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Fixation Probability and Time in Subdivided Populations
Michael C. Whitlockaa Department of Zoology, University of British Columbia, Vancouver, British Columbia V6T 1Z4, Canada
Corresponding author: Michael C. Whitlock, University of British Columbia, 6270 University Blvd., Vancouver, BC V6T 1Z4, Canada., whitlock{at}zoology.ubc.ca (E-mail)
Communicating editor: D. CHARLESWORTH
| ABSTRACT |
|---|
New alleles arising in a population by mutation ultimately are either fixed or lost. Either is possible, for both beneficial and deleterious alleles, because of stochastic changes in allele frequency due to genetic drift. Spatially structured populations differ from unstructured populations in the probability of fixation and the time that this fixation takes. Previous results have generally made many assumptions: that all demes contribute to the next generation in exact proportion to their current sizes, that new mutations are beneficial, and that new alleles have additive effects. In this article these assumptions are relaxed, allowing for an arbitrary distribution among demes of reproductive success, both beneficial and deleterious effects, and arbitrary dominance. The effects of population structure can be expressed with two summary statistics: the effective population size and a variant of Wright's FST. In general, the probability of fixation is strongly affected by population structure, as is the expected time to fixation or loss. Population structure changes the effective size of the species, often strongly downward; smaller effective size increases the probability of fixing deleterious alleles and decreases the probability of fixing beneficial alleles. On the other hand, population structure causes an increase in the homozygosity of alleles, which increases the probability of fixing beneficial alleles but somewhat decreases the probability of fixing deleterious alleles. The probability of fixing new beneficial alleles can be simply described by 2hs(1 - FST)Ne/Ntot, where hs is the change in fitness of heterozygotes relative to the ancestral homozygote, FST is a weighted version of Wright's measure of population subdivision, and Ne and Ntot are the effective and census sizes, respectively. These results are verified by simulation for a broad range of population structures, including the island model, the stepping-stone model, and a model with extinction and recolonization.
THE rate of evolution is determined by the balance between the changes in frequency of beneficial and deleterious alleles. If important alleles are always present in populations in large numbers of copies, then the rate of evolution will be deterministic, with beneficial alleles always increasing in frequency and deleterious alleles decreasing. However, if the product of the effective population size and mutation rates is small enough, then there will not always be "large" numbers of each allele in a population at any given time. Indeed, for the range of population sizes experienced by many (or most) species, all possible alleles are not present at any given time. Many alleles are therefore present initially as a single copy, and even in a large population the future of this allele will depend on stochastic processes. If the rate of evolution is limited by the occurrence and fixation of these new mutations, rather than relying on a pool of standing variation for adaptive change, then the rate of evolution will depend on the probability of fixation of these new mutations.
Furthermore, if population size is small enough, deleterious alleles will occasionally fix in species by genetic drift, and this can cause a decline in mean fitness, perhaps even to extinction (![]()
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The first approach to this problem of finding the probability of fixation of a new mutation was made by ![]()
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Spatial population structure was introduced to the study of fixation by ![]()
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This article uses Kimura's diffusion methods with some recent results on spatially structured populations to find the probability of fixation of beneficial or deleterious alleles with arbitrary dominance, allowing for a broad diversity of population structures. All previous results are obtained as special cases. Furthermore, the expected times to fixation and loss are calculated. These analytic results make several assumptions, but simulations show that the results are, perhaps surprisingly, fairly robust to deviations from these assumptions.
| KIMURA'S DIFFUSION RESULTS |
|---|
![]()
![]()
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x) and the variance in that change (V
x) as a function of allele frequency (x). V
x is given by x(1 - x)/2Ne, where Ne is the diploid variance effective population size. Following Kimura, we write the indefinite integral
(or, more properly,
). The probability of fixation can be found as
![]() |
(1) |
where u[p] is the probability of fixation for an allele initially at frequency p. If the function M
x is of the form M
x =
x(1 - x) (as it is in the simplest case of additive, directional selection in an ideal population), then the integrals in Equation 1 can be solved to give
![]() |
(2) |
If the fitnesses of diploid individuals carrying 0, 1, or 2 copies of the allele in question are 1, 1 + s/2, and 1 + s, respectively,
in the previous equation can be replaced by s/2. If s > 0, such that this allele is beneficial, then for alleles of relatively weak effect the probability of fixation of an allele present in the population as a single copy turns out to be
sNe/N. In an ideal population, such that Ne = N, this recreates Haldane's result of u = s, for p = 1/2N. [Note that, for consistency with later notation, the heterozygous effect has been defined as s/2 here, rather than the more traditional s in ![]()
![]()
x, such as that which occurs with arbitrary dominance, the integrals in Equation 1 may have to be solved numerically.
