We explore the long-time behavior and equilibrium properties of a system of linear filaments growing through nucleated polymerisation. We show that the length distribution for breakable filaments evolves through two well defined limiting cases: first, a steady state distribution determined by the balance of breakage and elongation is reached; upon monomer depletion at the end of the growth phase, an equilibrium length distribution biased towards smaller filament fragments emerges. We furthermore compute the time evolution of the concentration of small oligomeric filament fragments. For frangible filaments, oligomers are present both at early times and at equilibrium, whereas in the absence of fragmentation, oligomers are only present in significant quantities at the beginning of the polymerisation reaction. Finally, we discuss the significance of these results for the biological consequences of filamentous protein aggregation.
I IntroductionThe polymerisation of proteins into fibrillar structures is a type of behavior characteristic of many different systems, both in the context of functional [1][2][3][4][5] and aberrant biological pathways [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20] in nature. In particular, aberrant protein aggregation is observed in relation with 50 or more disorders associated with formation of amyloid fibrils [14,16,21]. A key question characterising such linear growth phenomena is the size of the structures that are formed from the proteins, as this factor can influence the severity of disease or its rate of progression [22][23][24][25][26][27][28]. Nucleated polymerisation reactions yield filament populations with highly heterogeneous lengths [22,[29][30][31][32]], a complexity due to the concurrent action of competing microscopic processes favoring either the lengthening or shortening of individual filaments in the ensemble. In this paper we focus on the behaviour of the size distribution of aggregates for long times, and explore the nature of the equilibrium distribution using numerical solutions to the master equation of filamentous growth, and obtain analytical results for many of the important limiting cases.
II Master EquationThe starting point for the analysis of the length distribution of filaments is given by the master equation describing the kinetics of breakable filament assembly. Letting f(t, j) denote the number of filaments of size j the master equation reads [32][33][34][35][36]: