Chapter 9. Coevolution, polygenic traits, and spatial patterns of phenotypic variation Biological Motivation In the previous chapter, we explored how coevolution proceeds in spatially structured environments where gene flow connects isolated populations inhabiting potentially heterogeneous environments. Our primary focus was to understand how gene flow and coevolution interact to shape patterns of genetic polymorphism and genetic differentiation among and within populations when the outcome of interactions depends on a single genetic locus in each species. Although these results informed our understanding of a wide range of naturally occurring species interactions, such as those between M truncatula and S. meliloti, where a small number of genes are thought to be involved, they cannot effectively address the broad swath of species interactions that are mediated by quantitative traits. For instance, the well-studied interactions between wild parsnip XX and parsnip webworm XX are mediated by concentrations of toxic furanocoumarins in the plant and levels of detoxifying enzyme activity in the insect (REFS). Other well-studied interactions that appear to be mediated by quantitative traits include those between the garter snake predator, Thamnophis sirtalis, and its toxic prey, T. granulosa (REFS), and those between the Japanese Camellia and its seed predator XX (REFS), to name only a few. Over the past ten to twenty years, landscape level studies of interactions mediated by quantitative traits have revealed a wide range of interesting phenotypic patterns. For instance, in the interaction between the toxic newt, T. granulosa and its garter snake predator, T. sirtalis, average levels of newt toxicity vary widely across the western United States as do average levels of snake resistance (REFS). Within some regions, newt toxicity and snake resistance are wildly exaggerated, with a single newt carrying enough tetrodotoxin to kill a Tyranosaurus Rex and local snakes possessing such extreme resistance that they can actually manage to ingest these crawling toxic waste dumps (GET REAL FACTS FROM BUTCH; REFS). Overall, when snake and newt populations are studied together across the western Unites States, the pattern that emerges is one where newt toxicity and snake resistance vary in concert, with geographic regions with elevated toxicity generally associated with elevated levels of resistance (REFS). Comparable patterns have been observed in a wide range of interactions (REFS), suggesting that similar evolutionary processes may be driving the evolution of quantitative traits mediating these well-studied species interactions. The central goal of this chapter will be to explore the potential for coevolution to generate these commonly observed phenotypic patterns. In order to achieve this goal, and address the key questions that follow, we need to integrate spatial structure into the quantitative genetic models of coevolution we first developed in Chapter 3. Key Questions: ο· ο· ο· Can coevolution generate phenotypic variation across space? Is there reason to expect exaggerated trait values within regions of intense coevolution? Does coevolution lead to well-matched phenotypes in interacting species? Building a Model of Snake-Newt Interactions Mathematica Resources: http://www.webpages.uidaho.edu/~snuismer/Nuismer_Lab/the_theory_of_coevolution.htm In Chapter 2, we developed a model of coevolution between two species mediated by a quantitative trait and a mechanism of phenotype differences. This model assumes the probability of a “successful” interaction occurring depends on the extent to which the phenotype of one species exceeds