Understanding the Concentration Dependence of Viral Capsid Assembly Kinetics - the Origin of the Lag Time and Identifying the Critical Nucleus Size

Understanding the Concentration Dependence of Viral Capsid Assembly   Kinetics - the Origin of the Lag Time and Identifying the Critical Nucleus   Size
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The kinetics for the assembly of viral proteins into a population of capsids can be measured in vitro with size exclusion chromatography or dynamic light scattering, but extracting mechanistic information from these studies is challenging. For example, it is not straightforward to determine the critical nucleus size or the elongation time (the time required for a nucleated partial capsid to grow completion). We show that, for two theoretical models of capsid assembly, the critical nucleus size can be determined from the concentration dependence of the assembly reaction half-life and the elongation time is revealed by the length of the lag phase. Furthermore, we find that the system becomes kinetically trapped when nucleation becomes fast compared to elongation. Implications of this constraint for determining elongation mechanisms from experimental assembly data are discussed.


💡 Research Summary

The assembly of viral capsid proteins into complete shells is a multistep process that can be monitored in vitro by techniques such as size‑exclusion chromatography or dynamic light scattering. However, extracting mechanistic parameters—especially the size of the critical nucleus and the time required for a nucleated intermediate to grow to a full capsid (the elongation time)—has remained difficult. In this study the authors address these challenges by analyzing two theoretical frameworks: a simple nucleation‑elongation model and a multistep nucleation model. Both models separate the overall reaction into a nucleation step, in which a critical number (n*) of subunits must come together, and an elongation step, in which additional subunits add sequentially to the nucleus.

The key insight is that the concentration dependence of the reaction half‑life (t½) directly reveals the critical nucleus size. By plotting log t½ versus log


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