Rhombic Analysis Extension of a Plant-Surface Water Interaction-Diffusion Model for Hexagonal Pattern Formation in an Arid Flat Environment ()

Bonni J. Kealy-Dichone^{1}, David J. Wollkind^{2}, Richard A. Cangelosi^{1}

^{1}Department of Mathematics, Gonzaga University, Spokane, USA.

^{2}Department of Mathematics, Washington State University, Pullman, USA.

**DOI: **10.4236/ajps.2015.68128
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An existing weakly nonlinear diffusive instability hexagonal planform analysis for an interaction-diffusion plant-surface water model system in an arid flat environment [11] is extended by performing a rhombic planform analysis as well. In addition a threshold-dependent paradigm that differs from the usually employed implicit zero-threshold methodology is introduced to interpret stable rhombic patterns. The results of that analysis are synthesized with those of the existing hexagonal planform analysis. In particular these synthesized results can be represented by closed-form plots in the rate of precipitation versus the specific rate of plant density loss parameter space. From those plots, regions corresponding to bare ground and vegetative Turing patterns consisting of tiger bush (parallel stripes and labyrinthine mazes), pearled bush (hexagonal gaps and rhombic pseudo-gaps), and homogeneous distributions of vegetation, respectively, may be identified in this parameter space. Then that predicted sequence of stable states along a rainfall gradient is both compared with observational evidence and used to motivate an aridity classification scheme. Finally this system is shown to be isomorphic to the chemical reaction-diffusion Gray-Scott model and that isomorphism is employed to draw some conclusions about sideband instabilities as applied to vegetative patterning.

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Kealy-Dichone, B. , Wollkind, D. and Cangelosi, R. (2015) Rhombic Analysis Extension of a Plant-Surface Water Interaction-Diffusion Model for Hexagonal Pattern Formation in an Arid Flat Environment. *American Journal of Plant Sciences*, **6**, 1256-1277. doi: 10.4236/ajps.2015.68128.

1. Introduction

In order to explain more fully the occurrence of tiger bush (or banded thicket) patterns in arid flat environments [1] , Kealy and Wollkind [2] introduced a two-component interaction-diffusion model system based on the Klausmeier [3] differential flow instability model but including the diffusion of surface water rather than its advection. That is, they considered the dimensionless coupled partial differential interaction-diffusion equation model for plant biomass density and surface water content, where a two- dimensional spatial coordinate system and time,

(1.1)

(1.2)

defined on an unbounded planar domain with

. (1.3)

Here A and L are the rates of precipitation and evaporation for the water; R and M, the rates of water infiltration and biomass loss for the plants; J, the yield of plant biomass per unit water consumed; and and, the constant dispersal and diffusion coefficients of the plants and water, respectively.

From a linear stability analysis of its possible critical points, Kealy and Wollkind [2] deduced that system (1.1)-(1.2) admitted both a bare ground trivial equilibrium point (,) , which existed and was stable for all parameter values, and a homogeneous vegetation community equilibrium point which could generate a Turing [4] -type diffusive instability. They then performed a variety of weakly nonlinear instability analyses on that community equilibrium point finding from a one-dimensional analysis that it bifurcated supercritically to form a stationary striped vegetative pattern and from a two-dimensional hexagonal planform analysis that a close-packed array of vegetative gaps could occur in a narrow region flanking the marginal stability curve in their diffusive instability parameter space for the typical value of [5] . Finally, Kealy and Wollkind [2] identified these theoretical predictions with tiger and pearled bush patterns, respectively, and compared them with numerical simulations of Klausmeier’s [3] model system. Specifically, they showed that the predicted wavelength of the tiger bush patterns including the width ratio between stripes and interstripes was in very good quantitative agreement with the vegetative bands involving acacia trees in the Go-Gub area of Somaliland [6] . To make this comparison Kealy and Wollkind [2] employed the concept of low threshold patterns, originally introduced by Wollkind and Stephenson [7] and Boonkorkuea et al. [8] , without explicitly specifying the mechanism required to pose the proper threshold value for vegetative biomass associated with that methodology. After Cangelosi et al. [9] , who investigated a model for mussel bed patterning, in order to make this selection process more precise it is necessary for us to extend the weakly nonlinear stability analyses of Kealy and Wollkind [2] by performing a two-dimensional rhombic planform analysis of the community equilibrium point of (1.1)-(1.2) as well.