that of the other (Chapter 2, Figure X). In the context of interactions between T. sirtalis and T. granulosa, a “successful” interaction is one where the snake successfully consumes the newt, with the probability of consumption depending on the quantity of tetrodotoxin in the newt (π¦Μ ) and the resistance to tetrodotoxin in the snake (π₯Μ ). Being consumed reduces newt fitness (by an amount π π ) and increases snake fitness (by an amount π π ). In addition to selection imposed by the interaction, an extension of this basic model accounted for constraints on toxicity and resistance in the form of stabilizing selection toward optimal trait values ππ and ππ . These assumptions, along with the classical quantitative genetic assumptions of weak selection, fixed additive genetic variance, and Gaussian phenotype distributions allowed us to derive expressions for the population mean phenotypes of the interacting species in the next generation: π₯Μ ′ ≈ π₯Μ + ππ πΊπ + 2πΎπ πΊπ (ππ − π₯Μ ) (1a) π¦Μ ′ ≈ π¦Μ + ππ πΊπ + 2πΎπ πΊπ (ππ − π¦Μ ) (1b) where ππ = πΌ π π 2(2+π π ) and ππ = πΌ π π 2(2−π π ) , and XXX and XXX. In order to use this model to study the spatial patterns that characterize many interactions mediated by quantitative traits, we need to integrate multiple populations and gene flow between them. CAUTION ABOUT THE PERILS OF SPATIAL STRUCTURE, GENE FLOW, AND BIMODALITY π₯Μ π′ ≈ π₯Μ π + ππ,π πΊπ + 2πΎπ πΊπ (ππ − π₯Μ π ) (2a) π¦Μ π′ ≈ π¦Μ π + ππ,π πΊπ + 2πΎπ πΊπ (ππ − π¦Μ π ) (2b) where… Our basic approach will be like that in the previous chapter. We will explore one of the simplest possible spatial scenarios: a pair of populations connected by gene flow at rates X and X. π₯Μ π′′ ≈ (1 − ππ )π₯Μ π′ + ππ π₯Μ π′ (3a) π¦Μ π′′ ≈ (1 − ππ )π¦Μ π′ + ππ π¦Μ π′ (3b) Analyzing the Model We will then clarify and focus our unbderstanding by yusing the change of variables analogous to that we also used in the previous chapter βππ = πΊπ (ππΜ − 2πΎπ (ππ − ππ )) (4a) 2 βπΏπ = −2ππ πΏπ + πΊπ (1 − 2ππ )(πΏππ − 2πΎπ πΏπ ) (4b) βππ = πΊπ (ππΜ − 2πΎ(ππ − ππ )) (4c) βπΏπ = −2ππ πΏπ + πΊπ (1 − 2ππ )(πΏππ − 2πΎπ πΏπ ) (4d) where XXX… Interestingly, (3) shows that the coevolutionary dynamics of average phenotypes are decoupled from the coevolutionary dynamics of spatial structure. We can capitalize on this independence to first solve for the coevolutionary dynamics oif trait means, which is identical to what we did in Chapter 3 and has time depdnent solution: Next, we can study how spatial structure coevolves using (4b,d). Thus, ultimately, we expect coevolution between snake and newt to lead to an equilibrium where: πΜ πΜ π = ππ + 2πΎπ (5a) π (1−2ππ ) πΏπ πΊπ πΏΜπ = 2πΎ πΊ π(1−2π (5b) π )+2ππ π π πΜ πΜ π = ππ + 2πΎπ (5c) π πΏΜπ = πΏππ πΊπ (1−2ππ ) (5d) 2πΎπ πΊπ (1−2ππ )+2ππ So what can we learn from (5)? First, we see that as long as selection mosaics are present in both species, we will observe spatial variability in the population mean phenotypes of the interacting species. In the case of interactions between the snake and newt we would observe spatial variability on newt tetrodotoxin concentrations and snake resistance directly proportional to the strength of the selection mosaics acting on each species. What this implies is that the larger the difference in the fitness consequences of interactions across sites, the greater the difference in population mean trait values (Figure 1). Second, our equilibrium solution clearly shows that the populations with the strongest fitness consequences of interactions (coevolutionary hot spots) will be those where the traits mediating the interaction are most exagereated (Figure 1). Finally, we can use (5) to identify the conditions under which the traits of the interacting species will match, or be positively correlated across space. The easiest way to do this is to recognize that the population mean trait values of the two species will be positively correlated anytime the product πΏΜπ × πΏΜπ is greater than zero. Inspecting this product shows that this can only occur if the product of the selection mosaics, πΏππ × πΏππ , is also greater than zero (Figure 2). Taken together, our results suggest that c 3 Answers to Key Questions: Can coevolution generate phenotypic variation across space? Potentially. Our results show that in a homogenous environment, coevolution alone cannot cause population mean phenotypes to diverge among populations. However, when species interactions impose different fitness consequences in different geographic regions, population mean phenotypes escalate to different degrees. The result of this differential escalation is spatial variation in mean phenotype. Is there reason to expect exaggerated trait values within regions of intense coevolution? Yes. Regions where both species experience strong fitness consequences from interacting, and thus intense coevolution, should be characterized by exaggerated trait values. The extent to which trait values are exaggerated in these coevolutionary “hot spots” depends on the balance between coevolutionary selection and stabilizing selection. Does coevolution lead to well-matched phenotypes in interacting species? Potentially. If both species experience stronger than average selection from species interactions in the same geographic locations and weaker than average selection from species interactions in the same geographic locations, the population mean phenotypes of the two species will be positively correlated and well-matched. Put differently, if the fitness consequences of species interactions are positively correlated, then so too will population mean phenotypes. If, however, the fitness consequences of interactions are uncorrelated or negatively correlated, the population mean phenotypes of the interacting species will also be uncorrelated or even systemically mismatched. New Questions Arising: Our simple model of coevolution between the snake XX and the newt XX has provided us with several interesting insights into the potential for coevolution to generate spatial variation in the quantitative traits mediating the interaction. In addition, our model has also identified conditions under which coevolution is likely to cause the phenotypes of the species to be correlated over space. At the same time, however, our model has ignored other forces that may also generate spatially variable and correlated phenotypes and has focused on only a single class of ecological interaction mediated by a particular functional relationship between quantitative traits. These limitations of our basic model lead to several obvious questions: ο· Can forces other than coevolution produce spatially variable and potentially correlated phenotypes? ο· Are some functional forms of interaction more likely to produce spatial variation and correlation than others? 