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. 2006 Feb 10;7:9. doi: 10.1186/1471-2156-7-9

Models and partition of variance for quantitative trait loci with epistasis and linkage disequilibrium

Tao Wang 1,3, Zhao-Bang Zeng 1,2,
PMCID: PMC1456990  PMID: 16472377

Abstract

Background

A genetic model about quantitative trait loci (QTL) provides a basis to interpret the genetic basis of quantitative traits in a study population, such as additive, dominance and epistatic effects of QTL and the partition of genetic variance. The standard quantitative genetics model is based on the least squares partition of genetic effects and also genetic variance in an equilibrium population. However, over years many specialized QTL models have also been proposed for applications in some specific populations. How are these models related? How to analyze and partition a QTL model and genetic variance when both epistasis and linkage disequilibrium are considered?

Results

Starting from the classical description of Cockerham genetic model, we first represent the model in a multiple regression setting by using indicator variables to describe the segregation of QTL alleles. In this setting, the definition of additive, dominance and epistatic effects of QTL and the basis for the partition of genetic variance are elaborated. We then build the connection between this general genetic model and a few specialized models (a haploid model, a diploid F2 model and a general two-allele model), and derive the genetic effects and partition of genetic variance for multiple QTL with epistasis and linkage disequilibrium for these specialized models.

Conclusion

In this paper, we study extensively the composition and property of the genetic model parameters, such as genetic effects and partition of genetic variance, when both epistasis and linkage disequilibrium are considered. This is the first time that both epistasis and linkage disequilibrium are considered in modeling multiple QTL. This analysis would help us to understand the structure of genetic parameters and relationship of various genetic quantities, such as allelic frequencies and linkage disequilibrium, on the definition of genetic effects, and will also help us to understand and properly interpret estimates of the genetic effects and variance components in a QTL mapping experiment.

Background

Modeling quantitative trait loci (QTL) started with Yule [1,2] and Pearson [3] (see [4,5] for the early history of quantitative genetics). However, it was Fisher [6] who laid the firm foundation for quantitative genetics. Fisher defined gene effects (additive, dominance and epistatic effects) based on the partition of genetic variance. He partitioned the genetic variance into a portion due to additive effects (averaged allelic substitution effects), a portion due to dominance effects (allelic interactions), and a portion due to epistatic effects (non-allelic interactions) of genes. He then studied the correlation between relatives using the model. Cockerham [7] used the orthogonal contrasts to redefine the additive and dominance effects of QTL and, by extending the contrasts to include epistatic effects, he partitioned the epistatic variance of two loci into those due to additive × additive, additive × dominance, dominance × additive and dominance × dominance effects of QTL. Cockerham then generalized the model to multiple loci. This was further generalized by Kempthorne [8,9] to multiple alleles. This model has been used as the basis for studying quantitative genetics ever since.

However, over years, many specialized models have also been proposed. Some are just special cases of the general genetic model and some are simplified variants tailored for particular applications or interpretations. With the propagation of numerous quantitative genetic models, there have also been some confusions in literature on the definition and interpretation of additive, dominance and epistatic effects of QTL and their relationship to the partition of genetic variance. Also, there has never been a study that considers both epistasis and linkage disequilibrium in the partition of genetic variance for multiple QTL. In this paper, we try to build the connection between the general genetic model and a few other commonly used genetic models to clarify the basis for the interpretation of different genetic models.

We start with an introduction of the genetic model as expressed in [7] in the context of variance components. Then by introducing an indicator variable for each QTL allele, we represent the model in a multiple regression setting and examine the definition and meaning of the genetic effects (additive, dominance and epistatic effects) of QTL and partition of the genetic variance in an equilibrium population and also in a disequilibrium population. Most of previous studies on modeling QTL discuss epistasis only in reference to an equilibrium population. An examination of properties of a model with both epistasis and linkage disequilibrium is important for QTL analysis in both experimental and natural populations. This is another goal of the paper and is studied in great detail here. We discuss a few reduced models used for QTL analysis, such as backcross model (essentially a haploid model) and F2 model. We also give details for a general two-allele model which may be useful for studying the genetic architecture in a natural population using single nucleotide polymorphisms (SNPs).

Previously, in [10], we compared F2 model and the general two-allele model with another commonly used genetic model, called Fmodel. By specifying the basis of definition for each model, we compared the properties of these models in the estimation and interpretation of QTL effects including epistasis and discussed a few potential problems of using Fmodel in a segregating population for QTL analysis. Similarly, we also compared these models with another model proposed by Cheverud [11,12].

An important result of [10] is that the genetic effects defined in reference to an equilibrium population also apply to a disequilibrium population. The partial regression coefficients, that define the genetic effects in a disequilibrium population, equal to the simple regression coefficients in a corresponding equilibrium population – the usual basis to define and interpret a genetic effect including an epistatic effect. Hardy-Weinberg and linkage disequilibria only introduce covariances between different genetic effects. With this result, in this paper our discussion on epistasis and linkage disequilibrium is focused on the partition and composition of genetic variances and covariances between different genetic effects in different populations.

Results

The genetic model

A general genetic model for the partition of genetic variance (particularly epistatic variance) in a random mating population was first given by Cockerham [7,13] and extended to multiple alleles by Kempthorne [8,9], following the basic genetic model formulated by Fisher [6]. The model for two loci A and B with multiple alleles was expressed as follows

Gjlik=μ+αi+αj+δji+βk+βl+γlk+(αiβk)+(αiβl)+(αjβk)+(αjβl)+(αiγlk)+(αjγlk)+(δjiβk)+(δjiβl)+(δjiγlk)     (1)

where the genotypic value Gjlik is the expected phenotype of an individual carrying alleles Ai, Aj, Bk, and Bl with phased genotype AiBk/AjBl formed by the union of a paternal gamete AiBk and a maternal gamete AjBl. The model partitions the total genotypic value into a number of genetic effects which include additive effects of each allele (α's and β's), dominance effects between two alleles at each locus (δ's and γ's), additive × additive interactions between two alleles at two loci ((αβ)'s), additive × dominance interactions involving three alleles ((αγ)'s and (δβ)'s), and dominance × dominance interaction involving all four alleles ((δγ)'s).

As an ANOVA model, it is known that not all the parameters in model (1) are estimable. A number of constraint conditions on these parameters are therefore needed. Let pi, qk denote allelic frequencies for alleles on paternal gametes, and pj, ql allelic frequencies for alleles on maternal gametes. It is usually assumed that a weighted summation of genetic effects is zero over any index for each genetic component as a deviation from the mean. Some examples are

ipiαi=0, ipiδji=0, jpjδji=0,ipi(αiβk)=0, kpk(αiβk)=0,jpj(δjiβk)=0, kqk(δjiβk)=0,      (2)

Under the assumption of random mating and linkage equilibrium and allowing for different allelic frequencies in paternal and maternal gametes, the mean and genetic effects can be expressed as follows based on the least squares principle:

μ=i,j,k,lpipjqkqlGjlik     (3)αi=G..i.G...., βk=G...kG....,αj=Gj...G...., βl=G.l..G....,δji=Gj.i.G..i.Gj...+G....,γlk=G.l.kG...kG.l..+G....,(αiβk)=G..ikG..i.G...k+G....,(αiβl)=G.li.G..i.G.l..+G....,(αjβk)=Gj..kGj...G...k+G....,(αjβl)=Gjl..Gj...G.l..+G....,(αiγlk)=G.likG..ikG.li.G.l.k+G..i.+G...k+G.l..G....,(αjγlk)=Gjl.kGj..kG.l.kGjl..+Gj...+G...k+G.l..G....,(δjiβk)=Gj.ikG..ikGj.i.Gj..k+G..i.+G...k+Gj...G....,(δjiβl)=Gjli.Gj.i.G.li.Gjl..+G..i.+Gj...+G.l..G....,(δjiγlk)=GjlikGj.ikG.likGjli.+Gjl.k+G..ik+Gjl..+Gj.i.+G.l.k+Gj..k+G.li.G..i.G...kGj...G.j..+G....

where G....=i,j,k,lpipjqkqlGjlik, G..i.=j,k,lpjqkqlGjlik, and so on. The total genetic variance is VG=i,j,k,lpipjpkpl(Gjlikμ)2, and has an orthogonal partition under random mating and linkage equilibrium