As a prelude to that investigation, we summarize the hexagonal planform results of Kealy and Wollkind [2] in Section 2. We perform the rhombic planform nonlinear diffusive instability analysis of the homogeneous vegetative equilibrium point of (1.1)-(1.2) in Section 3. In particular we find that, although square patterns of rhombic angle are not stable, rhombic patterns of other characteristic angles do occur. In the process we introduce a threshold-dependent paradigm to interpret those stable rhombic patterns that differs from the implicit zero- threshold methodology usually employed for this purpose. We synthesize the results of Sections 2 and 3, in Section 4. These synthesized results can be represented by closed-form plots in parameter space for a fixed value of. From those plots, regions corresponding to bare ground and vegetative patterns consisting of tiger bush (parallel stripes and labyrinthine mazes), pearled bush (hexagonal gaps and rhombic pseudo-gaps), and homogeneous distributions of vegetation, respectively, may be identified in this parameter space. Then that predicted sequence of stable states along a rainfall gradient is both compared with observational evidence and used to motivate an aridity classification scheme based upon the vegetative patterning inherent to our system. Unlike strictly numerical procedures these analytical stability methods can be employed to determine quantitative relationships between system parameters and stable patterns which make it easier to compare theoretical predictions with field observations. Finally, we show our model to be isomorphic to the Gray-Scott chemical reaction- diffusion system and apply sideband instability results deduced for the latter to nonlinear vegetative pattern formation.

2. The One-Dimensional and Hexagonal-Planform Results of Kealy and Wollkind [2]

Kealy and Wollkind [2] found that the homogeneous vegetation equilibrium point of (1.1)-(1.2), which existed for, was linearly stable in the absence of diffusion when

(2.1)

They performed a hexagonal planform analysis of that community equilibrium point of system (1.1)-(1.2) by seeking a solution to it that to lowest order satisfied

(2.2)

where, for even permutations of (1, 2, 3),

(2.3)

(2.4)

with an analogous expansion for.

Their one-dimensional pattern formation results can be deduced by taking

(2.5)

in (2.2) and (2.3)-(2.4). From a linear stability analysis Kealy and Wollkind [2] found that the components of the maximum point of the marginal curve in their wave number squared-bifurcation parameter two-dimensional space were given by

(2.6)

where

(2.7)

with being the most dangerous mode of linear theory. Then, for fixed and, when, when, and when. Thus the locus served as a marginal stability surface in three-dimensional space. In addition the locus where

(2.8)

depicted in Figure 1, served as a similar surface in space.

Under the conditions of (2.5), the amplitude-phase equations of (2.3)-(2.4) reduced to the Landau equation

(2.9)

Figure 1. Three-dimensional plots of the marginal stability surface of with and the planar surface for and.

From their one-dimensional nonlinear stability analysis Kealy and Wollkind [2] found that

(2.10)

where is plotted versus in Figure 2 for and. That Landau constant, given explicitly in the Appendix, had the asymptotic representation [2]

(2.11)

where

(2.12)

Figure 2 consists of two parts: A left-hand part for which has been plotted for the same -domain as in Figure 1, namely; and a right-hand one, which is an enlargement of the former restricted to the lower end of that -domain. From Figure 2, it can be observed that this curve has a zero at characterized by

(2.13)

where

(2.14)

and a linear asymptote of the form which is almost coincident with it when the -scale of Figure 1 is employed. Since for ecologically relevant values of―e.g., and [3] , the constraint was satisfied identically should [5] , Kealy and Wollkind [2] considered positive and concluded that when, the community equilibrium point was stable giving rise to a uniform homogeneous vegetative distribution while when a re-equilibrated state of stationary

Figure 2. Plots of the Landau constant of versus for with (solid line) and its asymptotic approximation as given by (2.11) (dashed line). The right-hand panel is an enlargement to illustrate the behavior of the approximation near.

parallel vegetative stripes resulted with amplitude and dimensional and dimensionless wavelength

(2.15)

respectively.

The one-dimensional pattern formation results of Kealy and Wollkind [2] are summarized in the plane of Figure 3 for The traces of the Turing bifurcation boundary surface and the plane of Figure 1 are plotted in that figure versus when. Then the regions, and can be identified with bare ground, stationary striped vegetative patterns, and homogeneous vegetative distributions, respectively, in that parameter space. Finally note that and should while (2.1) is satisfied identically for.

