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Probability of viral entry as a function of receptor concentration c ∞ , and viral degradation µ 0 , for various D, when the number of receptors needed for fusion is N ) 4 (left) and N ) 8 (right). Here, we assume random receptor binding and let degradation act only at the n ) 0 state, with magnitude µ 0 . Other parameters used are κ in ) q ) 0.0001. All quantities are dimensionless.  

Probability of viral entry as a function of receptor concentration c ∞ , and viral degradation µ 0 , for various D, when the number of receptors needed for fusion is N ) 4 (left) and N ) 8 (right). Here, we assume random receptor binding and let degradation act only at the n ) 0 state, with magnitude µ 0 . Other parameters used are κ in ) q ) 0.0001. All quantities are dimensionless.  

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Enveloped viruses attach to host cells by binding to receptors on the cell surface. For many viruses, entry occurs via membrane fusion after a sufficient number of receptors have engaged ligand proteins on the virion. Under conditions where the cell surface receptor densities are low, recruitment of receptors may be limited by diffusion rather than...

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Context 1
... Receptor Binding. In this section, we study the case of random receptor binding, where R ) 1. We first assume that cellular degradation acts only on the "naked" glycoprotein spike so that the nondimensional degradation rates µ 0 > 0 and µ n ) 0 for n * 0. Figure 2 shows the probability P in of the virus penetrating the cell as a function of the nondimen- sional receptor concentration c ∞ , degradation rate µ 0 , and receptor diffusion coefficient D, when the number of receptors necessary for entry is N ) 4 (left) and N ) 8 (right). Nondimensional kinetic rates are set to κ in ) q ) 0.0001. ...
Context 2
... shown in Figure 2, when µ 0 ) 0, the time-integrated entry probability P in ) 1 for all positive receptor diffusion coefficients and receptor concentrations. The fact that P in is a decreasing function of µ 0 is expected since only degradation represented by µ 0 > 0 can diminish the total entry probability. ...
Context 3
... fact that P in is a decreasing function of µ 0 is expected since only degradation represented by µ 0 > 0 can diminish the total entry probability. Even in the presence of degradation (µ 0 > 0), the fusion probability P in f 1 provided the receptor concentration c ∞ f ∞. Figure 2 also confirms that P in is an increasing function of the receptor diffusion coefficient D. Indeed, increasing D replenishes the concentration of receptors near the glycoprotein spike, speeding the receptor engagement process and increasing the probability of fusion. These qualitative results reveal that as long as c(r ) 1,t) is sufficiently large, either due to large D or large c ∞ , P in will be near unity. ...
Context 4
... the range of the parameters c ∞ , µ 0 , and D shown in Figure 2, the entry probabilities remain relatively insensitive to changes in the number of receptors N necessary for fusion when N goes from N ) 4 to N ) 8. However, there is an interesting quantitative transition in P in . ...
Context 5
... Figure 4, we plot the conditional mean time to viral entry, T (using eq 10), as a function of receptor concentration c ∞ and degradation rate µ 0 . We used the same parameters values as those used to generate Figure 2. Mean entry times are rather insensitive to receptor diffusivity D except at very low receptor concentrations c ∞ where receptor binding is highly diffusion- limited. ...
Context 6
... increasing the diffusion coefficient does not significantly increase the entry probability P in , the entry behavior in this regime is dominated by the degradation term. However, compared to the case where degradation occurs only at the receptor-free state (µ n ) 0 for n * 0, as shown in Figure 2), uniform degradation dramatically decreases the entry prob- ability as µ n ) µ 0 /(N + 1) increases. Even though the relative total strength of degradation is the same as that in Figure 2, the virus can now be degraded at any state n before the final irreversible fusion process, and it is not enough to escape the n ) 0 state to avoid degradation. ...
Context 7
... compared to the case where degradation occurs only at the receptor-free state (µ n ) 0 for n * 0, as shown in Figure 2), uniform degradation dramatically decreases the entry prob- ability as µ n ) µ 0 /(N + 1) increases. Even though the relative total strength of degradation is the same as that in Figure 2, the virus can now be degraded at any state n before the final irreversible fusion process, and it is not enough to escape the n ) 0 state to avoid degradation. P in is thus lower in Figure 5 than in Figure 2. ...
Context 8
... though the relative total strength of degradation is the same as that in Figure 2, the virus can now be degraded at any state n before the final irreversible fusion process, and it is not enough to escape the n ) 0 state to avoid degradation. P in is thus lower in Figure 5 than in Figure 2. ...
Context 9
... can also study how the relative magnitude of the kinetic rate constants affects the viral entry probabilities. Upon varying the unbinding rate constant q, and letting degradation act only on the n ) 0 unbound state, the probabilities P in are monotonic in D and c ∞ and quite similar to those shown in Figure 2 for each value of q. However, nonmonotonic behavior emerges in the dependence of the conditional mean entry time T on c ∞ and q, as shown in Figure 7 for N ) 4 (left) and N ) 8 (right). ...
Context 10
... Receptor Binding. In this section, we consider viral entry dynamics for the R ) 0 case of sequential adsorption using the same parameter values used in the previous sections and in Figures 2 and 4. Here, we only consider the case when degradation acts only on the n ) 0 state, with magnitude µ 0 . ...

