exist in these experiments. These inspections provide&#13;
new insight into the mechanisms that determine the rate of actin filament treadmilling. Specifically, we find that mechanisms for&#13;
enhancing Pi release from the ADP-Pi intermediate on filaments, for increasing the off rate of ADP-bound subunits at pointed&#13;
ends, and the multiple, simultaneous functions of profilin, make unique and essential contributions to increased treadmilling. In&#13;
combination, these mechanisms have a theoretical capacity to increase treadmilling to levels limited only by the amount of&#13;
available actin. This limitation arises because as the cycle becomes more dynamic, it tends toward the unpolymerized state.
Biophysical Journal, 2004
</description>
<pubDate>Sat, 01 May 2004 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/1721.1/26696</guid>
<dc:date>2004-05-01T00:00:00Z</dc:date>
</item>
<item>
<title>Simultaneous Measurements of Actin Filament Turnover, Filament Fraction, and Monomer Diffusion in Endothelial Cells</title>
<link>http://hdl.handle.net/1721.1/26695</link>
<description>Simultaneous Measurements of Actin Filament Turnover, Filament Fraction, and Monomer Diffusion in Endothelial Cells
McGrath, J. L.; Tardy, Y.; Dewey, C. F. Jr; Meister, J. J.; Hartwig, J. H.
The analogous techniques of photoactivation of fluorescence (PAF) and fluorescence recovery after photobleaching&#13;
(FRAP) have been applied previously to the study of actin dynamics in living cells. Traditionally, separate&#13;
experiments estimate the mobility of actin monomer or the lifetime of actin filaments. A mathematical description of the&#13;
dynamics of the actin cytoskeleton, however, predicts that the evolution of fluorescence in PAF and FRAP experiments&#13;
depends simultaneously on the diffusion coefficient of actin monomer, D, the fraction of actin in filaments, FF, and the lifetime&#13;
of actin filaments, t (Tardy et al., 1995, Biophys. J. 69:1674–1682). Here we report the application of this mathematical model&#13;
to the interpretation of PAF and FRAP experiments in subconfluent bovine aortic endothelial cells (BAECs). The following&#13;
parameters apply for actin in the bulk cytoskeleton of subconfluent BAECs. PAF: D 5 3.1 6 0.4 3 1028 cm2/s, FF 5 0.36 6&#13;
0.04, t 5 7.5 6 2.0 min. FRAP: D 5 5.8 6 1.2 3 1028 cm2/s, FF 5 0.5 6 0.04, t 5 4.8 6 0.97 min. Differences in the&#13;
parameters are attributed to differences in the actin derivatives employed in the two studies and not to inherent differences&#13;
in the PAF and FRAP techniques. Control experiments confirm the modeling assumption that the evolution of fluorescence&#13;
is dominated by the diffusion of actin monomer, and the cyclic turnover of actin filaments, but not by filament diffusion. The&#13;
work establishes the dynamic state of actin in subconfluent endothelial cells and provides an improved framework for future&#13;
applications of PAF and FRAP.
Biophysical Journal, 1998
</description>
<pubDate>Tue, 01 Sep 1998 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/1721.1/26695</guid>
<dc:date>1998-09-01T00:00:00Z</dc:date>
</item>
<item>
<title>Theoretical Estimates of Mechanical Properties of the Endothelial Cell Cytoskeleton</title>
<link>http://hdl.handle.net/1721.1/26694</link>
<description>Theoretical Estimates of Mechanical Properties of the Endothelial Cell Cytoskeleton
Satcher, Robert L. Jr.; Dewey, C. Forbes Jr.
Current modeling of endothelial cell mechanics does not account for the network of F-actin that permeates the&#13;
cytoplasm. This network, the distributed cytoplasmic structural actin (DCSA), extends from apical to basal membranes, with&#13;
frequent attachments. Stress fibers are intercalated within the network, with similar frequent attachments. The microscopic&#13;
structure of the DCSA resembles a foam, so that the mechanical properties can be estimated with analogy to these&#13;
well-studied systems. The moduli of shear and elastic deformations are estimated to be on the order of 10^5 dynes/cm^2 . This&#13;
prediction agrees with experimental measurements of the properties of cytoplasm and endothelial cells reported elsewhere.&#13;
Stress fibers can potentially increase the modulus by a factor of 2-10, depending on whether they act in series or parallel to&#13;
the network in transmitting surface forces. The deformations produced by physiological flow fields are of insufficient&#13;
magnitude to disrupt cell-to-cell or DCSA cross-linkages. The questions raised by this paradox, and the ramifications of&#13;
implicating the previously unreported DCSA as the primary force transmission element are discussed.
Biophysical Journal, 1996
</description>
<pubDate>Mon, 01 Jan 1996 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/1721.1/26694</guid>
<dc:date>1996-01-01T00:00:00Z</dc:date>
</item>
<item>
<title>Interpreting Photoactive Fluorescence Microscopy Measurements of Steady-State Actin Dynamics</title>
<link>http://hdl.handle.net/1721.1/26693</link>
<description>Interpreting Photoactive Fluorescence Microscopy Measurements of Steady-State Actin Dynamics
Tardy, Y.; McGrath, J.L.; Hartwig, J.H.; Dewey, C.F.
A continuum model describing the steady-state actin dynamics of the cytoskeleton of living cells Has been&#13;
developed to aid in the interpretation of photoactivated fluorescence experiments. In a simplified cell geometry, the model&#13;
assumes uniform concentrations of cytosolic and cytoskeletal actin throughout the cell and no net growth of either pool. The&#13;
spatiotemporal evolution of the fluorescent actin population is described by a system of two coupled linear partial-differential&#13;
equations. An analytical solution is found using a Fourier-Laplace transform and important limiting cases relevant to the&#13;
design of experiments are discussed. The results demonstrate that, despite being a complex function of the parameters, the&#13;
fluorescence decay in photoactivated fluorescence experiments has a biphasic behavior featuring a short-term decay&#13;
controlled by monomer diffusion and a long-term decay governed by the monomer exchange rate between the polymerized&#13;
and unpolymerized actin pools. This biphasic behavior suggests a convenient mechanism for extracting the parameters&#13;
governing the fluorescence decay from data records. These parameters include the actin monomer diffusion coefficient,&#13;
filament turnover rate, and ratio of polymerized to unpolymerized actin.
Biophysical Journal, 1995
</description>
<pubDate>Sun, 01 Jan 1995 00:00:00 GMT</pubDate>
<guid isPermaLink="false">http://hdl.handle.net/1721.1/26693</guid>
<dc:date>1995-01-01T00:00:00Z</dc:date>
</item>
</channel>
</rss>