The diffusion approach makes several assumptions. First, it assumes that the state of a population at any given time can be described by its allele frequency, meaning that the history of the population is unimportant except as described by the current allele frequency. With population structure, many different states of the metapopulation have the same mean allele frequency. An additional assumption required for the approach below is that some description of the population structure does not change much over time. Wright's FST can take this role.
The second assumption of the diffusion approach is that the changes in allele frequency per generation are small enough that the process can be adequately described by a continuous-time approximation. In practice this requires that the effective population size is not too small and the strength of selection is not too large (s << 1). Finally, the diffusion approach assumes that the third and higher moments of change in allele frequency per generation are negligibly small. As simulations indicate, the robustness of these assumptions is not much affected by adding population structure to the model. See ![]()
| PROBABILITY OF FIXATION IN A METAPOPULATION |
|---|
Diffusion models and metapopulations:
With some recent results on evolution in subdivided populations, Kimura's approach can be easily modified to reach results about the probability of fixation of alleles in metapopulations. The amount of genetic drift in metapopulations has recently been described (![]()
![]()
where
is the mean frequency of an allele (weighted by local population size). This formulation accounts for not only the random changes in allele frequency due to drift in a single generation, but also the long-term effects of these changes (caused, for example, by correlations over time in the differential success of demes). This formulation allows the demographic properties of each deme to change over time, but does assume that the metapopulation has reached a dynamic equilibrium, such that the distribution of demographic states is constant over time. Note that when each deme is weighted by its size, the mean frequency of an allele is also its frequency in the metapopulation as a whole. Thus it remains to find the expected change in allele frequency in a metapopulation due to selection. A recent article (![]()
For diploid individuals, the relative fitnesses of the three possible genotypes are defined to be 1, 1 + hs, and 1 + s, respectively, for 0, 1, or 2 copies of the x allele. Assume for now that there is random mating within each deme such that the genotypes are present in local Hardy-Weinberg proportions. The distribution of allele frequencies across populations can be described usefully by a variation of Wright's FST, where
and V[x] is the variance among demes in allele frequency, weighted by population size. Note that this differs from the standard definition of FST by weighting each individual, but not necessarily each population, equally.
The individuals in each deme may contribute to the following generation in two ways: they can have offspring that remain in the same deme as residents and offspring that migrate to other demes. The total contribution of a deme to the next generation is the sum of these offspring individuals, regardless of whether they migrate or not. If the total contribution of a deme is independent of the genotypes in the deme (but instead depends on the total resources available to the deme and/or the luck of the deme with respect to local catastrophes, etc.), then I refer to this as soft selection (see ![]()
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When all local populations contribute to the next generation independently of their genotype frequencies (soft selection), the change in allele frequency over a generation in a metapopulation is approximately
![]() |
(3) |
where to order s2
![]() |
(4) |
(![]()
![]() |
(5) |
as expected. Note that this additive case is proportional to
(1 -
), so the corresponding ratio M
x/V
x will not be a function of the allele frequency; therefore Kimura's equation can be solved directly.
When the expected contribution of a deme to the next generation is proportional to its mean fitness determined by its distribution of genotypes, (hard selection) causes the allele frequency to change over generations as
![]() |
(6) |
where
![]() |
(7) |
(![]()
![]() |
(8) |
which is again a function of order
(1 -
). As pointed out in the previous article (![]()
soft is therefore approximately equal to (1 - r)
hard, where r is the relatedness of individuals within a deme (r
2FST/(1 + FST)). Hard selection in a structured population is always more effective than selection in an undivided population because of the increased frequency of homozygotes, as long as h < 1.
With these equations for the mean and variance of the overall allele frequency of the set of populations, an approximation of the probability of fixation can be found by putting M
x and V
x into Equation 1. This is an approximation, not only because the diffusion itself is an approximation as discussed above, but also because the true system of equations describing a set of populations would be a complex set of separate diffusion equations for each local population. We see that the simpler approximation using the overall allele frequency change with FST values determined by neutral equilibrium expectations does extremely well, surprisingly so, to predict the actual probabilities of fixation.
