key: cord-0700465-7wr878p5
authors: Kanso, M. A.; Chaurasia, V.; Fried, E.; Giacomin, A. J.
title: Peplomer bulb shape and coronavirus rotational diffusivity
date: 2021-03-30
journal: Phys Fluids (1994)
DOI: 10.1063/5.0048626
sha: dd326e9da88f5045e632842e145e5e9da2578e58
doc_id: 700465
cord_uid: 7wr878p5

Recently, the rotational diffusivity of the coronavirus particle in suspension was calculated, from first principles, using general rigid bead-rod theory [M. A. Kanso, Phys. Fluids 32, 113101 (2020)]. We did so by beading the capsid and then also by replacing each of its bulbous spikes with a single bead. However, each coronavirus spike is a glycoprotein trimer, and each spike bulb is triangular. In this work, we replace each bulbous coronavirus spike with a bead triplet, where each bead of the triplet is charged identically. This paper, thus, explores the role of bulb triangularity on the rotational diffusivity, an effect not previously considered. We thus use energy minimization for the spreading of triangular bulbs over the spherical capsid. The latter both translates and twists the coronavirus spikes relative to one another, and we then next arrive at the rotational diffusivity of the coronavirus particle in suspension, from first principles. We learn that the triangularity of the coronavirus spike bulb decreases its rotational diffusivity. For a typical peplomer population of 74, bulb triangularity decreases the rotational diffusivity by [Formula: see text].

Recently, we calculated the rotational diffusivity of the coronavirus particle in suspension as a function of peplomer population, from first principles, using general rigid bead-rod theory ( Fig. 12 of Ref. 1). We did so by beading the capsid and then also by replacing each of its bulbous spikes with a single bead (Fig. 1) . One of the challenges of ab initio calculations from general rigid bead-rod theory on coronaviruses is that the peplomer arrangement is not known. However, we do know that the spikes are charge-rich. 2, 3 It also seems reasonable to assume that they are charged identically. Furthermore, we know that the coronavirus spikes are not anchored into its hard capsid, but rather just into its elastic viral membrane (Sec. 1 of Ref. 4 ). The coronavirus spikes are, thus, free to rearrange under their own electrostatic repulsions. This is why coronavirus spikes normally present microscopically as uniformly distributed over the capsid. In our previous work, we followed the well-known polyhedral solutions to the Thomson problem for singly charged particles repelling one another over a spherical surface. [5] [6] [7] By Thomson problem, we mean determination of how identically charged particles repel and then spread over a sphere by minimizing system potential energy. This minimum system electrostatic potential energy, when divided by the sphere area, is not to be confused with surface energy.

Since each coronavirus spike is a glycoprotein trimer, each spike bulb is triangular (Fig. 14 (Fig. 2) with a bead triplet (Fig. 3) , with each bead identical and charged identically. We must, thus, replace the well-known polyhedral solutions to the single-bead Thomson problem with our new solutions to the triple-bead Thomson problem. In this work, we thus use minimum potential energy peplomer arrangements for our coronavirus model particles.

Since coronavirus bulbs are trimers, they not only translate into a set of centroidal positions relative to one another but also twist into a set of orientations relative to one another. Our potential energy minimization for our triply beaded peplomers thus yields both triplet positions and triplet orientations (Fig. 4) . This new potential energy minimization yields a set of bead positions for the triply beaded peplomers whose centroid positions differ, of course, from the bead positions for the singly beaded counterpart of the same N p : In other words, the polyhedra of centroids differ from the well-known Thomson solutions used in Ref. 1.

The challenge in determining the rotational diffusivity of a virus particle, from first principles, begins with modeling its intricate geometry with beads, locating the position of each bead. Once overcome, the next challenge is to use this geometry to arrive at the transport properties for the SARS-CoV-2 particle. From these, we deepen our understanding of how these remarkable particles align their peplomers both for long enough, and often enough, to infect. 1 Whereas our prior work relied on the Thomson solution for point charges (Fig. 1) , here, we work with triads of point charges each spaced rigidly and equilaterally (Fig. 4) . We, thus, complicate the energy minimization with the length of this equilateral triangle, r D . From Table X ;

(1) and in this work, we choose r D =r p ¼ 0:19 for our energy minimization. To compare with our previous work, we match the dimensionless virus radius of Fig. 12 Table III) .

