Research





Cell Membrane Dynamics :
During cell motility, the leading edge of the cell exhibits a range of dynamic structures such as  lamellipodia (flat disk-like extensions), filopodia (thin needle like protrusions) and membrane ruffles (wave-like instability). These structures are like the “feet” of the cell and are put out in an effort to feel and make attachments to the surroundings. They are hence vital to the process of motility. These dynamic surface patterns of moving cells are usually observed to have length-scales in the micron range, and appear in many different cell types.  They occur usually when the cell is stimulated by an external signal, indicating that the receptors on the cell membrane have a role to play. The receptors actually turn on in response to the signal and in turn initiate actin polymerization activity in their vicinity, which leads to force production. Our recent work showed that the dynamic membrane structures described above can arise from a simple analytic model which couples the membrane dynamics to the dynamics of receptors that reside on the membrane and the actin based protrusive forces they generate. Our model predicted membrane ruffling and the onset of filopodia and also gave explanations for several experimentally observed puzzling features such as the increased microviscosity at the leading edges of motile cells and the temperature dependence of the ruffle velocities.

N. Gov, A. Gopinathan, "Dynamics of Membranes Driven by Actin Polymerization", Biophys .J, 90(2), 454(2006)



Actin based propulsion :  A key process in motility is the production of a protrusive force that drives the cell’s leading edge forward. It has been well established that the cytoskeletal protein actin forms a dense, branched and crosslinked network of filaments at the leading edge and it is the polymerization of these filaments that gives rise to the force. The discovery that intracellular pathogens like listeria use the cell’s actin machinery to propel themselves played a vital role in establishing the biochemical basis of motility.  However, there still remains a hotly debated question: How does the polymerization activity at the molecular scale translate into a macroscopic force?  This led to the development of both the microscopic view that considers the protrusive force as arising from the monomer-by-monomer growth of a population of these filaments  and macroscopic models that treat the filaments as a continuum gel. Both of these describe the phenomenon albeit at very different length and time scales and are unable to satisfactorily account for all aspects of the motility (see for example the work by Kuo Lab. To get a correct and unified picture, we introduced a “dynamic gel” picture where we treated the actin network as an elastic gel modeled by a finite element mesh while allowing for spatial variations in polymerization activity .We treat the actin comet tail as an elastic continuum tethered to the rear of the bacterium. The interplay of polymerization and tethering gives rise to inhomogeneous stresses calculated with a finite element analysis. We quantitatively reproduce many distinctive features of actin propulsion that have been observed experimentally, including stepped motion, hopping, tail shape and the propulsion of flat surfaces.
 

Ajay Gopinathan and Andrea Liu, "Elastic Actin Tails: Shape, Stresses and Propulsion" in preparation



Biopolymer bundles: Bundles of stiff biopolymer bundles such as actin and microtubules among others form important structural elements in the cell including filopodia, microvili, cilia and contractile rings. These structures have specific functions to perform that rely crucially on their mechanical properties which in turn depend on the internal organization of the bundles. Recent investigations of microtubule bundles that were assembled  in vitro in the presence of different linker molecules were carried out here at the Safinya Lab. The resultant bundles were significantly curved at wavelengths several orders of magnitude less than their persistence length. We show that these severe distortions of the bundles can be explained by the presence of edge dislocation and twist defects indicating that these defects could play a significant role in vivo.

Ajay Gopinathan, M. Henle, U. Raviv and D. Needleman, "Defect Induced Morphologies of Biopolymer Bundles" in preparation



Polymer Translocation in Crowded Environments : Polymer translocation is an extensively studied topic and is biologically an important process that occurs in a variety of circumstances where biopolymers (like DNA say from a virus) are transported across a membrane into a different environment (say the cell interior). An important question that arises is : How does the crowded nature of the cellular cytoplasm affect this process? While this has been addressed in the context of protein folding and biochemical rates in vivo, one would expect this to have a dramatic effect on translocation. We systematically treat the entropic penalty due to the crowded environment and find new power law scalings of the translocation time with polymer length. We also find that the crowding inflicts a significant barrier and that adding a chemical potential gradient in order to overcome this results in very interesting translocation regimes as a function of crowding, chemical potential and polymer length.

work in progress (with Yong-Woon KIm)



Cytoskeletal Kinetics : Controlling the polymerization activity of cytoskeletal actin network plays an important role in cell motility. Even in the absence of motility, the actin network is not static but evolves via kinetic processes such as actin polymerization, depolymerization, capping, branching and severing which are regulated by various proteins in the cell .
Abnormal levels of expression of these regulatory proteins lead to diseased states characterized by drastic morphological changes in the cytoskeleton and loss of function. It is therefore imperative to understand how the regulatory protein concentrations act in concert to maintain a normal cytoskeletal morphology. Previous work treated one or more but not all of the above mentioned processes. We recently studied the steady-state morphology of such networks and derived simple expressions for characteristics such as the length distribution of filaments and branches, branch spacing, and monomer to filamentous actin ratio as functions of regulatory protein concentrations. We found that these characteristics exhibit several scaling regimes with respect to the different protein concentrations and that the severing and branching activities are optimally coupled in the cell.
 