Wishing to refine their one-dimensional pattern formation predictions summarized in Figure 3, Kealy and Wollkind [2] next considered the full two-dimensional hexagonal planform expansions of (2.2) and (2.3)-(2.4). Since and were given by their one-dimensional analysis only and needed to be evaluated. Proceeding in the same manner as they did with the one-dimensional expansion to determine, Kealy and Wollkind [2] employed the relevant Fredholm-type solvability conditions to yield explicit formulae (see the Appendix) for the remaining two Landau constants

(2.16)

catalogued the critical points of equations (2.3)-(2.4); summarized their orbital stability behavior; and identified the potentially stable ones with various vegetative patterns obtaining the following critical point identifications: I, homogeneous distributions; II, stripes, spots; and gaps. Note, in this context, that I and II represent the same identifications as catalogued in Figure 3. The contour plots relevant to critical points are depicted in Figure 4, where Figure 4(a) is for and Figure 4(b), for. Here, the spatial variables are measured in units of while dark and light regions correspond to high and low densities, respectively, in accordance with the aerial photographs appearing in [6] and [10] .

Kealy and Wollkind [2] first determined that critical point I was stable provided. Then, since the existence and stability of critical points II and depended upon them, they examined the signs of, , , and as functions of by plotting those quantities as well as versus for with which we reproduce in Figure 5 for. Kealy and Wollkind [2] found that was identically positive while all the other relevant quantities in Figure 5 were positive for, having zeroes less than. Thus, since only critical points II and could be stable [11] . Note, in this context, that critical point cannot be stable under these conditions and hence this model may only predict vegetative gaps but not spots. Finally, Kealy and Wollkind [2] represented their stability results graphically in the plane by generating the loci associated with with, 1, and 2,

Figure 3. Stability diagram in the plane for our one- dimensional interaction-diffusion model system with and, denoting the predicted vegetative patterns. The curves depicted in this figure are cross-sections of the plane with the surfaces of Figure 1. Hence, the upper one is the Turing boundary with and the lower one, the straight line.

(a) (b)

Figure 4. (a) A contour plot of the hexagonal array of spots for; (b) A contour plot of the hexagonal array of gaps for.

respectively, for

(2.17)

from (2.8)

Figure 5. Plots of, , , and of (A.1) and (A.2) versus for with, where plots of and are presented for purposes of comparison.

(2.18)

where

(2.19)

We plot these loci along with those of Figure 3 in Figure 6 for and. Using the stability criteria for critical points II and [11] , Kealy and Wollkind [2] made the morphological predictions that stripes could occur for while hexagonal close-packed arrays of vegetative gaps could occur for. Since homogeneous distributions of vegetation could occur for, there were two regions of bistability: Namely, , where homogeneous distributions and gaps could occur; and, , where gaps and stripes could occur. Further bare ground occurred for.

We close this section with the observation that in order to retain only terms through third-order in our expansions of (2.3)-(2.4) its Landau constants must be in the relation [12]

(2.20)

which is satisfied for those quantities as depicted in Figure 5.

3. Two-Dimensional Analysis: Rhombic-Planform Nonlinear Stability Results

Wishing to refine further the two-dimensional hexagonal planform predictions summarized in Figure 6 and to investigate more precisely the possibility of occurrence of the low-threshold tiger bush patterns observed by Levefer and Lejeune [6] , we next consider a rhombic-planform solution of system (1.1)-(1.2) of the form [7]

(3.1)

Figure 6. Plots of, , and of (2.19) as well as and of Figure 3 versus for with. The right-hand panel is an enlargement depicting the intersection point between the vertical line and the locus (see Section 4). Note that the plots of and virtually coincide.

where

(3.2)

with an analogous expansion for, such that

(3.3)

(3.4)

Here we are employing the notation for the coefficient of each term in (3.1) of the form The terms on the right-hand side of (3.3)-(3.4) can be deduced by examining the amplitude functions in (3.1) proportional to and, respectively. Then substituting this rhombic-planform solution of (3.1)-(3.2) into system (1.1)-(1.2), we obtain a sequence of problems, each of which corresponds to one of these terms. In order to catalogue the solutions of those problems we introduce the following notation. Denoting the interaction terms in (1.1)-(1.2) by

(3.5)

we define the expansion coefficients

(3.6)

which are tabulated below:

(3.7)

Solving those problems we find that

(3.8)

while applying the same method of analysis, as employed for deducing (A.1) and (A.2), to the, , system yields the Fredholm-type solvability condition for the second rhombic-planform third-order Landau constant

(3.9)

where the components of

(3.10)

as well as the solutions for the relevant second-order systems are catalogued in the Appendix.