VG=VA1+VA2+VD1+VD2+VA1A2+VA1D2     (4)+VD1A2+VD1D2

with

VA1=ipi(αi)2+jpj(αj)2VD1=i,jpipj(δji)2VA2=kqk(βk)2+lql(βl)2VD2=k,lqkql(γlk)2VA1A2=i,kpiqk(αiβk)2+j,lpjql(αjβl)2+i,lpiql(αiβl)2+j,kpjqk(αjβk)2VA1D2=i,k,lpiqkql(αiγlk)2+j,k,lpjqkql(αjγlk)2VD1A2=i,j,kpipjqk(δjiβk)2+i,j,lpipjql(δjiβl)2VD1D2=i,j,k,lpipjqkql(δjiγlk)2

Using indicator variables, we can represent model (1) in another form. Assume that the two loci A and B have alleles Ai, i = 1, 2, ..., n1; and Bk, i = 1, 2, ..., n2, respectively. We define the following indicator variables to represent the segregation of alleles in a population.

zMi(1)={1,for Ai allele from paternal gamete0,otherwise.zFj(1)={1,for Aj allele from maternal gamete0,otherwise.

for i, j = 1, 2, ..., n1 at locus A, and

zMk(2)={1,for Bk allele from paternal gamete0,otherwise.zFl(2)={1,for Bl allele from maternal gamete0,otherwise.

for k, l = 1, 2, ..., n2 at locus B. In terms of these indicator variables, we have the following.

• Hardy-Weinberg equilibrium (HWE) implies that {zMi(1), i = 1, 2, ..., n1} are independent of {zFj(1), j = 1, 2, ..., n1}, and {zMk(2), k = 1, 2, ..., n2} are independent of {zFl(2), l = 1, 2, ..., n2}.

• Linkage equilibrium (LE) implies that {zMi(1), i = 1, 2, ..., n1} are independent of {zMk(2), k = 1, 2, ..., n2}, and {zFj(1), j = 1, 2, ..., n1} are independent of {zFl(2), l = 1, 2, ..., n2}.

• There is another type of disequilibrium; i.e., the so-called genotypic disequilibrium [14] for two alleles on different gametes and at different loci. So, the genotypic equilibrium (GE) here means that {zMi(1), i = 1, 2,..., n1} are independent of {zFl(2), l = 1, 2, ..., n2}, and {zFj(1), j = 1, 2, ..., n1} are independent of {zMk(2), k = 1, 2, ..., n2}.

It is known that under random mating we have both HWE and GE, which together are called gametic phase equilibrium. Now, let G denote the genotypic value of a progeny drawn randomly from the current population. Based on Cockerham model, G can be expressed as

G=μ+i=1n1αizMi(1)+j=1n1αjzFj(1)+i,jδjizMi(1)zFj(1)+k=1n2βkzMk(2)+l=1n2βlzFl(2)+k,lγlkzMk(2)zFl(2)+[i,k(αiβk)zMi(1)zMk(2)+i,l(αiβl)zMi(1)zFl(2)+j,k(αjβk)zFj(1)zMk(2)+j,l(αjβl)zFj(1)zFl(2)]+[i,k,l(αiγlk)zMi(1)zMk(2)zFl(2)+j,k,l(αjγlk)zFj(1)zMk(2)zFl(2)]+[i,j,k(δjiβk)zMi(1)zFj(1)zMk(2)+i,j,l(δjiβl)zMi(1)zFj(1)zFl(2)]+i,j,k,l(δjiγlk)zMi(1)zFj(1)zMk(2)zFl(2)     (5)

This is simply a different presentation of Cockerham model with the same constraint conditions applied on the coefficient parameters. For a given individual with genotype AiBk/AjBl, G will take the same value of Gjlik as before. However, this expression is helpful for us to understand some details about each component of genetic effects. We can see this more clearly in the examination of some reduced models later.

In general, the genetic effects can be defined separately for alleles that are paternally and maternally transmitted to account for possible biological differences. As a fully parameterized model for Gjlik, model (3) may give GjlikGjkilGiljkGikjl depending on how genetic effects are defined. If locus A has n1 alleles, and locus B has n2 alleles, there are N = n12n22 possible phased genotypes in total with the partition of the degrees of freedom given in Table 1.

Table 1.

Partition of degrees of freedom for two loci with number of alleles n1 and n2 (a general case)

Source Degrees of Freedom
additive (α) 2(n1 - 1)
dominance (δ) (n1 - 1)2
additive (β) 2(n2 - 1)
dominance (γ) (n2 - 1)2
additive × additive (αβ) 4(n1 - 1)(n2 - 1)
additive × dominance (αγ) 2(n1 - 1)(n2 - 1)2
dominance × additive (δβ) 2(n1 - 1)2(n2 - 1)
dominance × dominance (δγ) (n1 - 1)2(n2 - 1)2

total n12n22 - 1

If we assume that the union of paternal gamete AiBk with maternal gamete AjBl have the same mean effect as that of paternal gamete AjBl with maternal gamete AiBk(i.e., Gjlik=Gikjl), the coupling and repulsion heterozygotes have the same genotypic value (i.e., Gjlik=Gjkil), and paternal and maternal gametes have the same gametic frequency distribution, we do not need to distinguish paternal and maternal effects. In this case, the two loci can be regarded as 2 factors and each factor has ni2 (i = 1, 2) levels produced by the allelic combinations of ni alleles (cf. [7]). The total number of genotypes is N = n1(n1 + 1)n2(n2 + 1)/4 and the partition of degrees of freedom is shown in Table 2. Since in this case, αi = αi, βk = βk, ..., and so on, the model can also be expressed as follows

Table 2.

Partition of degrees of freedom for two loci with number of alleles n1 and n2 (a simplified case without distinguishing the paternal and maternal origins)

Source Degrees of Freedom
additive (α) n1 - 1
dominance (δ) n1(n1 - 1)/2
additive (β) n2 - 1
dominance (γ) n2(n2 - 1)/2
additive × additive (αβ) (n1 - 1)(n2 - 1)
additive × dominance (αγ) (n1 - 1)n2(n2 - 1)/2
dominance × additive (δβ) n1(n1 - 1)(n2 - 1)/2
dominance × dominance (δγ) n1(n1 - 1)n2(n2 - l)/4

total n1(n1+1)2n2(n2+1)21

G=μ+i=1n1αi(zMi(1)+zFi(1))+i,jδjizMi(1)zFj(1)+k=1n2βk(zMk(2)+zFk(2))+k,lγlkzMk(2)zFl(2)+i,k(αiβk)(zMi(1)+zFi(1))(zMk(2)+zFk(2))+i,k,l(αiγlk)(zMi(1)+zFi(1))zMk(2)zFl(2)+i,j,k(δjiβk)zMi(1)zFj(1)(zMk(2)+zFk(2))+i,j,k,l(δjiγlk)zMi(1)zFj(1)zMk(2)zFl(2))     (6)

For the case of an arbitrary number of loci, the situation will become more complicated. In addition to the additive and dominance effects at each locus and two locus interactions (additive × additive, additive × dominance, dominance × additive, dominance × dominance, with a total number of 22 terms), there are 3 locus interactions (additive × additive × additive, additive × additive × dominance, ..., with a total number of 23 terms), 4 locus interactions (additive × additive × additive × additive, ..., with a total number of 24 terms), and so on. Though the extension is straightforward, the total number of terms will increase dramatically. We will show some models with multiple loci in later examples by ignoring trigenic and higher order epistasis.

Effects and variance components

Let pi, pj (i, j = 1, 2, ..., n1) be allelic frequencies of paternal and maternal gametes at locus A, respectively. Let also qk, ql (k, l = 1, 2, ..., n2) denote allelic frequencies of paternal and maternal gametes at locus B, respectively. In the analysis of variance for the model, it is convenient to use deviations of the indicator variables zMi(1), zFi(1), zMj(2) and zFj(2) from their expected values. That is

xMi(1)=zMi(1)E(zMi(1))=zMi(1)pi={1pi,for Ai allele from paternal gametepi,otherwise

Similarly, define

xFj(1)=zFj(1)E(zFj(1))=zFj(1)pjxMk(2)=zMk(2)E(zMk(2))=zMk(2)qkxFl(2)=zFl(2)E(zFl(2))=zFl(2)ql

Taking the constraint conditions on the genetic effects into account, we can show that,

i=1n1αixMi(1)=i=1n1αizMi(1)i,jδjixMi(1)xFj(1)=i,jδjizMi(1)zFj(1)i,k,l(αiγlk)xMi(1)xMk(2)xFl(2)=i,k,l(αiγlk)zMi(1)zMk(2)zFl(2)i,j,k,l(δjiγlk)xMi(1)xFj(1)xMk(2)xFl(2)=i,j,k,l(δjiγlk)zMi(1)zFj(1)zMk(2)zFl(2)

and so on. For example,

i=1n1αixMi(1)=i=1n1αi(zMi(1)pi)=i=1n1αizMi(1)i=1n1αipi=i=1n1αizMi(1)

as i=1n1αipi=0 by the constrain condition (2). Therefore, model (5) can be rewritten as

G=μ+i=1n1αixMi(1)+j=1n1αixFj(1)+i,jδjixMi(1)xFj(1)+k=1n2βkxMk(2)+l=1n2βlxFl(2)+k,lγlkxMk(2)xFl(2)+[i,k(αiβk)xMi(1)xMk(2)+i,l(αiβl)xMi(1)xFl(2)+j,k(αjβk)xFj(1)xMk(2)+j,l(αjβl)xFj(1)xFl(2)]+[i,k,l(αiγlk)xMi(1)xMk(2)xFl(2)+j,k,l(αjγlk)xFj(1)xMk(2)xFl(2)]+[i,j,k(δjiβk)xMi(1)xFj(1)xMk(2)+i,j,l(δjiβl)xMi(1)xFj(1)xFl(2)]+i,j,k,l(δjiγlk)xMi(1)xFj(1)xMk(2)xFl(2)     (7)

When we deal with some reduced models in the next section, we will find that the model of this form is especially helpful as it makes the model parameter constraints built into regression variables which is suited for genetic interpretation. The form of model (7) can also facilitate the demonstration that under Hardy-Weinberg, linkage and genotypic equilibria, the regression coefficients (genetic effects) are Cockerham's least squares effects (3) (Appendix A), and the genotypic variance VG has the orthogonal partition (4) (Appendix B).

Now we discuss the properties of model in a disequilibrium situation. As stated in [14], there are three types of disequilibria

• Typel: between alleles on the same gametes but at different loci

• Type2: between alleles at the same locus but on different gametes

• Type3: between alleles on different gametes and at different loci.

If we denote Pjlik as the genotypic frequency of AiBk/AjBl, Pj.i. as the genotypic frequency of Ai/Aj, and so on, following [14], the digenic disequilibria can be written as

D..ik=Cov(zMi(1),zMk(2))=E(xMi(1)xMk(2))=P..ikpiqkDjl..=Cov(zFj(1),zFl(2))=E(xFj(1)xFl(2))=Pjl..pjqlDj.i.=E(xMi(1)xFj(1))=Pj.i.pipjD.l.k=E(xMk(2)xFl(2))=P.l.kqkqlD.ji.=E(xMi(1)xFl(2))=P.li.piqlDj..k=E(xFj(1)xMk(2))=Pj..kpjqk.

And the trigenic disequilibria

Dj.ik=E(xMi(1)xFj(1)xMk(2))=Pj.ikpiPj..kqkPj.i.pjP..ik+2pipjqkD.lik=E(xMi(1)xMk(2)xFl(2))=P.likpiP.l.kqkP.li.qlP..ik+2piqkqlDjli.=E(xMi(1)xFj(1)xFl(2))=Pjli.piPjl..pjP..i.qlPj.i.+2pipjqlDjl.k=E(xFj(1)xMk(2)xFl(2))=Pjl.kpjP.l.kqkPj..lqlPj..k+2pjqkql

Similarly for the quadrigenic disequilibrium, we may define

Djlik=E(xMi(1)xFj(1)xMk(2)xFl(2))=PjlikpiPjl.kpjP.likqkPjli.qlPj.ik+pipjP.l.kpiqkPjl..+piqlPj..k+pjqkP.li.+pjqlP..ik+qkqlPj.i.3pipjqkql.

If we express Djlik as a function of lower-order linkage disequilibria, we have

Djlik=PjlikpiDjl.kpjD.likqkDjli.qlDj.ikpipjD.l.kpiqkDjl..piqlDj..kpjqkD.li.pjqlD..ikqkqlDj.i.pipjqkql.

This definition is the same as that given by [15,16]. Note that izMi(1)=1. Then, we have

iDjlik=E[(ixMi(1))xFj(1)xMk(2)xFl(2)]=E[i(zMi(1)pi)xFj(1)xMk(2)xFl(2)=0

In general, Djlik is summed to zero over any allele involved, so are Dj.ik and other disequilibrium measurements.

With Hardy-Weinberg and genotypic equilibria but linkage disequilibrium, model (7) leads to the following expression for the overall mean

E(G)=μ+i,k(αiβk)D..ik+j,l(αjβl)Djl..+i,j,k,l(δjiγlk)DikDjl

where μ is the mean genotypic value under linkage equilibrium, and Δμ=i,k(αiβk)D..ik+j,l(αjβl)Djl..+i,j,k,l(δjiγlk)D..ikDjl.. represents the departure from μ due to linkage disequilibrium and epistasis. If there is no epistasis, linkage disequilibrium does not affect the mean genotypic value. Similar results were given by [17]. Note that for marginal means of the genotypic values, we have

G....=i,j,k,lP..ikPjl..Gjlik, G..i.=1pij,k,lP..ikPjl..Gjlik,G..ik=j,lPjl..Gjlik, Gj.i.=1pipjk,lPjl..P..ikGjlik,Gj.ik=1pjlPjl..Gjlik, ...

and so on.

Then the question is what the genetic effects are in a disequilibrium population. Do Hardy-Weinberg and linkage disequilibria change the definition and values of genetic effects? The short answer to this question is "no" in a fully characterized model, but "yes" in a model that ignores some QTL or genetic effects. This is proved and discussed in [10]. With Hardy-Weinberg and linkage disequilibria, the genetic effects no longer correspond to the deviations from marginal means of genotypic values in a disequilibrium population. In a multiple regression model (7), the genetic effects are partial regression coefficients. These partial regression coefficients correspond to the simple regression coefficients, or deviations from marginal means of genotypic values, only in an equilibrium population. In a disequilibrium population, a direct analysis on the partial regression coefficients can be very complex (see the appendix of [10] for a relatively simple example). However, in a full model which includes all relevant loci and genetic effects, the model parameters depend only on how the regressors, i.e. x variables in (7), are defined and are independent of correlations between x variables, i.e. Hardy-Weinberg and linkage disequilibria. So, the genetic effects are still the same as those defined in the equilibrium population, although the population mean and marginal means of genotypic values are changed in a disequilibrium population.

Hardy-Weinberg and linkage disequilibria introduce correlation between x variables, thus covariances between different genetic effect components. Define

A1=i=1n1αixMi(1)+j=1n1αjxFj(1)D1=i,jδjixMi(1)xFj(1)A2=k=1n2βkxMk(2)+l=1n2βlxFl(2)D2=k,lγlkxMk(2)xFl(2)A1A2=i,k(αiβk)xMi(1)xMk(2)+i,l(αiβl)xMi(1)xFl(2)+j,k(αjβk)xFj(1)xMk(2)+j,l(αjβl)xFj(1)xFl(2)A1D2=i,k,l(αiγlk)xMi(1)xMk(2)xFl(2)+j,k,l(αjγlk)xFj(1)xMk(2)xFl(2)A2D1=i,j,k(δjiβk)xMi(1)xFj(1)xMk(2)+i,j,l(δjiβl)xMi(1)xFj(1)xFl(2)D1D2=i,j,k,l(δjiγlk)xMi(1)xFj(1)xMk(2)xFl(2)

Then we can write

G = μ + A1 + A2 + D1 + D2 + A1A2 + A1D2 + A2D1 + D1D2

In a disequilibrium population, the partition of the genotypic variance becomes

VG=i=18j=18Vij=1TV1

where

V = (Vij)8 × 8

It is a symmetric matrix. In Appendix C, we give the detailed result for each component of the matrix with linkage disequilibrium, but assuming Hardy-Weinberg equilibrium.

For the rest of paper, when we discuss disequilibrium, we mainly discuss linkage disequilibrium and assume Hardy-Weinberg and genotypic equilibria which can be achieved by random mating in one generation. Hardy-Weinberg disequilibrium can be taken into account which will make results more complex and is thus omitted.

Reduced models

In many genetic applications, experimental population has some regular genetic structure by design. In these cases, the genetic model can be further simplified to reflect the experimental design structure. Also sometimes we may want to simplify the genetic model by imposing certain constrains or assumptions, such as the number of alleles, to increase the feasibility of analysis. In this section, we give a few reduced genetic models that are relevant to many genetic applications.

1. Backcross population or recombinant inbred population (haploid model)

Backcross population or recombinant inbred population is a common experimental design for QTL mapping study. By crossing two inbred lines, we can create a F1 population. If we randomly backcross F1 to one of the inbred lines, we have a backcross population. Let us assume that the cross is AA (paternal) × Aa (maternal). In a random-mating backcross population, there are only two possible genotypes at each segregating locus ArAr or Arar, for r = 1, 2, ..., m, where m is the number of QTL. Since for the paternal gametes,

zM1(r)={1,for Ar allele from paternal gamete0,otherwise =1,

and

zM2(r)={1,for ar allele from paternal gamete0,otherwise =0,

thus xM1(r)=zM1(r)1=0 and xM2(r)=zM2(r)=0 for r = 1, 2, ..., m. For maternal gametes however,

xF1(r)={1/2, for Ar from maternal gamete1/2, otherwise=xF2(r), for r=1,2,,m.

Thus the model becomes

G=μ+r=1marxF1(r)+r<sbrs(xF1(r)xF1(s))+r<s<tcrst(xF1(r)xF1(s)xF1(t))+     (8)

where ar=α1(r)α2(r) is the substitution effect between homozygote genotype ArAr and heterozygote genotype Arar,brs=(α1(r)α1(s))(α1(r)α2(s))(α2(r)α1(s))+(α2(r)α2(s)) is the interaction effect between loci r and s,crst=(α1(r)α1(s)α1(t))(α1(r)α1(s)α2(t))(α1(r)α2(s)α1(t))+(α1(r)α2(s)α2(t))(α2(r)α1(s)α1(t))+(α2(r)α1(s)α2(t))+(α2(r)α2(s)α1(t))(α2(r)α2(s)α2(t)), ..., and so on. Taking constraint conditions into account, we have α1 = -α2, β1 = -β2, and so on. Then, ar = 2α1(r), brs = 4(α1(r)α1(s)), and crst = 8(α1(r)α1(s)α1(t)), and so on. With linkage equilibrium, the genetic effects as the partial regression coefficients of the model correspond to the simple regression coefficients. For example, for the substitution effect of locus r, ar, it is the covariance between genotypic value G and substitution effect design variable xF1(r) divided by the variance of xF1(r). So in general, we have

ar=E[(Gμ)xF1(r)]/E(xF1(r)2)=E[G(zF1(r)1/2)]/(1/4)=2[E(G|zF1(r)=1)E(G)]brs=E[(Gμ)xF1(r)xF1(s)]/[E(xF1(r)2)E(xF1(s)2)]=4[E(G|zF1(r)=zF1(s)=1)E(G|zF1(r)=1)E(G|zF1(s)=1)+E(G)]crst=E[(Gμ)xF1(r)xF1(s)xF1(t)]/[E(xF1(r)2)E(xF1(s)2)E(xF1(t)2)]=8[E(G|zF1(r)=zF1(s)=zF1(t)=1)E(G|zF1(r)=zF1(s)=1)E(G|zF1(r)=zF1(t)=1)E(G|zF1(s)=zF1(t)=1)+E(G|zF1(r)=1)+E(G|zF1(s)=1)+E(G|zF1(t)=1)E(G)]

The orthogonal partition of the genotypic variance in an equilibrium population is

VG=14r=1lar2+142r<sbrs2+143r<s<tcrst2+     (9)

As noted above, linkage disequilibrium does not change the values of genetic effects in a full model. The model parameters are still the same as those defined in the equilibrium population. However, in this case there is a simple relationship between the substitution effects at multiple loci and marginal means of genotypic values in a disequilibrium population [18]. This is noted here. Let Prs=P{zF1(r)=zF1(s)=1}, and the digenic linkage disequilibrium be defined as

Drs=Cov(zF1(r),zF1(s))=E(xF1(r)xF1(s))

Ignoring trigenic and higher order linkage disequilibria, we have

E[(Gμ)xF1(r)]=14ar+r'rDrr'ar'

E[(Gμ)xF1(r)xF1(s)]=142brs

Therefore, the digenic interaction effects can be expressed as

brs=42[PrsE(G|zF1(r)=zF1(s)=1)Drsμ]4[E(G|zF1(r)=1)+E(G|zF1(s)=1)E(G)]

Then the substitution effects can be expressed as a function of marginal means in the disequilibrium population as

(a1a2al)=(I+4D)1(2q)

where I is a m × m identity matrix, D = (Dij)m × m with all diagonal elements being zeros;

q = (q1, q2, ..., qm,)T, with qi = E(G|zF1(i) = 1) - E(G), for i = 1, 2, ..., m.

The partition of genetic variance with linkage disequilibrium is complex. Here we give details of the partition of genotypic variance for the following model

G=μ+r=1marxF1(r)+r<sbrs(xF1(r)xF1(s))     (10)

Let xr = xF1(r) and xs = xF1(s) to simplify the notation here. The genotypic variance is

VG=V(rarxr)+2Cov(rarxr,r<sbrsxrxs)+V(r<sbrsxrxs)=rar2pr(1pr)+2r<sarasDrs+2r<s[arbrs(12pr)Drs+asbrs(12ps)Drs]+2r<s<t(arbst+asbrt+atbrs)Drst+r<sbrs2[(12pr)(12ps)Drs+pr(1pr)ps(1ps)Drs2]+2r<s<t{brsbrt[(12pr)Drstpr(1pr)DstDrsDrt]+brsbst[(12ps)Drst+ps(1ps)DrtDrsDst]+brtbst[(12pt)Drst+pt(1pt)DrsDrtDst]}+2r<s<t<u[brtbsu(DrstuDrtDsu)+brubst(DrstuDruDst)+brsbtu(DrstuDrsDtu)]     (11)

where

Drst = E(xrxsxt) and Drstu = E(xrxsxtxu)

are three locus and four locus linkage disequilibria. This is a general partition of genetic variance for a haploid model.

For the backcross population, it can be shown that Drst = 0 (see Appendix D for both backcross and F2 populations) and Drstu = DrsDtu for loci r, s, t and u in this order under the assumption of no crossing-over interference. Also with this assumption, Drt = 4DrsDst and Drs = (1 - 2λrs)/4, where λrs is the recombination frequency between loci r and s. Since, pr = ps = 1/2, the variance becomes

VG=14rar2+2r<sarasDrs+116r<sbrs2(116Drs2)+12r<s<t[brsbrt(116Drs2)Dst+brtbst(116Dst2)Drs]+2r<s<t<u(brtbsu+brubst)(116Dst2)DrsDtu     (12)

In this partition of variance, the first summation term is the genetic variance due to the substitution effect of each QTL, the second summation term is the covariance between substitution effects of QTL pairs due to linkage disequilibrium, the third summation term is the genetic variance due to epistatic effects of QTL, and the fourth and fifth summation terms are the covariance between different epistatic effects of QTL due to linkage disequilibrium. There is no covariance between the main substitution effects and epistatic effects (see also [19]).

For a backcross population, the genetic interpretation of the substitution effect ar depends on which parental line is backcrossed. In one backcross AA × Aa, the substitution effect is traditionally defined as the difference between the additive effect and dominance effects, and in the other backcross Aa × aa, it is the sum of the additive and dominance effects. Only with both backcrosses, can one estimate both additive and dominance effects separately (for example [20]).

The same model also applies to a recombinant inbred population which is another very popular experimental design for QTL mapping study. For a recombinant inbred population, the substitution effects of QTL are the additive effects and the epistatic effects are the additive × additive interaction effects. Statistical methods to map QTL and to estimate various components of the genetic variance due to QTL including epistasis has been developed through the maximum likelihood approach [19,21]. In a few cases where the method was applied, we estimated, for the first time, how the quantitative genetic variance was partitioned into various components in designed experimental populations. For example, Weber et al. [22] reported the result of QTL mapping for wing shape on the third chromosome of Drosophila melanogaster from a cross of divergent selection lines. From 519 recombinant inbred lines, 11 QTL were mapped on the third chromosome. Nine QTL pairs showed significant epistatic effects. The total genetic variance amounts to 95.5% of the phenotypic variance in the recombinant inbred lines with phenotypes measured and averaged over 50 male flies for each recombinant inbred line. The partition of the genetic variance is as follows (see Table 6 and 7 of [22]): 27.4% due to the variances of additive effects (equivalent to the first summation term of (12)); 67.3% due to the covariances between additive effects (the second summation term); 7.2% due to the variances of epistatic effects (the third summation term); and -6.0% due to the covariances between epistatic effects (the fourth and fifth summation terms). The covariances between additive and epistatic effects, expected to be 0, account for -0.4% due to sampling. Similar kind of partition of the genetic variance is also observed in a group of 701 second chromosome recombinant inbred lines from a cross of the same divergent selection lines (see Table 4 and 5 of [23]). See also [20] for another example.