Additive beneficial alleles:
General model:
For the additive cases, as suggested above, the integration in Equation 1 is simple. In fact,
in the single population case in the previous section can be replaced by s(1 - FST)/2 with soft selection or by s(1 + FST)/2 with hard selection. Thus we can write
![]() |
(9) |
for soft selection and
![]() |
(10) |
for hard selection. For beneficial alleles in a large metapopulation, the denominator of these functions will be approximately unity, and the frequency of a new allele present as a single copy will be 1/2Ntot (where Ntot is the total census size of the metapopulation), so that the probability of fixation of a new weakly beneficial allele will be approximately
![]() |
(11) |
for soft selection or
![]() |
(12) |
with hard selection. Given that the variance effective population size of a subdivided population is likely to be lower than its census size and lower than the Ne of an undivided population with the same number of individuals (![]()
Strictly speaking, the value of FST used in these equations should be the expected value for an allele under the same selection as the alleles in question. Finding this value is difficult, however. Fortunately, for relatively weakly and uniformly selected alleles, the FST expected for neutral variation does an excellent job of predicting the FST of selected alleles (![]()
![]()
The island model and stepping-stone models:
The island model and other models with conservative migration have been considered previously (![]()
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(13) |
Changing the fitness function from 1:1 + s/2:1 + s to the 1:1 + s:1 + 2s assumed in the previous work, the current equation is in complete agreement for these reduced cases with completely conservative migration. For example, with a one-dimensional stepping-stone model and an additive beneficial allele, simulation results show that Equation 13 is quite accurate for weak selection. However, these models are aberrant in one significant way: the variance among populations in reproductive success is set to a minimum, zero. Each population contributes exactly equally to the following generation. This mathematical convenience does not reflect biological reality, unfortunately. For more realistic cases where migration is not completely conservative, such that there is some variance in mean fitness among populations, the effective population size is no longer given by Ntot/(1 - FST) and the probability of fixation is no longer given by s. Such cases are dealt with next.
Extinction-recolonization models:
The only other models of population structure that, to my knowledge, have been considered analytically for the probability of fixation of alleles are two analyzed by ![]()
The extinction-recolonization model to be considered here derives from a model introduced by ![]()
![]()
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that two individuals in a colonizing group come from the same source population. Otherwise the metapopulation functions like an island model, with each extant population exchanging m of its individuals equally among all other populations at random each generation.
Barton considered two special cases of recolonization, one where a new population was founded by a single haplotype (k = 1/2) and another where the population was founded at carrying capacity by individuals chosen at random from the rest of the large metapopulation (k = N,
= 0). In these cases, the probabilities of fixing a new beneficial allele, making the nomenclature consistent with the rest of this article, are
![]() |
(14) |
and
![]() |
(15) |
respectively (![]()
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![]() |
(16) |
and
![]() |
(17) |
(![]()
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Simulations confirm that these equations are in fact successful at predicting the probability of fixing new beneficial alleles. Fig 1 shows the correspondence between the theoretical approximation and the simulation results. The approximations involved in using the diffusion approximation and in using the neutral value of FST work extremely well.
|
Hard and soft selection:
The examples in the previous sections have all assumed that the productivity of a deme is unrelated to its genotype frequencies; i.e., they have assumed soft selection. When the fitness of a deme does affect its productivity (hard selection), selection is more effective, because competition among relatives no longer hinders the response to selection. The productivity of a deme includes not only the migrants that it gives to other demes, but also the resident individuals that descend from local individuals (see ![]()
For example, consider a modified island model, where the total contribution of a deme is determined by the product of its current size and its relative mean fitness. A deme with higher fitness grows proportionally, and its contribution to the migrant pool increases accordingly. Each individual has a constant probability of emigrating, and the total metapopulation size is held constant. All demes receive the same number of immigrants from the migrant pool each generation. As long as s < m, the new allele will migrate out of its original deme before it reaches fixation there, and the FST of the system will be well approximated by the neutral FST (![]()
|
Source-sink metapopulations:
For many (or most) structured populations, the contribution to the next generation varies substantially among demes. This variance in reproductive success causes a reduction in the effective population size, and we have already seen the effects of such variance in the section on extinction and colonization. However, sometimes this variance among demes in reproductive success is maintained across generations; that is, the most successful demes continue to be successful and unproductive demes also remain so. This generates a correlation in reproductive success across generations, which also decreases the effective population size (![]()
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|
Beneficial alleles with arbitrary dominance:
With partially recessive alleles (h
1/2), such that the fitness of the heterozygote is not exactly halfway between the fitness of the two homozygotes, the mean change in allele frequency is no longer of order
(1 -
), but it has higher-order terms in mean allele frequency. (See Equation 3, Equation 4, Equation 6, and Equation 7 above.) As such, it is not possible to explicitly solve the integrals to find a closed-form solution to the probability of fixation.
For beneficial alleles, however, an allele is very likely to fix once it is present in the metapopulation at a sufficient frequency that deterministic forces become paramount. For rare beneficial alleles, it is usually sufficient to calculate the value of M
x assuming the new allele is rare enough that terms of order
3 can be ignored. This gives
![]() |
(18) |
and
![]() |
(19) |
such that the probability of fixation is expected to be
2
sNe/Ntot, where the appropriate
is used depending on the nature of competition among populations.
These approximations work so well that the differences between the more exact and approximate results are not visible on a graph, except for the case when both h and FST are very close to zero. Complete recessivity (h = 0) causes the allele frequency change to behave very differently from the case of partial recessivity in panmictic populations (![]()
Fig 4 shows the probability of fixation of beneficial alleles with arbitrary dominance for a range of values of FST. While dominant alleles are always more likely than recessive alleles to fix for a given homozygous effect, population structure allows a much higher probability of fixation for recessive alleles than does panmixia, as long as the effective population size is not much affected (see Fig 4, left). Note that for hard selection, the probability of fixation is always higher (for h < 1) with population structure, if the effective population size is unaffected. With soft selection, recessive beneficial alleles may be much more likely to fix with structure, because they can be expressed during the critical phase when they are rare. However, soft selection with population structure hinders the fixation of dominant alleles, because these alleles gain nothing in fitness when expressed as homozygotes when rare, but lose from the competition between relatives within local populations caused by soft selection. This is all true with an island model or other models of conservative migration, although for models with a high rate of extinction or other variation among populations in reproductive success, the reduction in Ne that results can cause population structure to reduce the probability of fixation of even recessive alleles. With an extinction-colonization model, the probability of fixation can be much reduced relative to panmixia (see Fig 4 and Fig 5A).
|
|
A stronger test of the robustness of the assumptions of the diffusion approximation is a one-dimensional stepping-stone model. Here the probability of fixation is much increased relative to a panmictic population for recessive beneficial alleles, due to both the increase in Ne and the increased expression of recessive beneficial alleles when rare. Fig 5B shows simulation results for the stepping-stone model, where it can be seen that for all parameters examined with biologically reasonable FST values and weak selection, the diffusion approximation does remarkably well.
Deleterious alleles:
Equation 1 can be used to determine the probability of fixation of deleterious alleles as well. With deleterious alleles, the relative fitness of the allele at all frequencies affects the probability of fixation, not just its fitness when rare. This is because an unconditionally deleterious allele never increases deterministically at any allele frequency. Therefore fewer approximations can be made. For the additive case, the closed-form equations in (9) and (10) are accurate; for arbitrary dominance, the answer must be left in integral form. The probability of fixation, as given by Equation 1, resolves to
![]() |
(20) |
where erf[x, y] = erf[y] - erf[x], and A = (FST + (1 - FST)h)
, B = (1 - (1 - FST)h)
, C = (1 - (1 - FST)(1 - h - p + 2hp))
, and
![]() |
(21) |
where b is a measure of the relative strength of hard selection. (b = 0 corresponds to soft selection; b = 1 means hard selection. See ![]()
|
Note that, unlike the case with beneficial alleles, the probability of fixation does not depend heavily on the dominance coefficient h but is almost entirely determined by Ne and s. This is especially the case with population structure, since many of the deleterious effects of alleles are now expressed in homozygous form anyway. The effect on fixation of deleterious alleles from population subdivision is determined mainly by Ne: if subdivision reduces Ne, then deleterious alleles are more likely to fix than those in an undivided population (see Fig 7).