Having developed these formulae for its growth rate and Landau constants, we now turn our attention to the rhombic-planform amplitude Equations (3.3)-(3.4), which possess the following equivalence classes of critical points:

(3.11)

Assuming that and investigating the stability of these critical points one finds that [7] :

(3.12)

Note that I and II, as in the one-dimensional analysis of the previous section, represent the uniform homogeneous and supercritical banded states, respectively, while V can be identified with a rhombic pattern possessing characteristic angle [7].

We now use these criteria to pursue those goals stated at the beginning of this section. Toward that end, we first plot versus for, , , and with in the four parts of Figure 7, respectively, each of which also includes a plot of the of Figure 5. Here represents a limiting case where the rhombic pattern reduces to parallel stripes while represents a square planform (see below). Upon comparing with in Figure 7, we see that for,

(a) (b)(c) (d)

Figure 7. Plots of of (3.9)-(3.10) (dashed curve) and of (solid curve) versus with for (a) 0; (b); (c), and (d).

for and and for. Hence, since the latter condition violates the stability criterion of (3.12), we can conclude that stable square patterns do not occur for this problem when. From (3.11)-(3.12) we can deduce that, to demonstrate conclusively a rhombic pattern of angle exists and is stable, we must show that or, equivalently after Geddes et al. [13] defining the ratio of these Landau constants by, that

(3.13)

provided, in addition, that or. Next, we plot this ratio of Landau constants versus for the fixed values of and in Figure 8. Restricting ourselves to the interval of interest, we see from this figure that there are two bands of stable rhombic patterns flanking for or when where

(3.14)

which have been designated by vertical lines. Both of these lie between and, which have been designated by horizontal lines. In particular, consistent with Figure 7(b) and Figure 7(c) when, note that while. In this context, observe that, for the special case of, (3.13) reduces to or. Observe from Figure 8 that

(3.15)

which is consistent with Figure 7(a). Also note that this figure has been drawn for the extended interval in order to demonstrate graphically the symmetry about characteristic of rhombic patterns since

(3.16)

Here, properties (3.15) and (3.16) are a consequence of mode interference occurring exactly at and modal interchange, respectively [14] .

We have deferred until now a detailed morphological interpretation of the rhombic patterns that can be identified with critical point V for the values of the characteristic angle relevant to Figure 7. Then, to lowest order, the equilibrium vegetative pattern associated with that critical point satisfies

(3.17)

where

Figure 8. A plot of of (3.13) versus for and.

(3.18)

The three parts of Figures 9-12 are threshold contour plots of (3.18) for, , , and with threshold values of, 0, and 1, respectively. Here the spatial variables are again being measured in units of and regions exceeding that threshold in each part appear dark while those below it appear light. Hence from left to right the parts of these figures correspond to what Wollkind and Stephenson [7] , Boonkorkuea et al. [8] , and Cangelosi et al. [9] termed lower, zero, and upper threshold patterns, respectively. In this context note that. Traditionally, most pattern formation analyses of this type have used the dimensional homogeneous vegetative solution value of where [2]

(3.19)

Figure 9. Striped patterns relevant to of (3.17)-(3.18) for with threshold values from left to right of (a), (b) 0, and (c) 1.

Figure 10. Rhombic patterns relevant to of (3.17)-(3.18) for with threshold values from left to right of (a), (b) 0, and (c) 1.

Figure 11. Rhombic patterns relevant to of (3.17)-(3.18) for with threshold values from left to right of (a), (b) 0, and (c) 1.