2. F2 population

F2 is created from a cross between pairs of F1 individuals. It is also a very popular experimental design for QTL mapping study. The advantage of this design is that both additive and dominance effects of a QTL can be estimated as well as various epistatic effects. The design also has more statistical power for QTL detection as compared to a backcross population. In a random-mating F2 population, there are only two alleles at each segregating locus and allelic frequencies are expected to be one half if there is no segregation distortion.

Let us consider only two loci first. Let A and a denote the two alleles at locus 1, and B and b at locus 2. In this case, xM1(1)=xM2(1) and xF1(1)=xF2(1). Assuming Gjlij=Gikjl=Gjkil=Giljk, it also holds that α1 = α1 = -α2 = -α2, δ11=δ22=δ12, and so on. The additive term for locus 1 then becomes

A1=α1(xM1(1)xM2(1))+α1(xF1(1)xF2(1))=2α1 w1

with

w1=xM1(1)+xF1(1)={1, for AA at locus 10, for Aa at locus 11, for aa at locus 1     (13)

and the dominance term is

D1=2(δ11)(xM1(1)xF1(1)+xM1(1)xF1(1))=(2)(δ11)v1

with

v1=(2)xM1(1)xF1(1)={1/2, for AA at locus 11/2, for Aa at locus 11/2, for aa at locus 1     (14)

Note that the v variable in this section for F2 differ, by a factor -2, from the v variable in the next section for a general two-allele model to conform to the usual definition for the F2 model. Similarly, for locus 2

A2 = 2β1w2 and D2 = (-2)(γ12)v2

with

w2={1, for BB at locus 20, for Bb at locus 21, for bb at locus 2

and

v2={1/2, for BB at locus 21/2, for Bb at locus 21/2, for bb at locus 2     (15)

The model can then be written as

G=μ+a1w1+d1v1+a2w2+d2v2+(aa)12(w1w2)+(ad)12(w1v2)+(da)12(v1w2)+(dd)12(v1v2)     (16)

where the parameters are related as a1 = 2α1, a2 = 2β2, d1 = - 2δ11, d2 = -2γ11, (aa)12 = 4(α1β1), (ad)12 = 8(α1γ11), (da)12 = 8(δ11β1), (dd)12 = 16(δ11γ11). With random mating and linkage equilibrium, we have

a1=E[Gμ)w1]/E(w12)=2(G1...G....)d1=E[(Gμ)v1]/E(v21)=(2)(G1.1.2G1...+G....)a2=2(G.1..G....)d2=(2)(G.1.12G.1..+G....)(aa)12=E[(Gμ)w1w2]/E(w12w22)=4(G..11G1...G.1..+G....(ad)12=E[(Gμ)w1v2]/E(w12v22)=(4)(G11.12G11..G.1.1+G1...+2G.1..G....)(da)12=E[(Gμ)v1w2]/E(v12w22)=(4)(G111.2G11..G1.1.+G.1..+2G1...G....)(dd)12=E[(Gμ)v1v2]/E(v12v22)=4(G11112G111.2G11.1+G1.1.+G.1.1+4G11..2G1...2G.1..+G....)

The orthogonal partition of the genotypic variance is

VG=12a12+14d12+12a22+14d22+14(aa)122+18(ad)122+18(da)122+116(dd)122.     (17)

Recently, Kao and Zeng [18] have examined many genetic and statistical issues of the above F2 model and the effects of linkage disequilibrium. As we have shown here, the F2 model is a special case of Cockerham model with two alleles at each locus and all allelic frequencies being 1/2.

Now we give the partition of genetic variance for m loci with epistasis and linkage disequilibrium in the F2 population. Generalizing model (16) to m loci and ignoring the trigenic and higher order epistasis, we have the following model

G=μ+r=1marwr+r=1mdrvr+r<s(aa)rs(wrws)+rs(ad)rs(wrvs)+r<s(dd)rs(vrvs)=μ+A+D+AA+Ad+DD     (18)

The partition of genetic variance for this model under the assumption of Hardy-Weinberg equilibrium is

VG=VA+VD+VAA+VAD+VDD+2Cov(A,D)+2Cov(A,AA)+2Cov(A,AD)+2Cov(A,DD)+2Cov(D,AA)+2Cov(D,AD)+2Cov(D,DD)+2Cov(AA,AD)+2Cov(AA,DD)+2Cov(AD,DD).     (19)

The detail of each component is presented in Appendix D.

The F2 model is a special case of the general two-allele model with pr = 1/2. Note the difference on the v variable used for the F2 model and for the general two-allele model below. This partition of genetic variance can provide a basis for the interpretation of genetic variance estimation by multiple interval mapping in a F2 population [19,21].

3. A general two-allele model

Here, we provide details of a general two-allele model for multiple loci. This model is probably useful for studying genetic architecture of a quantitative trait in natural populations. Let the two alleles at locus r be Ar and ar for r = 1, 2, ..., m with m the number of QTL. Assume that the frequencies and genetic effects of alleles are the same for both paternal and maternal gametes. Let pr denote the frequency of allele Ar at locus r. Note that in this case zM1(r)=1zM2(r), r = 1, 2, ..., m. Also xM1(r)=zM1(r)E[zM1(r)]=(1zM2(r))E(1zM2(r))=xM2(r). Similarly, xF2(r)=xF1(r) Ignoring higher order epistasis involving at least three loci, we can define a two-allele model as

G=μ+r=1marwr+r=1mdrvr+r<s(aa)rs(wrws)+rs(ad)rs(wrvs)+r<s(dd)rs(vrvs)     (20)

where

wr=xM1(r)+xF1(r)={(1pr)for ArAr at locus r12prfor Arar at locus r2prfor arar at locus r     (21)

vr=xM1(x)xF1(x)={(1pr)2for ArAr at locus rpr(1pr)for Arar at locus rpr2for arar at locus r     (22)

for r = 1, 2, ..., m. The coefficients are associated with the original parameters in Cockerham model as follows.

ar=α1(r)α2(r)dr=δ11(r)δ21(r)δ12(r)+δ22(r)(aa)rs=(α1(r)α1(s))(α1(r)α2(s))(α2(r)α1(s))+(α2α2(s))(ad)rs=(α1(r)δ11(s))(α1(r)δ21(s))(α1(r)δ12(s))+(α1(r)δ22(s))(α2(r)δ11(s))+(α2(r)δ21(s))+(α2(r)δ12(s))(α2(r)δ22(s))(dd)rs=(δ11(r)δ11(s))(δ11(r)δ21(s))(δ11(r)δ12(s))+(δ11(r)δ22(s))(δ21(r)δ11(s))+(δ21(r)δ21(s))+(δ21(r)δ12(s))(δ21(r)δ22(s))(δ12(r)δ11(s))+(δ12(r)δ21(s))+(δ12(r)δ12(s))(δ12(r)δ22(s))+(δ22(r)δ11(s))(δ22(r)δ21(s))(δ22(r)δ12(s))+(δ22(r)δ22(s))

The constraint conditions further lead to

ar=α1(r)(pr)(1pr)α1(r)=1(1pr)α1(r)dr=1(1pr)2δ11(r)(aa)rs=1(1pr)(1ps)(α1(r)α1(s))(ad)rs=1(1pr)(1ps)2(α1(r)δ11(s))(dd)rs=1(1pr)2(1ps)2(δ11(r)δ11(s))