4 ο· Should we expect mutualistic interactions to produce similar patterns of spatial phenotypic variation and trait correlation? In the next three sections, we will develop extensions and variations of our basic model that allow us to answer these questions and gain further insight into the process of coevolution. Extensions Extension 1: Can forces other than coevolution produce spatially variable and potentially correlated phenotypes? π₯Μ π′ ≈ π₯Μ π + ππ πΊπ + 2πΎπ πΊπ (ππ,π − π₯Μ π ) (6a) π¦Μ π′ ≈ π¦Μ π + ππ πΊπ + 2πΎπ πΊπ (ππ,π − π¦Μ π ) (6b) WARNING: EXPLAIN DANGERS OF DISTANT THETAS AND APPROXIMATIONS… π₯Μ π′′ ≈ (1 − ππ )π₯Μ π′ + ππ π₯Μ π′ (7a) π¦Μ π′′ ≈ (1 − ππ )π¦Μ π′ + ππ π¦Μ π′ (7b) βππ = πΊπ (ππ − 2πΎπ (ππ − ππΜ )) (8a) βπΏπ = −2ππ πΏπ − 2πΎπ πΊπ (1 − 2ππ )(πΏπ − πΏππ ) (8b) βππ = πΊπ (ππ − 2πΎ(ππ − πΜ π )) (8c) βπΏπ = −2ππ πΏπ + 2πΎπ πΊπ (1 − 2ππ )(πΏπ − πΏππ ) (8d) πΜ π = ππΜ + ππ 2πΎπ πΎ πΊ πΏ (9a) (1−2ππ ) π π ππ πΏΜπ = πΎ πΊ (1−2π π π πΜ π = πΜ π + (9b) π )+ππ ππ 2πΎπ (9c) (1−2ππ ) πΎπ πΊπ πΏππ πΏΜπ = πΎ πΊ (1−2π π π (9d) π )+ππ 5 We are now in a good place to use equations (8) to learn more about the potential origins of spatial variation in the traits mediating interactions between species. First, we see that as long as the optimum phenotypes favored by stabilizing selection vary across space so too will the population mean phenotypes of the interacting species. This is true even if coevolutionary selection is entirely absent (e.g., S->0). Second, our equilibrium solution clearly shows that populations where both snake and newt are less constrained will be those where the traits mediating the interaction are most exaggerated (Figure 3). Third, equations (5) allow us to identify conditions under which the traits of the interacting species will match, or be positively correlated across space. The easiest way to do this is to recognize that the population mean trait values of the two species will be positively correlated anytime the product πΏΜπ × πΏΜπ is greater than zero. Inspecting this product shows that this can only occur if the product of the selection mosaics, πΏππ × πΏππ , is also greater than zero (Figure 4). So how do these mathematical results better inform our understanding of the potential causes shaping the remarkable patterns we observe in the snake new interaction? result mean for Returning again to the interactions between snake and newt, this result implies that we will observe spatial variation in toxicity and resistance anytime could, in principle be fooled into believing we had a coevolutionary hot spot if there exist regions where, for whatever reason, stabilizing selection favors larger trait values independent of coevolution. This might occur, if, for instance, the cost of producing tetrodotoxin were less within a population that also imposed reduced costs of modifying your sodium channels… Extension 2: Are some functional forms of interaction more likely to produce spatial variation and correlation than others? π₯Μ π′ ≈ π₯Μ π + ππ πΊπ (π¦Μ π − π₯Μ π ) + 2πΎπ πΊπ (ππ,π − π₯Μ π ) (10a) π¦Μ π′ ≈ π¦Μ π + ππ πΊπ (π₯Μ π − π¦Μ π ) + 2πΎπ πΊπ (ππ,π − π¦Μ π ) (10b) π₯Μ π′′ ≈ (1 − ππ )π₯Μ π′ + ππ π₯Μ π′ (10a) π¦Μ π′′ ≈ (1 − ππ )π¦Μ π′ + ππ π¦Μ π′ (10b) 6 NOW WE MAKE A CHANGE OF VARIABLES AND ALSO ASSUME m is small βππ = ππ πΊπ (ππ − ππ ) − 2πΎπ πΊπ (ππ − ππΜ ) (11a) βπΏπ = −2ππ πΏπ − πΊπ (ππ (πΏπ − πΏπ ) + 2πΎπ (πΏπ − πΏππ )) (11b) βππ = ππ πΊπ (ππ − ππ ) − 2πΎπ πΊπ (ππ − πΜ π ) (11c) βπΏπ = −2ππ πΏπ + πΊπ (ππ (πΏπ − πΏπ ) + 2πΎπ (πΏπ − πΏππ )) (11d) πΜ π = Μ π +ππ πΎπ π Μ π πΎπ (ππ +2πΎπ )π ππ πΎπ +(ππ +2πΎπ )πΎπ πΏΜπ = π πΜ π = (12a) πΊπ (πΎπ (2ππ +πΊπ (ππ +2πΎπ ))πΏππ +πΊπ ππ πΎπ πΏππ ) π (2ππ +πΊπ (ππ +2πΎπ ))+πΊπ (ππ (ππ +2πΎπ )+πΊπ (ππ πΎπ +(ππ +2πΎπ )πΎπ )) Μ π +(ππ +2πΎπ )πΎπ π Μ π ππ πΎπ π ππ πΎπ +(ππ +2πΎπ )πΎπ πΏΜπ = π (12b) (12c) πΊπ (πΊπ ππ πΎπ πΏππ +(2ππ +πΊπ (ππ +2πΎπ ))πΎπ πΏππ ) π (2ππ +πΊπ (ππ +2πΎπ ))+πΊπ (ππ (ππ +2πΎπ )+πΊπ (ππ πΎπ +(ππ +2πΎπ )πΎπ )) (12d) Extension 3: Should we expect mutualistic interactions to produce similar patterns of spatial phenotypic variation and trait correlation? Although interactions … Conclusions and Synthesis 7 Tables Figure Legends References 8