Figure 12. Square patterns relevant to of (3.17)-(3.18) for with threshold values from left to right of (a), (b) 0, and (c) 1.

as the threshold to trigger the color change from light to dark (see Figure 4). Thus all spatial regions characterized by appear light and those characterized by, dark, where again light regions correspond to low plant biomass density or bare ground and dark ones to high plant biomass density. This is equivalent to our zero threshold cases of Figures 9-12 upon assuming, without loss of generality, that Explicitly denoting

(3.20)

Kealy and Wollkind [2] plotted for, 0, and 1, as well as the marginal stability curve in the plane with for. Analogous to the morphological stability predictions of Figure 6, they concluded that homogeneous distributions could occur for, stripes for, and gaps for. We reproduce these results in Figure 13 for and defining

(3.21)

adopt the protocol that represents this threshold instead. Then, where or, the lower threshold patterns of Figures 9-12 would occur while, where or, the upper threshold patterns would occur. Given their similarity of appearance to the hexagonal vegetative patterns of Figure 4 we shall now label these lower and upper threshold rhombic vegetative arrays as pseudo gaps and pseudo spots and denote them by and, respectively. In this context, after Sekimura et al. [15] , the lower and upper threshold patterns of Figure 12 could be labeled as square gaps and square spots, respectively.

4. Synthesis, Aridity Classification Scheme, and Comparisons

We first wish to synthesize the morphological stability predictions summarized in Section 2 and developed in Section 3, respectively. To do so, we begin by considering our rhombic pattern formation results of the latter section in conjunction with the hexagonal pattern formation ones of the former section. Extrapolating from the conclusions of Golovin et al. [16] and Schatz et al. [17] , who demonstrated theoretically and experimentally, respectively, that square patterns only occurred for Marangoni convection with poorly conducting boundaries in the neighborhood of the marginal stability curve where supercritical Bénard cells but not rolls would normally be predicted from a hexagonal planform analysis, we can deduce that our stable rhombic vegetative patterns will only occur in the region of parameter space satisfying in Figure 13 or, equivalently, in Figure 6. Since (see Figure 13), these stable rhombic patterns will be of the lower threshold variety or pseudo gaps. Hence, we can synthesize our morphological stability predictions of Section 2 and Section 3 by means of Table 1 which identifies the relevant regions of parameter space in Figure 6 and Figure 13 with the stable vegetative patterns that can occur in those regions.

Observe from Figure 6 that the plot of seems to be visibly coincident with the Turing boundary. In this context, note that, for the parameter value of relevant to tiger bush [3] ,

Figure 13. Plots of the marginal curves of (2.6)-(2.7) and (3.20)-(3.21) versus with.

(4.1)

The locus is designated by the vertical line appearing in Figure 6. Since the behavior portrayed in (4.1) occurs for all and deviations of this sort are well within the allowable observational error, we shall take

(4.2)

in what follows. Under this simplification the rainfall column of the morphological stability predictions of Table 1 reduces to that of Table 2.

We represent generic versions of these patterns in Figure 14. Here we have made use of the fact that serves as the critical threshold which can be deduced from our adoption of for that purpose in conjunction with Table 1. Hence we may conclude that lower, zero, or upper threshold patterns occur for a greater than, equal to, or lesser than, respectively. Note that the gap and pseudo gap patterns depicted in Figure 14 are of the lower threshold type since they occur for as opposed to the gap pattern of Figure 4(b) which was implicitly of the zero-threshold type while the depicted stripe patterns are of all the three threshold types appearing in Figure 9. We now after von Hardenberg et al. [18] offer an aridity classification scheme along a rainfall gradient in Table 3 based upon the results of Table 2 particularized to those values of (4.1) for and.

Kealy and Wollkind [2] compared their theoretical predictions with relevant observational evidence involving periodic self-organized vegetative patterns of tiger and pearled bush occurring in homogeneous ecosystems (reviewed by Rietkerk et al. [19] ). Tiger bush tends to consist of parallel vegetative stripes. When the ground surface slopes, these stripes migrate upslope while when that surface is practically flat static banded vegetation patterns result. Couteron et al. [1] catalogued those differences between these two-types of banded thicket patterns. The static banded states provided good qualitative agreement with tiger bush patterns found in arid flat environments while the upslope migrating stripes predicted by Klausmeier [3] , Sherratt [20] , and Sherratt and Lord [21] provided such agreement with those found in sloping environments. Hence, Wollkind and Kealy [2]

(a) (b)(c) (d)

Figure 14. Predicted generic vegetative patterns relevant to Table 3 for (a) Pseudo Gaps and Gaps; (b) Gaps and Low-threshold Stripes; (c), Zero-threshold Stripes; (d), High-threshold Stripes.