With Hardy-Weinberg, linkage and genotypic equilibria, the partial regression coefficients in the above model correspond to the simple regression coefficients

ar=1(1pr)[E(G|zM1(r)=1)E(G)]dr=1(1pr)2[E(G|zM1(r)=zF1(r)=1)2E(G|zM1(r)=1)+E(G)](aa)rs=1(1pr)(1ps)[E(G|zM1(r)=zM1(s)=1)E(G|zM1(r)=1)E(G|zM1(s)=1)+E(G)](ad)rs=1(1pr)(1ps)2[E(G|zM1(r)=zM1(s)=zF1(s)=1)2E(G|zM1(r)=zM1(s)=1)E(G|zM1(s)=zF1(s)=1)+E(G|zM1(r)=1)+2E(G|zM1(s)=1)E(G)](dd)rs=1(1pr)2(1ps)2[E(G|zM1(r)=zF1(r)=zM1(s)=zF1(s)=1)2E(G|zM1(r)=zF1(r)=zM1(s)=1)2E(G|zM1(r)=zM1(s)=zF1(s)=1)E(G|zM1(r)=zF1(r)=1)+E(G|zM1(s)=zF1(r)=1)+4E(G|zM1(r)=zF1(s)=1)2E(G|zM1(r)=1)2E(G|zM1(s)=1)+E(G)]

Note that in this case the genetic effects in the original model are

α1(r)=E(G|zM1(r)=1)E(G)δ11(r)=E(G|zM1(r)=zF1(r)=1)2E(G|zM1(r)=1)+E(G)(α1(r)α1(s))=E(G|zM1(r)=zM1(s)=1)E(G|zM1(r)=1)E(G|zM1(s)=1)+E(G)(α1(r)δ11(s))=E(G|zM1(r)=zM1(s)=zF1(s)=1)2E(G|zM1(r)=zM1(s)=1)E(G|zM1(s)=zF1(s)=1)+E(G|zM1(r)=1)+2E(G|zM1(s)=1)E(G)(δ11(r)δ11(s))=E(G|zM1(r)=zF1(r)=zM1(s)=zF1(s)=1)2E(G|zM1(r)=zF1(r)=zM1(s)=1)2E(G|zM1(r)=zM1(s)=zF1(s)=1)+E(G|zM1(r)=zF1(r)=1]+E(G|zM1(s)=zF1(s)=1)+4E(G|zM1(r)=zF1(s)=1)2E(G|zM1(r)=1)2E(G|zM1(s)=1)+E(G)

They are the same as the least squares definition.

Yet another form of this result is shown in Table 1 of [10]. Zeng et al. [10] also show that linkage disequilibrium does not change the values of genetic effects in a full model. This means that the partial regression coefficients in a disequilibrium population equal to the simple regression coefficients in a corresponding equilibrium population with the same allelic frequency configuration.

The partition of genotypic variance in an equilibrium population is

VG=2r=1mpr(1pr)ar2+r=1mpr2(1pr)2dr2+4r<sprps(1pr)(1ps)(aa)rs2+2rspr(1pr)ps2(1ps)2(ad)rs2+r<spr2ps2(1pr)2(1ps)2(dd)rs2     (23)

or

VG=2pr(1pr)r=1m(α1(r))2+pr2(1pr)2r=1m(δ11(r))2+4prps(1pr)(1ps)r<s(α1(r)α1(s))2+2prps2(1pr)(1ps)2rs(α1(r)δ11(s))2+pr2ps2(1pr)2(1ps)2r<s(δ11(r)δ11(s))2     (24)

The partition of the genetic variance with epistasis and linkage disequilibrium is complex. We give the result with trigenic and quadrigenic linkage disequilibria included as well. The partition of variance has a similar form as (19). The detail of each component is presented in Appendix E.

Discussion

In this paper we explore various properties of the standard quantitative genetic model with multiple interacting loci in linkage equilibrium and disequilibrium. Starting from the traditional least squares model, we represent it in the setting of multiple regression with standardized allelic indicator variables and their products as the independent variables and the trait value as the dependent variable. Then the partial regression coefficients associated with these indicator variables define the additive, dominance and epistatic effects for QTL. This is the original definition of QTL effects introduced by Fisher [6] and extended to epistasis by Cockerham [7]. We examine the properties and meaning of these QTL effects in an equilibrium population and also in a disequilibrium population. We show details of the partition of genetic variance for both equilibrium and disequilibrium populations in terms of QTL effects, allelic frequencies and disequilibrium measures. Moreover, we relate this general model to several reduced models used for QTL mapping analysis in cross populations from inbred lines, such as F2, backcross and recombinant inbred lines. The detailed partition of genetic variance in these populations can provide a basis for the interpretation of genetic variance component estimates from multiple interval mapping [21].

The purpose of modeling QTL is to provide a meaningful and convenient framework and basis to infer and interpret relative significance of each QTL and intricate inter-relationship among QTL on a set of quantitative traits in an experimental or natural population for genetic study. The linear model provides a framework to study the effects of QTL on the mean and variance of the distribution of a trait or multiple traits in a population. With the assumption of a normal distribution for both genotypic and phenotypic values of a quantitative trait or multiple traits, this analysis on the first and second order statistics is sufficient to characterize the relationship between QTL and trait (s). Otherwise, it is an approximation on the relationship. In this model, the model parameters are partitioned into two parts: one is the effects of QTL (additive, dominance and epistatic effects), and the other is frequencies and correlations (Hardy-Weinberg and linkage disequilibria) of QTL alleles. Together they characterize the genetic architecture of quantitative traits in a population.

This linear model also provides a framework for statistical inference of genetic model parameters. If QTL genotypes are known and directly observed, a regression analysis of trait phenotype on QTL genotypes would provide a direct estimation of the genetic model parameters. However, if QTL genotypes are unknown and are only indirectly observed through molecular markers, the statistical inference of QTL and model parameters becomes more complicated. Statistically, we can regard QTL genotypes as missing data with trait phenotypes and marker genotypes as observed data and use a mixture model through the maximum likelihood analysis to infer the conditional distribution of missing data and through that to infer QTL parameters which also include the number and genomic position of QTL [19,24,25]. The likely positions of QTL are searched in the whole genome if data permit and the number of significant QTL positions can be estimated through some model selection procedure.

On modeling QTL, the consistence of model parameters in a multiple-locus setting is an important consideration. It is important for a model to be multiple-locus consistent, and the relationship within and between loci can be clearly and readily analyzed, estimated and interpreted. Here the consistence means that the effect of a QTL is consistently defined in a reference equilibrium population for one, two or multiple loci. In statistics, this is the property of orthogonality. This property is particularly important for the study of epistasis. With that the additive, dominance and epistatic effects can be independently and consistently estimated for one, two, three or multiple loci in the reference population where the model is defined and interpreted. Thus, if the number of QTL is incorrectly identified which seems to be always the case in practice, the parameter values for those identified QTL can still be consistently estimated. However, the situation would certainly be different and complicated if the population is not at equilibrium, for example for QTL in linkage disequilibrium. Linkage disequilibrium would complicate the partition of genetic variance, and could certainly bias the estimation of parameter values for those identified QTL if the QTL model (number and genomic position of QTL) is miss-identified.

In this paper, we study extensively the composition and property of the genetic model parameters, such as genetic effects and partition of genetic variance, when both epistasis and linkage disequilibrium are considered. This would help us to understand the relationship of various genetic quantities, such as allelic frequencies and linkage disequilibrium, on the definition of genetic effects. It would also help us to understand and properly interpret estimates of the genetic effects and variance components in a QTL mapping experiment. It is important to emphasize that modeling QTL is inherently population based as it defines the variation of QTL in reference to a population, either a study population, cross population or natural population. The very basic concept of additive effect of a QTL is a population concept and is population dependent. It depends on the genotypes at other loci and depends on the genetic structure of the population (allelic frequencies, Hardy-Weinberg and linkage disequilibria).

We also clarify the connection between the general genetic model and some reduced models. By restricting the number of alleles at each locus to two and setting allelic frequencies to half, the general genetic model is reduced to the F2 model. This simplification reduces the partition of genetic variance enormously.

Another property for this F2 population is that, if there is no crossing-over interference, the three-locus linkage disequilibrium is expected to be zero regardlessly whether the loci are linked. Also the four-locus disequilibrium is reduced to the product of the two-locus disequilibria for the two non-adjacent locus pairs. If there is crossing-over interference, the three-locus linkage disequilibrium would be a good measure of the interference. As many QTL mapping experiments are performed in a F2 population, this reduced model is very relevant to QTL mapping analysis for the interpretation of genetic architecture in a F2 population. Another reduced model is the backcross model which is essentially a haploid model.