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... Regarding the simulation of the viral entry into a cell membrane via endocytosis (Fig. 5), such important aspects were involved as the contact mechanics of viruses onto a flexible membrane [30, 82, 83 ,84, 85], effects of virus size and ligand density on the membrane wrapping [86], as well as, influence of receptor concentration gradient on the ligand-receptor binding [87]. The change of receptor density over the host membrane was described [37,88,89] by the Fick's second law [90,91,92], however, without consideration of diffusion induced stresses [93,94,95,96,97,98]. Continuum modeling was used for adhesive contact between the virus and cell membrane, driven by adhesion [82,83,84] or driven by adhesion and, additionally, by external displacement (or force) [30,85], however, under the assumption of linear elasticity. ...
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... Regarding the simulation of the viral entry into a cell membrane via endocytosis (Fig. 5), such important aspects were involved as the contact mechanics of viruses onto a flexible membrane [30, 82, 83 ,84, 85], effects of virus size and ligand density on the membrane wrapping [86], as well as, influence of receptor concentration gradient on the ligand-receptor binding [87]. The change of receptor density over the host membrane was described [37,88,89] by the Fick's second law [90,91,92], however, without consideration of diffusion induced stresses [93,94,95,96,97,98]. Continuum modeling was used for adhesive contact between the virus and cell membrane, driven by adhesion [82,83,84] or driven by adhesion and, additionally, by external displacement (or force) [30,85], however, under the assumption of linear elasticity. ...
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Introdution. Viruses are a large group of pathogens that have been identified to infect animals, plants, bacteria and even other viruses. The 2019 novel coronavirus SARS-CoV-2 remains a constant threat to the human population. Viruses are biological objects with nanometric dimensions (typically from a few tens to several hundreds of nanometers). They are considered as the biomolecular substances composed of genetic materials (RNA or DNA), protecting capsid proteins and sometimes also of envelopes. Objective. The goal of the present review is to help predict the response and even destructuration of viruses taking into account the influence of different environmental factors, such as, mechanical loads, thermal changes, electromagnetic field, chemical changes and receptor binding on the host membrane. These environmental factors have significant impact on the virus. Materials and methods. The study of viruses and virus-like structures has been analyzed using models and methods of nonlinear mechanics. In this regard, quantum, molecular and continuum descriptions in virus mechanics have been considered. Application of single molecule manipulation techniques, such as, atomic force microcopy, optical tweezers and magnetic tweezers has been discussed for a determination of the mechanical properties of viruses. Particular attention has been given to continuum damage–healing mechanics of viruses, proteins and virus-like structures. Also, constitutive modeling of viruses at large strains is presented. Nonlinear elasticity, plastic deformation, creep behavior, environmentally induced swelling (or shrinkage) and piezoelectric response of viruses were taken into account. Integrating a constitutive framework into ABAQUS, ANSYS and in-house developed software has been discussed. Conclusion. Link between virus structure, environment, infectivity and virus mechanics may be useful to predict the response and destructuration of viruses taking into account the influence of different environmental factors. Computational analysis using such link may be helpful to give a clear understanding of how neutralizing antibodies and T cells interact with the 2019 novel coronavirus SARS-CoV-2.
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... 11 It was also shown that sometimes multiple receptors are needed for a virus to enter the cell, which might lead to even longer and more complex diffusion processes. 13 The problem of association of small ligands with specific active sites on the surfaces has been investigated before using various theoretical tools. [14][15][16][17][18][19][20] Analysis of this class of problems was initiated by Berg. ...
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... 11 It was also shown that sometimes multiple receptors are needed for a virus to enter the cell, which might lead to even longer and more complex diffusion processes. 13 The problem of association of small ligands with specific active sites on the surfaces has been investigated before using various theoretical tools. 14-17 A diffusion limited association, when the reaction of binding to the surface (both specific and non-specific) is instantaneous, has been considered by Berg. ...
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Full-text available
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