Table 1. Synthesized morphological stability predicitions for Figure 6 and Figure 13.

Table 2. Simplified morphological stability predictions along a rainfall gradient.

identified their parallel stationary diffusive instability stripes with those tiger bush patterns found on plateaus. In order to demonstrate that their model also provided good quantitative agreement with observed tiger bush patterning, they considered Figure 1 of Lefever and Lejeune [6] which is a photograph of regular parallel stripes

Table 3. Aridity classification scheme along a rainfall gradient for.

consisting of Acacia bussei trees in the Go-Gub area of Somaliland. These stripes are about 100 m wide while the width of the separating interstripes is about 50m. Thus the dimensional wavelength associated with this pattern is approximately

(4.3)

To compare these predicted pattern wavelengths of (2.15) with this result, they first reformulated the wavenumber expression of (2.6) by solving the marginal stability curve for to obtain

(4.4)

and then substituting (4.4) into (2.6) found that

(4.5)

Now, employing this formula of (4.5) in (2.15) and making use of the definition of from (1.3), they represented

(4.6)

and

(4.7)

Introducing the evaporation rate and surface water diffusion values from Klausmeier [3] and Rietkerk et al. [5] , respectively,

(4.8)

into (4.6)-(4.7) then yielded

(4.9)

which, upon comparison with (4.3), implied that

(4.10)

Finally, inverting (4.6), Kealy and Wollkind [2] obtained

(4.11)

where

(4.12)

They then used (4.11)-(4.12) to plot lines of various constant wavelength in the striped patterned region in their figure analogous to our Figure 3 which we reproduce in Figure 15 but for with. From (4.11)-(4.12), Kealy and Wollkind [2] deduced that the contour in Figure 15 satisfied the linear relationship

(4.13)

Recalling that, this corresponds to and is consistent with Klausmeier’s [3]

Figure 15. A reproduction of the plane of Figure 3 denoting the lines of various constant wavelength as determined by (4.11)-(4.12) in the striped vegetation patterned region. Here the line corresponds to.

assertion that. These results are catalogued in Table 4 and represented graphically in Figure 6 by the point of intersection between the vertical line and the linear locus of (4.13).

Observed from Table 2 and Figure 14, that stripes of this sort, occurring at the upper bound of allowable - values for such patterns in what we have classified as the semiarid region by Figure 3, are of the lower-threshold variety. In order to obtain the required 2 to 1 width ratio between stripes and interstripes, it is only necessary that we adopt a critical threshold of [2] . Note that this corresponds to the lower threshold part of Figure 9 which was for a threshold value of since when. Anticipating this result, that part of Figure 9 has been employed as the representative lower-threshold stripe pattern in Figure 14. Hence our prediction of vegetative parallel stripes is in both good qualitative and quantitative agreement with these tiger bush patterns made up of acacia trees.

We conclude this discussion with an ecological interpretation of the hexagonal close-packed vegetative distribution of gaps and rhombic arrays of pseudo gaps also predicted in the region classified as semiarid in Table 3. Such patterns are generally identified with pearled or spotted bush made up of bare spots uniformly distributed in dense vegetation or vegetative nets within which interior patches of low density occur [8] . In this context, Deblauwe et al. [22] reported a region in Sudan where only gapped and one-dimensional isotropic vegetative patterns occurred with a transition from the former to the latter as rainfall decreased. An occurrence of this sort is consistent with our model’s morphological predictions summarized in Table 3.

We close by discussing our results in relation to those obtained for the Gray-Scott chemical reaction-diffusion model system. Recently, van der Stelt et al. [23] performed a nonlinear stability analysis in the limit of large advection on a one-dimensional version of what they termed a Generalized Klausmeier-Gray-Scott model, which when restricted to Fickian diffusion can be shown to be equivalent to the one treated by Ursino [24] who performed a linear stability analysis of the Klausmeier model including surface water diffusion as well. Further, van der Stelt et al. [23] stated that the nonlinear stability results of Morgan et al. [25] on the one-dimensional Gray-Scott model were strongly related to the corresponding ones of Kealy and Wollkind [2] . To show the