We give many details for a general two-allele model with epistasis and linkage disequilibrium. Research on QTL mapping analysis has been shifted in recent years from inbred line crosses to natural populations. With the availability of very dense SNP markers, it is now possible to use SNP for fine mapping of QTL in a natural population. Currently most QTL fine mapping studies are concentrated on candidate genes. It will be increasingly possible to have genome-wide SNP data for a sample of individuals from a natural population. The general two-allele model can be used as a framework to interpret and estimate the genome-wide genetic architecture for a quantitative trait in a natural population. The model can be extended to multiple alleles to take haplotypes into account if needed.

Authors' contributions

TW conducted the initial derivation of models and partition of variance and drafted the initial manuscript. ZBZ extended the derivation of models and partition of variance, revised and finalized the manuscript. Both authors have read and approved the final manuscript. Comments and requests should be addressed to ZBZ or TW.

Appendix

A. Cockerham least squares estimates

In this appendix, we show that the regression coefficients (genetic effects) in model (7) are Cockerham least squares estimates under Hardy-Weinberg, linkage and genotypic equilibria. First, note that at each locus only one allele is present on a gamete. That is if an individual inherits an allele Ai from a parental gamete, zMi(1) = 1 and the other zMj(1) = 0 for j i Therefore, when i j, we have E(zMi(1)zMj(1)) = 0 or E(xMi(1)xMj(1))=E(zMi(1)zMj(1))E(zMi(1))E(zMj(1))=pipj. Using these relationships, we can show the following for model (7).

• Additive effects: For i = 1, 2, ..., n1, we can show

E[(Gμ)xMi(1)]=E[(i'αi'xMi'(1))xMi(1)]=αiE(xMi(1)2)+i'iαi'E(xMi'(1)xMi(1))=αipi(1pi)+i'iαi'(pi'pi)=αipi+(pi)i'αi'pi'=αipi,

On the other hand,

E[(Gμ)xMi(1)]=E(G xMi(1))=E[G(zMi(1)pi)]=E(GzMi(1))piE(G)=E[E(GzMi(1)|zMi(1))]piG....=piE(G|zMi(1)=1)piG....=pi(G..i.G....).

Therefore, αi=G..i.G.... for i = 1, 2, ..., n1. Similarly, we can show that αj=Gj...G.... for j = 1, 2, ..., n1, and βk=G...kG...., βl=G.l..G.... for k, l = 1, 2, ..., n2.

• Dominance effects: For locus 1, we have

E[(Gμ)xMi(1)xFj(1)]=E[(i',j'δj'i'xMi'(1)xFj'(1))xMi(1)xFj(1)]=j'δj'iE(xMi(1)2)E(xFj(1)xFj'(1))+i'ij'δj'i'E(xMi(1)xMi'(1))E(xFj(1)xFj'(1))=pi(1pi)j'δj'iE(xFj(1)xFj'(1))+i'i(pipi')j'δj'i'E(xFj(1)xFj'(1))=pij'δj'iE(xFj(1)xFj'(1))i'pipi'j'δj'iE(xFj(1)xFj'(1))=pi(pjδji+j'δj'ipj')pij'E(xFj(1)xFj'(1))i'pi'δj'i'=pipjδji for i,j=1,2,,n1.

On the other hand,

E[(Gμ)xMi(1)xFj(1)]=E[G(zMi(1)pi)(zFj(1)pj)]=E(GzMi(1)zFj(1)piE(GzFj(1))pjE(GzMi(1))+pipjE(G)=E[E(GzMi(1)zFj(1)|zMi(1),zFj(1))]piE[E(GzFj(1)|zFj(1)])pjE[E(GzMi(1)|zMi(1))]+pipjG....=pipj(Gj.i.G..i.Gj...+G....)

Therefore, δji=Gj.i.G..i.Gj...+G.... for i, j = 1, 2, ..., n1. Similar results can be derived for other dominance terms at locus 2.

• Additive × additive effects: Note that

E[(Gμ)xMi(1)xMk(2)]=i,k(αiβk)E(xMi(1)xMi(1))E(xMk(2)xMk(2))=k'(αiβk)E(xMi(1)2)E(xMk(2)xMk(2))+iik(αiβk)(pipi)E(xMk(2)xMk(2))=pik(αiβk)E(xMk(2)xMk(2))piik(αiβk)piE(xMk(2)xMk(2))=piqk(αiβk)

and

E[(Gμ)xMi(1)xMk(2)]=E(GxMi(1)xMk(2))=E[G(zMi(1)pi)(zMk(2)qk)]=piqk(G..ikG..i.G...k+G....)

We have (αiβk)=G..ikG..i.G...k+G.... for i = 1, 2, ..., n1 and k = 1, 2, ..., n2. Similar results can be derived for other additive by additive terms.

• Additive × dominance effects: Note that

E[(Gμ)xMi(1)xMk(2)xFl(2)]=E[xMi(1)xMk(2)xFl(2)i,k,l(αiγlk)xMi(1)xMk(2)xFl(2)]=k,l(αiγlk)E(xMi(1)2)E(xMk(2)xMk(2))E(xFl(2)xFl(2))=pik,l(αiγlk)E(xMk(2)xMk(2))E(xFl(2)xFl(2))=piqkql(αiγlk)

and

E[(Gμ)xMi(1)xMk(2)xFl(2)]=E[G(zMi(1)pi)(zMk(2)qk)(zFl(2)ql)]=piqkql(G.likG..ikG.li.G.l.k+G..i.+G...k+G.l..G....)

For i = 1, 2, ..., n1 and k, l = 1, 2, ..., n2, we have

(αiγlk)=G.likG..ikG.li.G.l.k+G..i.+G...k+G.l..G....

Similar results can be derived for dominance by additive terms.

• Dominance × dominance effects: Note that

E[(Gμ)xMi(1)xFj(1)xMk(2)xFl(2)]=E[xMi(1)xFj(1)xMk(2)xFl(2)i,j,k,l(δjiγlk)xMi(1)xFj(1)xMk(2)xFl(2)]=i,jE(xMi(1)xMi(1))E(xFj(1)xFj(1))k,l(δjiγlk)E(xMk(2)xMk(2))E(xFl(2)xFl(2))=i,jE(xMi(1)xMi(1))E(xFj(1)xFj(1))(δjiγlk)qkql=(δjiγlk)pipjqkql

On the other hand

E[(Gμ)xMi(1)xFj(1)xMk(2)xFl(2)]=E[G(zMi(1)pi)(xFj(1)pj)(zMk(2)qk)(zFl(2)ql)]=pipjqkql(GjlikGj.ikG.likGjli.Gjl.k+G..ik+Gjl..+Gj.i.+G.l.k+Gj..k+G.li.G..i.G...kGj...G.l..+G....)

For i, j = 1, 2, ..., n1 and k, l = 1, 2, ..., n2, we have

(δjiγlk)=GjlikGj.ikG.likGjli.Gjl.k+G..ik+Gjl..+Gj.i.+G.l.k+Gj..k+G.li.G..i.G...kGj...G.l..+G....

B. Partition of genotypic variance in linkage equilibrium

Here we show that the genotypic variance VG of model (7) has the orthogonal partition (4) under Hardy-Weinberg, linkage and genotypic equilibria. First, note that the index variables xMi(1), xFj(1), xMk(2), xFl(2) have expectation zero. Second, the assumption of Hardy-Weinberg, linkage and genotypic equilibria mean that all alleles in different gametes and loci are independent so that, for example,

Cov(xMi(r),xFj(r))=E(xMi(r)xFj(r))=E(xMi(r))E(xFj(r))=0

Thus the additive and dominance effects within a locus are orthogonal to each other because

Cov(xMk(r),xMi(r),xFj(r))=E(xMk(r)xMi(r)xFj(r))=E(xMk(r))E(xMi(r))E(xFj(r))=0

for any 1 ≤ i, j, k n1 and locus r = 1 or 2. Similarly, the epistatic effects between loci are orthogonal to additive and dominance effects and also to other epistatic effects. Therefore, the total genotypic variance VG can be partitioned as

VG=VA1+VA2+VD1+VD2+VA1A2+VA1D2+VD1A2+VD1D2

with each component analyzed below.