A. Gopinathan, A.J. Liu, "Severing, Branching and their Optimal Coupling in Dynamic Actin Structures", to be submitted to Phys. Rev. Lett



Statistically locked-in transport : Measurements of colloidal transport through arrays of micrometer-scale potential wells created with holographic optical tweezers were performed at the Grier Lab . Varying the orientation of the trap array relative to the external driving force resulted in a hierarchy of lock-in transitions analogous to symmetry-selecting processes in a wide variety of systems with implications for immediate applications for continuously fractionating particles, biological cells, and macromolecules. Classical particles driven through periodically modulated potential energy landscapes are predicted to follow a Devil's staircase hierarchy of commensurate trajectories depending on the orientation of the driving force.The experiments did indeed reveal such a hierarchy, but not with the predicted structure. The microscopic trajectories, moreover, appeared to be random, with commensurability emerging only in a statistical sense. We introduced an idealized model for periodically modulated transport in the presence of randomness that captures both the structure and statistics of such statistically locked-in trajectories.

Ajay Gopinathan, D.G. Grier, "Statistically Locked-in Transport through Periodic Potential Arrays", Phys. Rev. Lett., 92, 130602 (2004)


Self Assembly of Nanowires : Experiments at the Jaeger lab have shown that when metals are evaporated and deposited on a templated substrate, like a phase separated diblock copolymer surface, certain metals show a marked preference for one phase over the other and in certain cases form continuous wires of nanometer scale. What surprised us was the stability of these wires which by surface energy considerations should exhibit the pearling instability (a liquid cylinder breaking up into drops ). We proposed an explanation based on the rate limiting step of nanocluster coalescence being nucleation of new terraces. We show that the different morphologies obtained can be understood in terms of the relative importance of the energetics and kinetics. We also show the existence of ``non-trivial'' correlations  between adjacent wires that can be understood based on a purely kinetic mechanism. We also compare these correlations quantitatively to those obtained from simulations done with the relevant experimental parameters and find them in good agreement.

Ajay Gopinathan, "Kinetic Self-Assembly of Metals on Co-Polymer Templates", Phys. Rev. E, 71(4) 041601 (2005)



Non-equilibrium kinetics :  Deliberately miscutting a crystal surface can  produce a regular array of monoatomic steps. Under suitable conditions (temperature, oxygen dosage) these steps can be made to merge to form double height double width steps. Experiments performed at the Sibener lab have been instrumental in elucidating the mechanism of this process. It is found that step doubling proceeds via a nucleation step where two adjacent step edges come together at a "point" and then the two steps "zipper" together irreversibly. Theoretical effort has gone into describing the mechanism for a pair of steps. However when there is a large array of steps, as in reality, the dynamical process of nucleation and zippering gives rise to a non-equilibrium evolution of the surface morphology. One also expects defect structures of various types.  We study the time evolution of the surface morphology by making an approximate mapping to the parking lot problem. This allows us to predict the number and nature of the defects as well as the time evolution. We also suggest protocols that can help generate surfaces with fewer defects in less time.

Defect Formation and Kinetics of Atomic Terrace Merging, Ajay Gopinathan and T.A. Witten, Phys. Rev. E 70, 041603 (2004)


Crumpling - Dynamics : A crumpled sheet has certain characteristic features that we are all familiar with. There are the sharply curved places - ridges and the almost flat places- the facets. Extensive work characterizing the static properties of the ridges and facets has been done by Witten and coworkers. But we knew of no characterization of the dynamics. We were interested in the question : what happens if we tap a certain point on a crumpled sheet and listen at another? What changes in elastic wave propagation arise due to the unique structures in a crumpled sheet ? To answer this we first derived the wave equation governing transverse elastic waves on an arbitratily curved and strained surface using a Lagrangian formalism. Our analysis led us to the conclusion that the ridges act as barriers leading to the trapping of certain modes within the facets!!

Trapping of Vibrational Energy in Crumpled Sheets :  Ajay Gopinathan, T.A. Witten and S.C. Venkataramani. Phys. Rev. E., 65, 036613 (2002)


Charged Colloidal Systems : There is now a growing body of evidence that like charge colloidal spheres dispersed in water need not simply repel each other. Under certain conditions they actually attract. Experiments like those performed at the Grier Lab are helping us gain insights into this phenomenon.In this work we investigated the influence of geometric confinement on the free energy of an idealized model for charge-stabilized colloidal suspensions. The mean-field Poisson-Boltzmann formulation for this system predicts pure repulsion among macroionic colloidal spheres. However fluctuations in the simple ions distribution provide a mechanism for the macroions to attract each other at large separations.Although this Casimir interaction long-ranged,we found it was too weak to influence colloidal crystals dynamics.

Weak Long-Ranged Casimir Attraction in Colloidal Crystals : Ajay Gopinathan, Tong Zhou, S.N. Coppersmith, L.P.  Kadanoff and D.G. Grier. Europhys. Lett., 57 (3), 451 (2002)


Phase Ordering Kinetics :  Consider a collection of spins at a high temperature that is suddenly quenched to zero temperature. What follows is domain coarsening where domains of up and down spins grow and grow. An interesting question is : given a spin what is the probability that after time t it still retains its original state without ever having flipped? An exponent characterizing how this probability scales with the typical length scale in the system is called the persistence exponent  beta. We found an exact expression for this quantity for 1D q-state Potts' system (spin with q states) with a suitably chosen model of coarsening.

Scaling Exponent Beta for Coarsening in a 1D q-state Potts' System : Ajay Gopinathan. J.Phys. A, 31 (1998) 5499