Table 4. Parameter values for acacia trees relevant to tiger bush patterns of wavelength 150 m.

validity of this statement, we first need to consider the Gray-Scott nondimensionalized reaction-diffusion model system [26] for the chemical species and where a two-dimen- sional co-ordinate system and time given by

(4.14)

(4.15)

defined on an unbounded planar domain. Here, and are the species diffusion coefficients while F and k represent flow and reaction rates, respectively. Now introducing the rescaled variables and parameters

(4.16)

where

(4.17)

system (4.14)-(4.15) is transformed into our interaction-diffusion model system (1.1)-(1.2). van der Stelt et al. [23] formulated their Generalized Klausmeier-Gray-Scott model from the traditional Gray-Scott model (4.14)- (4.15) by adding an advection term of the form

(4.18)

to the right-hand side of (4.14) and letting

(4.19)

in (4.15) where E was an unconstrained constant independent of F. Then from (4.17) and (4.19) we can make the identification that

(4.20)

Observe that when and this reduces to the one-dimensional Gray-Scott model system analyzed by Morgan et al. [25] . Then by virtue of the conversion demonstrated above that model is isomorphic to the one-dimensional Kealy-Wollkind [2] interaction-diffusion system (1.1)-(1.2) with.

So far we have limited our discussion to analyses for which the wavenumber was restricted to the critical wavenumber of linear stability theory alone. In order to investigate the consequence of considering other wavenumbers in the instability sideband centered about this critical wavenumber, we would need to convert our Landau-type amplitude equations in time to Ginzburg-Landau partial differential equations by adding the appropriate spatial derivative terms to them. That was precisely what Morgan et al. [25] did in their analysis of the Gray- Scott model. In particular for (,) and (,), they showed that stationary periodic solutions would occur in a subinterval of that instability interval (the so-called Busse bubble of the Eckhaus side-band). Given the isomorphism just described, this result may be directly applied to our problem. Then, as reviewed in detail by Wollkind et al. [12] , a two-dimensional analysis would yield two additional instabilities besides these parallel modes: Namely, zig-zag and cross-band relevant to the interaction of oblique and perpendicular modes, respectively. In the semiarid and arid regions of Table 3 where stable parallel stripes are predicted, the equivalence class designated as II in Section 2 actually contains three solutions making angles of 60˚ with each other, no two of which can be stable simultaneously [27] . All of these modes when randomly selected by initial conditions can collectively produce quite complicated labyrinthine mazes [8] , which are also characteristic of certain tiger bush vegetative patterns found in arid flat environments [19] . Such an occurrence is also consistent with the type of isotropic one-dimensional patterns found by Deblauwe et al. [22] in the Sudan region described earlier.

Note that the parameter values (,) and (,) for the Gray-Scott system (4.14)-(4.15) relevant to modeling its specific chemical reaction do not produce Turing patterns [28] . This raises the question of over what parameter ranges our results are valid. From condition (2.1) and the fact that, we require

(4.21)

This condition is certainly satisfied by the ecologically meaningful and ranges depicted in Figure 1 ([3] [5] ) for which

(4.22)

When (4.21) is violated, Klausmeier’s [3] nonspatial model can produce limit cycles oscillating about the community equilibrium point or excitable behavior related to the trivial equilibrium point Note that the Gray-Scott model system (4.14)-(4.15) having no parameter restriction of this sort behaves very differently. Thus not all results deduced for that chemical reaction can be directly extended to our ecological interaction.

Finally, recalling that is the community equilibrium point of the Kealy-Wollkind [2] interaction-diffusion model system (1.1)-(1.2), then from (4.16)-(4.17)

(4.23)

represents the corresponding equilibrium point of the Gray-Scott reaction-diffusion model system (4.14)-(4.15). Hence from (4.17) and (4.23) we may conclude that

(4.24)

which is equivalent to (3.19).

We end by restating von Hardenberg et al.’s [18] contention that the power of model systems such as ours of (1.1)-(1.2) is their predicted sequence of stable states along a rainfall gradient can be used to motivate aridity classification schemes of the sort offered in Table 3 that, in general, can be characterized by three rainfall thresholds

(4.25)

which, when particularized to for acacia trees, become

(4.26)

Here we are employing the notation of von Hardenberg et al. [18] for these three rainfall thresholds and in Table 3 introduced the following possible aridity classes based upon the inherent vegetative states of our system:

Dry-subhumid―The only vegetative state the system supports corresponds to a uniform homogeneous distribution.