General rigid bead-rod model of triple beaded coronavirus, N c ¼ 256, Table III ).

minimization to arrange and orient the coronavirus spikes relative to one another, we next arrive, from first principles, at the rotational diffusivity of the coronavirus particles with triple beaded peplomers in suspension.

For this work, we chose general rigid bead-rod theory for its flexibility and accuracy (Sec. I of Refs. 8 and 9). Using general rigid beadrod theory, we follow the method of Sec. II of Ref. 1 to construct our virus particles from sets of beads whose positions are fixed relative to one another. For example, the SARS-CoV-2 particle geometry is a spherical capsid surrounded by a constellation of protruding peplomers. We take our bead-rod models of virus particles to be suspended in a Newtonian solvent. To any such collection of bead masses, we can associate a moment of inertia ellipsoid (MIE) whose center is the center of mass and whose principal moments of inertia match those of the virus particle. The MIE, thus, determines the orientability of the virus particle, and thus, the virus rotational diffusivity. We use Eqs. 

which we will use for our results below. Symbols, dimensional, or nondimensional are defined in Table I or Table II , following the companion paper for singly beaded peplomer for SARS-CoV-2 particle. 1

In this paper, we focus on small-amplitude oscillatory shear flow (SAOS). For this flow field, for the molecular definition of small amplitude, general rigid bead-rod theory yields [Eq. (32) 

whose left side is the macromolecular Weissenberg number. The polymer contributions to the complex viscosity, 11,12

are [Eqs. (40) and (41) 

and

where kx is the Deborah number. In this paper, we plot the real and minus the imaginary parts of the shear stress responses to smallamplitude oscillatory shear flow as functions of frequency, . As x ! 0, for the polymer contribution to the zero-shear viscosity, we get

which we use in the table of Sec. V below.

As shown by Kirchdoerfer, 15 each trimeric peplomer head, consisting of three glycoproteins, is well-approximated by an equilateral 

Let N p be the number of trimeric peplomers attached to the capsid-sphere C of radius r c . Let T i denote the equilateral triangle that approximates the trimeric head of the i th peplomer. Let the p th vertex of T i be parameterized by r c r i;q , where i ¼ 1…N p and q ¼ 1; 2; 3. Let the length of the side of T i , i ¼ 1…N p be given by d. Thus, the vertices of T i are r 2 c jr i;1 À r i;2 j 2 ¼ r 2 c jr i;1 À r i;3 j 2 ¼ r 2 c jr i;2 À r i;3 j 2 ¼ d 2 :

Let ' be the length of the spike of each peplomer, with each spike normal to C at the point of contact on C. We assume that the centroid of T i is at the other end of the spike. Therefore, it must lie on the sphere S of radius r s ¼ r c þ ',

We also assume that each triangle T i lies in the tangential plane of the S at its centroid. This implies that normal to the plane of T i must align with the vector joining the centroid of T i to the center of S,

which simplifies to

Let each vertex of each triangle T i , i ¼ 1…N p be endowed with point charge Q. The total electrostatic energy of N p peplomers, constrained to the sphere S of radius r c , is given by

where is the dielectric permittivity. Using the constrained minimization approach of Ref. 16 , we obtain numerical equilibrium solutions r i;q , i ¼ 1…N p , and p ¼ 1; 2; 3 that locally minimize the energy in Eq. (13) while satisfying the kinematic constraints in Eqs. (9)-(12), for given values of N p . Since the charge Q appears only as a prefactor in Eq. (13), its value plays no role in determining equilibrium solutions. Our trimeric model amounts to a replacement for the Thompson problem, 5 the objective of which is to find a state that distributes N p equilateral triads of charges over a unit sphere as evenly as possible, with minimum electrostatic energy. By contrast, Wales 6, 7 distributed N p single charges, providing solutions for a large set of values of N p .