|
| DRIFT LOAD AND FIXATION FLUX IN A METAPOPULATION |
|---|
With recurrent deleterious mutations that have a nonzero probability of fixation, the mean fitness of a species would be expected to decline due to repeated fixations of harmful alleles via drift, all else being equal (![]()
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Not enough is known about the rate and distribution of effects of new mutations. Therefore, to study this we need to use an arbitrary distribution that has many of the properties one might expect the actual distribution to have. Therefore let us assume that the effects of new mutations of either beneficial or deleterious effect are drawn from a gamma distribution. For this section, let us also assume that new mutations are all additive. Then the expected change in fitness per generation due to new deleterious alleles is the product of the number of new deleterious mutations per genome times the number of genomes times the probability of their fixation times their effect, integrated over all possible mutational effects. Putting these together we can find the rate of change per generation of mean fitness due to new deleterious mutations,
![]() |
(22) |
where UD is the diploid genome deleterious mutation rate, u[p, s] is the probability of fixation of an additive allele given initial frequency p and selection against homozygotes of s, and
D[s] is the distribution of deleterious homozygous effects. [Note that this differs from the usage in ![]()
D| and coefficient of variation CD, we find
![]() |
(23) |
where
= (1 - FST) or (1 + FST) (for soft or hard selection, respectively) and
is the generalized Riemann zeta function. This corresponds exactly to the results given in ![]()
. If C2D
Ne|
D| >> 1, the
term will be between 1 and 1.65.
Similarly, we can find the flux in fitness due to new beneficial mutations:
![]() |
(24) |
For values of 2C2B
Ne
B > 1,
[2 + 1/C2B, 1/2C2B
Ne
B]
is
(2C2B
Ne
B)2+1/C2B. Thus we get
![]() |
(25) |
The equilibrium point where fitness is unchanging (
WB +
WD = 0) can be found using the approximations for the zeta functions mentioned above. Then, the critical Ne (above which the species can persist indefinitely) can be found. If both beneficial and deleterious alleles follow an exponential distribution (so CD and CB are both 1), this becomes
![]() |
(26) |
The critical effective size is changed by a factor of 1/
compared to a panmictic population with the same mutational properties.
Note that Ne may not stay constant as new alleles fix in a population. If fixation of deleterious alleles increases the extinction rate of demes or decreases the effective migration rate among demes, then Ne can be reduced, potentially by a substantial margin. Then population structure can feed back into the probability of fixation and increase the probability of mutational meltdown. ![]()
| TIME TO FIXATION |
|---|
![]()
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(27) |
where
![]() |
(28) |
These equations are robust when applied to fixation in a subdivided population. Evaluation of these equations requires numerical integration (even for the panmictic case with selection), and this has been done using Mathematica 4.0.
These equations match well with simulation results. Fig 8 shows that the time to fixation is well predicted by Equation 27 for metapopulations with local extinction and recolonization. Fig 9 shows that even with a stepping-stone structure, the time to fixation is well predicted by the diffusion results.
|
|
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The calculations for the time to loss of an allele, also given by ![]()
| LIMITS TO THE APPROXIMATIONS |
|---|
The diffusion approximations used in this article have their limitations. In particular, it has been assumed that (1) selection is weak, (2) FST is constant, and (3) neutral descriptions of population structure are approximately valid for weak selection. Let us explore these assumptions in turn.
The weak selection assumption is common to all diffusion models. In principle, the strength of selection should be weak enough that terms involving s2 and higher can be ignored. Fig 10 shows that the accuracy of the probability of fixation results drops as the strength of selection increases. In particular, the probability of fixation predicted by Equation 1 is an underestimate of the true probability of fixation. However, this is true even for undivided populations, but not to such a large degree. The time to fixation is still accurately predicted with strong selection (see Fig 10B.).
|
The second assumption, that FST is constant, is required for the time homogeneity assumption of the diffusion model to hold. In reality, the actual value of FST is likely to fluctuate as a result of the stochastic nature of pedigrees, but it seems from the agreement with the simulations that it is sufficient that the expected value of FST be the same for all stages of the selection process. This assumption seems to be potentially the weakest of the assumptions made by the application of the diffusion equation to population structure. Any setting in which the equilibrium FST would be reached slowly relative to the change of allele frequencies by selection would seem a priori to be unlikely to be well described by the diffusion model with a constant FST. Nevertheless, the simulations show that the model works well, much better than might be expected.
Finally, to use the results from this article it is necessary that the expected value of FST is known, and for most cases we know only the expected values of FST for neutral alleles. While FST for selected loci can differ strongly from that expected with neutral loci (![]()
![]()
| DISCUSSION |
|---|
Over the last century, we have come to know more and more about the fates of new mutations. The history of the study of the probability of fixation is one of increasing generality. First, the classic results of ![]()
![]()
2hs. ![]()
2hsNe/Ntot. Moreover, KIMURA's (1964) method turns out to be useful in even more general scenarios, such as those considered here. Population structure was added by ![]()
![]()
We have seen that the diffusion model generates results that are surprisingly useful for systems with spatial population structure. KIMURA's (1964; ![]()
This generality is a bit surprising, given that the assumptions of the diffusion are flagrantly abused by the inclusion of spatial structure. Most importantly, the pattern of spatial genetic differentiation will change as an allele increases in frequency, in a way that is not expected to be perfectly described by neutral FST, as has been assumed here. Yet simulations show that diffusion equations do very well to describe the probability and time to fixation of new alleles, even with neutral predictions of FST.