Semiarid―The only vegetative states the system supports correspond to gaps and pseudo gaps or stripes of lower threshold type.

Arid―The only vegetative state the system supports corresponds to stripes of upper threshold type.

Hyperarid―The only possible stable state the system supports is bare ground.

As noted by von Hardenberg et al. [18] the utility of the prospective aridity classification scheme is that it allows for future predictions for a dryland region based upon its present vegetative state. Recalling that the bare ground state always exists and is stable, regions whose aridity classes imply only the existence of this stable state or its coexistence with the occurrence of upper threshold vegetative patterns are vulnerable to desertification which can then be reversed by the land management strategies of crust disturbance for soil, seed augmentation for plants, and irrigation for surface water. Meron et al. [29] provided a positive-feedback cycling mechanism to explain the formation of bare patches characteristic of vegetative patterning along such a precipitation gradient. Note that a process of this sort occurs in all directions for bare gaps or pseudo gaps but only in two directions for bare interstripes.

In summary, after reprising the one-dimensional and hexagonal planform results of Kealy and Wollkind [2] for their interaction-diffusion plant-surface water model system in an arid flat environment, we extended that analysis by performing a rhombic planform analysis as well. We found that, although square vegetative patterns could not occur for our system, rhombic arrays of other characteristic angles included in two bands flanking were allowable. These occurred in that region of our diffusive instability parameter space where only stable gapped patterns but not stripes or uniform homogeneous distributions were predicted by the hexagonal analysis. Defining a critical plant biomass threshold to interpret such rhombic arrays, those patterns were of a lower threshold type or pseudo gaps.

Our main result could be represented by closed form plots in the rainfall a versus plant loss dimensionless parameter space for an appropriate fixed value of plant biomass-surface water diffusivity ratio. Since the upper boundary of the region where gaps can occur virtually coincided with the Turing marginal stability curve in that parameter space, we took them to be equivalent. Under this simplification, we identified regions in that parameter space corresponding to bare ground, stationary striped vegetative patterns of upper plant biomass threshold type, bistability between vegetative gaps and stripes or pseudo gaps of lower plant biomass threshold type, and homogeneous distributions of vegetation as the rainfall parameter a was increased. Then that predicted sequence of stable states along a rainfall gradient was shown to be in agreement with tiger and pearled bush patterns observed on arid plateaus. In addition, we showed our system to be isomorphic to the Gray-Scott chemical reaction-diffusion model and used that isomorphism to draw some conclusions about side-band instabilities as applied to vegetative pattern formation.

Finally, we introduced an aridity classification scheme, with classes based upon the inherent vegetative patterns included in that predicted morphological sequence along a rainfall gradient, which could be used both to forecast the possibility of desertification and to propose land management strategies to reverse this process. Implicit to our continuum formulation were the assumptions that the pattern wavelength was much greater than the mean coverage diameter of an individual plant but much less than the length scale characteristic of the arid environment which allowed us to have considered our interaction-diffusion equations on an unbounded spatial domain [30] .

We conclude by noting that although these results of our weakly nonlinear stability analyses are only asymptotically valid in the neighborhood of the marginal stability curve and the Go-Gub acacia tiger bush example as well as the occurrence of the rhombic vegetative arrays were restricted to such a region, numerical simulations of pattern formation for several reaction-diffusion systems or model evolution equations have shown that theoretical predictions of this sort can often be extended to those regions of the relevant parameter space relatively far from the marginal curve [8] [31] .

Appendix

Defining the vectors

and the matrix operators

we catalogue the explicit formulae for the Landau constants appearing in Kealy and Wollkind [2] :

(A.1)

where

with

for and 2; and

(A.2)

and

(A.3)

where

with

and

Observe, as Wollkind and Stephenson [7] have pointed out, that the expression for does not contain the component since its coefficient vanishes identically in this limit by virtue of the formula for and hence is often referred to as a free mode.

Finally, we catalogue the components relevant to the second rhombic-planform third-order Landau constant of (3.9)-(3.10):

where

for; and

Conflicts of Interest

The authors declare no conflicts of interest.

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