From Fig. 5 , we learn that the detailed triangular structure of the peplomer head and its singly beaded counterpart share the same qualitative behavior. For both, the rotational diffusivity, k 0 D r , descends monotonically with N p . However, the detailed triangular structure of the peplomer head reduces significantly k 0 D r of the coronavirus particle. Specifically, at the measured peplomer population of N p ¼ 74, we see a reduction in k 0 D r of 39%. On close inspection, Fig. 5 also reveals

that is, the dimensionless rotational diffusivity of a coronavirus with N p singly beaded peplomers has about the same dimensionless rotational diffusivity of a coronavirus with 1 3 N p triply beaded peplomers. From Fig. 6 , we learn that the elasticity, g 00 = g 0 À g s ð Þ , of the coronavirus particle suspension is slight and that the detailed triangular structure of the peplomer head slightly reduces this elasticity. From Table III , we see that the corresponding b is nearly zero so that the polymer contribution to the real part of the complex viscosity is constant, g 0 À g s ð Þ=nkTk ¼ g 0 À g s ð Þ =nkTk ¼ 3=2. From Table III , we learn that the detailed triangular structure of the peplomer head increases the relaxation time, k, and thus, decreases the zero-shear viscosity, g 0 . From the rightmost column of Table III , we learn that the detailed triangular structure of the peplomer head decreases the zeroshear value of the first normal stress coefficient, W 1;0 .

Whereas much prior work on fluid physics related to the virus has attacked transmission, 17-41 this paper focuses on the ab initio calculation of coronavirus transport properties. Specifically, we have determined the rotational diffusivity, the property governing the particle alignment for cell attachment (see Sec. I of Ref. 1). Although our work is mainly curiosity driven, it may deepen our understanding of drug, vaccine, and cellular infection mechanisms.

Chaurasia et al. 42 (see also Chaurasia 43 ) developed a framework to find equilibrium solutions of a system consisting of flexible structures, specifically charged elastic loops constrained to a sphere. Their framework could be used to model flexible peplomers with uniformly charged heads. We leave this daunting task for a future study.

Since the coronavirus capsid can be ellipsoidal (Fig. 3 . of Ref. 44 ), called pleomorphism, we must eventually consider this too. Whereas this work considered the detailed triangular structure of the peplomer head as triads of three point-charges, we could also consider uniformly charged triangular rigid peplomers constrained to a sphere. By uniformly charged triangular, we mean that the charge would be uniformly distributed over the edges of the triangle rather than point charges at its vertices. We leave this task for a later date.

One cognate transport problem is the transient translation and twist of coronavirus spikes rearranging freely under their own FIG. 6. Effect of single (red) and triple beading (blue) on minus the imaginary part of the complex viscosity (N c ¼ 256, N p ¼ 74 corresponds to, respectively, rows 1 and 2 of Table III ). The polymer contribution g 0 À g s ð Þ =nkTk is nearly constant: Physics of Fluids ARTICLE scitation.org/journal/phf electrostatic repulsions, for instance, the transient following the extraction of a single spike. This paper is, of course, silent on this interesting problem, which we leave for another day. As in our previous work, 1 we have used repulsions of charged particles over the surfaces of spheres for both the capsid and the peplomer heads of the coronavirus to arrive at its transport properties. It has not escaped our attention that our solutions to the Thomson problem can also be used to calculate the Young's modulus of the coronavirus particle [Eq. (3a) of Ref. 45] and that by extension this Young's modulus will depend upon peplomer population. We leave this calculation for another day. When using the references cited herein, it is best to be mindful of corresponding ganged errata in Ref. 46 .

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The data that support the findings of this study are available within the article.

Editor's pick. Errata: Eq. (21) should be "a 2 2 þ 2 3 ð6b À 9Þa þ 1 9 ð36b 2 À 123b þ81Þ ¼ 0;" in Table XIV , n 0 À n s should be g 0 À g s . In Table XV , w 1;0 should be W 1;0 , and nKT should be nkT. In Table IV