One of the most striking implications of the success of these equations is that the values of Ne and FST derived from neutral models of subdivided populations can be used to predict the probability and time of fixation of beneficial and deleterious alleles. There is extensive literature about the expected patterns of FST for a variety of models; moreover, it is relatively straightforward to calculate FST for any arbitrary neutral model. The variance Ne of a subdivided population can generally be calculated from the equations in ![]()
![]()
The most important effects of population structure entering the equations on probability or time of fixation are caused by changes in the effective population size. Population structure can either increase (as in the island model) or decrease (as is the case with local extinction and colonization or source-sink dynamics) the effective size of a species, for a given census size. When Ne /Ntot is reduced, the probability of fixation of beneficial alleles is decreased proportionally, and the probability of fixing deleterious alleles is increased. For both beneficial and deleterious alleles, the time to fixation is substantially shortened as Ne is reduced.
In addition to the changes in Ne caused by spatial structure, the pattern of genetic differentiation associated with population structure can cause an increase in competition between relatives (with soft selection). As a result, the mean change of allele frequency associated with selection is reduced. This in turn makes beneficial alleles less likely to fix, deleterious alleles more likely to fix, and the total time to fixation increase. With a traditional island model or stepping-stone model, where there is zero variance in reproductive success among demes and pure soft selection, the effect of this change in the efficacy of selection exactly counterbalances the effects of increasing Ne for additive beneficial alleles; thus the probability of fixation appears unaffected by population structure. Even in these simple cases, however, with deleterious alleles or if there is any dominance to either allele, population structure affects fixation probability.
If a new allele is partially recessive to the ancestral allele, population structure can have yet another effect: allowing the expression of recessive phenotypes because of increased homozygosity. A new beneficial recessive allele can be much more likely to fix with population structure because of this effect. Ignoring the effects of the change in Ne, which could be in either direction depending on the case, a new beneficial allele is
(FST + (1 - FST)h)/h times more likely to fix relative to a panmictic population.
In contrast, the fate of deleterious alleles is not much affected by dominance. This difference between beneficial and deleterious alleles reflects a difference in the critical period for fixation of the two types of allele. The fate of a beneficial allele is determined while it is rare and therefore its expression when rare is key. A deleterious allele is constantly subject to loss by deterministic forces and will never reach a frequency at which its future is determined. For the deleterious allele, its fitness at all frequencies is important, and therefore its dominance is less critical.
Most of the examples in this article have focused on soft selection, where the contribution of a deme to the next generation is independent of the local allele frequency. With hard selection, population structure increases the efficacy of selection for all dominance coefficients. In this case, there is an increased expression of homozygotes and therefore more efficient selection, but this is not accompanied by an increase in competition between relatives. Hard selection, all else being equal, allows a higher rate of fixation of beneficial alleles and a lower rate of fixation of deleterious alleles. However, "all else" may not be equal, since the very fact of hard selection requires the possibility of variance among populations in reproductive success. With hard selection, a model with strictly "conservative" migration is impossible, and effective population sizes may be therefore substantially lower.
The results in this article have focused on the case where selection is applied uniformly in all places. Clearly there are many exciting cases in which selection varies dramatically over space. A case can be made that most new mutations are consistently beneficial or deleterious throughout a species, although the proportion of such mutations is presently unknown. ![]()
Finally, we should consider the relevance of the amount of time required for fixation of alleles. Population structure affects the time to fixation mainly in the same way it influences the effective population size. If Ne is much reduced, then the time to fixation is on average much reduced, and the obverse is true if Ne is increased. The time to fixation of a beneficial allele is not invariant with population structure but can change dramatically depending on the details of the demography. A shortened time to fixation of a beneficial allele should, for example, cause the effect of genetic hitchhiking to be increased, since there is less time for recombination with other genotypes. Population structure can be an important determinant for the rate of evolution of a species.
| ACKNOWLEDGMENTS |
|---|
This article benefited greatly from discussion





