• The additive variance: For locus 1,

VA1=Var(i=1n1αixMi(1)+j=1n1αjxFj(1))=Var(i=1n1αixMi(1))+Var(j=1n1αjxFj(1))=E[(i=1n1αixMi(1))2]+E[(j=1n1αjxFj(1))2]=E[(i=1n1αizMi(1))i=1n1αipi)2]+E[(j=1n1αjxFj(1)j=1n1αjpj)2]=E[(i=1n1αizMi(1))2]+E[(j=1n1αjzFj(1))2]=i=1n1(αi)2E[(zMi(1))2]+j=1n1(αj)2E[(zFj(1))2]=i=1n1(αi)2pi+j=1n1(αj)2pj

as i=1n1αipi=0 by the constrain condition (2). Similarly, for locus 2, we have VA2=k=1n2(βk)2qk+j=1n2(βl)2ql.

• The dominance variance: For locus 1,

VD1=Var(i,jδjixMi(1)xFj(1))=E[(i,jδji(zMi(1))pi)(zFj(1)pj))2]=E[(i,jδjizMi(1)zFj(1)i,jpjδjizMi(1)i,jpiδjizFj(1)+i,jpipjδji)2]=E[(i,jδjizMi(1)zFj(1))2]=i,j(δji)2E(zMi(1)2)E(zFj(1)2)=i,j(δji)2pipj

Similarly, for locus 2, we have VD2=k,l(γlk)2qkql.

• The additive × additive variance:

VA1A2=Var(i,k(αiβk)xMi(1)xMk(2))+Var(i,l(αiβl)xMi(1)xFl(2))+Var(j,k(αjβk)xFj(1)xMk(2))+Var(j,l(αjβl)xFj(1)xFl(2))=i,kpiqk(αiβk)2+j,lpjql(αjβl)2+i,lpiql(αiβl)2+j,kpjqk(αjβk)2

• The additive × dominance variance:

VA1D2=Var(i,k,l(αiγlk)xMi(1)xMk(2)xFl(2))+Var(j,k,l(αjγlk)xFj(1)xMk(2)xFl(2))=i,k,lpiqkql(αiγlk)2+j,k,lpjqkql(αjγlk)2

Similarly, the dominance × additive variance is VD1A2=i,j,kpipjqk(δjiβk)2+i,j,lpipjql(δjiβl)2.

• The dominance × dominance variance:

VD1D2=Var(i,j,k,l(δjiγlk)xMi(1)xFj(1)xMk(2)xFl(2))=E[(i,j,k,l(δjiγlk)zMi(1)zFj(1)zMk(2)zFl(2))2]=i,j,k,lpipjqkql(δjiγlk)2

C. Partition of genotypic variance in linkage disequilibrium

We present the partition of the genotypic variance based on model (7) under the assumption of Hardy-Weinberg equilibrium but linkage disequilibrium.

• The additive variance:

VA1=i=1n1pi(αi)2+j=1n1pj(αj)2, VA2=k=1n2qk(βk)2+j=1n2ql(βl)2

• The dominance variance:

VD1=i,j(δji)2pipj,VD2=k,l(γlk)2qkql

• The additive × additive variance:

VA1A2=i,k(piqk+D..ik)(αiβk)2[i,k(αiβk)D..ik]2+j,l(pjql+Djl..)(αjβl)2[j,l(αjβl)Djl..]2+i,lpiql(αiβl)2+j,kpjqk(αjβk)2+2i,j,k,l(αiβk)(αjβl)Djl..D..ik+2i,j,k,l(αiβl)(αjβk)Djl..D..ik+2(i,k(αiβk)D..ik)(j,l(αjβl)Djl..)

• The additive × dominance variance:

VA1D2=i,k,lql(piqk+D..ik)(αiγlk)2+j,k,lqk(pjql+Djl..)(αjγlk)2+2i,j,k,l(αiγlk)(αjγlk)Djl..D..ik

• The dominance × additive variance:

VD1A2=i,j,kpj(piqk+D..ik)(δjiβk)2+i,j,lpi(pjql+Djl..)(δjiβl)2+2i,j,k,l(δjiβk)(δjiβl)Djl..D..ik

• The dominance × dominance variance:

VD1D2=i,j,k,l(δjiγlk)2(D..ik+piqk)(Djl..+pjql)

• The covariances related to additive and dominance effects:

Cov(A1,A2)=i,k(αiβk)D..ik+j,l(αjβl)Djl..Cov(D1,D2)=i,j,k,l(δji)(γlk)Djl..D..ikCov(A1,D1)=Cov(A1,D2)=Cov(A2,D1)=Cov(A2,D2)=0

• The covariances related to additive × additive effects:

Cov(A1,A1A2)=i,k(αi)(αiβk)D..ik+j,l(αj)(αjβl)Djl..Cov(A2,A1A2)=i,k(βk)(αiβk)D..ik+j,l(βl)(αjβl)Djl..Cov(D1,A1A2)=i,j,kpj(δji)(αjβk)D..ik+i,j,lpi(δji)(αiβl)Djl..Cov(D2,A1A2)=i,k,lql(αiβl)(γlk)D..ik+j,k,lqk(αjβk)(γlk)Djl..

• The covariances related to additive × dominance and dominance × additive effects:

Cov(A1,A1D2)=i,j,k,l[(αi)(αjγlk)+(αj)(αiγlk)]Djl..D..ikCov(A2,A1D2)=i,k,lql(βl)(αiγlk)D..ik+j,k,lqk(βk)(αjγlk)Djl..Cov(A1,D1A2)=i,j,kpj(αj)(δjiβk)D..ik+i,j,lpi(αi)(δjiβl)Djl..Cov(A2,D1A2)=i,j,k,l[(βk)(δjiβl)+(βl)(δjiβk)]Djl..D..ikCov(D1,A1D2)=i,j,k,l(δji)[(αiγlk)+(αjγlk)]Djl..D..ikCov(D2,A1D2)=i,k,lql(γlk)(αiγlk)D..ik+j,k,lqk(γlk)(αjγlk)Djl..Cov(D1,D1A2)=i,j,kpj(δji)(δjiβk)D..ik+i,j,lpi(δji)(δjiβl)Djl..Cov(D2,D1A2)=i,j,k,l(γlk)[(δjiβk)+(δjiβl)]Djl..D..ikCov(A1A2,A1D2)=i,k,lql(αiβl)(αiγlk)D..ik+j,k,lqk(αjβk)(αjγlk)Djl..+i,j,k,l[(αiβk)(αjγlk)+(αiβl)(αjγlk)+(αjβk)(αiγlk)+(αjβl)(αiγlk)]Djl..D..ikCov(A1,A2,D1A2)=i,j,kpj(αjβk)(δjiβk)D..ik+i,j,lpi(αiβl)(δjiβl)Djl..+i,j,k,l[(αiβk)(δjiβl)+(αjβk)(δjiβl)+(αiβl)(δjiβk)+(αjβl)(δjiβk)]Djl..D..ikCov(A1D2,D1A2)=i,j,k,l[(αiγlk)(δjiβk)(D..ik+piqk)Djl..+(αiγlk)(δjiβl)Djl..D..ik+(αjγlk)(δjiβk)Djl..D..ik+(αjγlk)(δjiβl)(Djl..+pjql)D..ik]

• The covariances related to dominance × dominance effects:

Cov(A1,D1D2)=i,j,k,l(δjiγlk)(αi+αj)Djl..D..ikCov(A2,D1D2)=i,j,k,l(δjiγlk)(βk+βl)Djl..D..ikCov(D1,D1D2)=i,j,k,l(δjiγlk)(δji)Djl..D..ikCov(D2,D1D2)=i,j,k,l(δjiγlk)(γlk)Djl..D..ikCov(A1A2,D1D2)=(i,k(αiβk)D..ik+j,l(αjβl)Djl..)(i,j,k,l(δjiγlk)Djl..D..ik)+i,j,k,l(δjiγlk){[(αiβk)+(αiβl)+(αjβk)+(αjβl)]Djl..D..ik+(αiβk)piqkDjl..+(αjβl)pjqlD..ik}Cov(A1D2,D1D2)=i,j,k,l(δjiγlk)[(αiγlk)(D..ik+piqk)Djl..+(αjγlk)(Djl..+pjql)D..ik]Cov(D1A2,D1D2)=i,j,k,l(δjiγlk)[(δjiβk)(D..ik+piqk)Djl..+(δjiβl)(Djl..+pjql)D..ik]

D. Partition of genotypic variance in F2 population with linkage disequilibrium

Detail of each component of equation (19) for F2 population is presented here.

• The additive variance:

VA=12r=1mar2+2rsarasDrs

• The dominance variance:

VD=14r=1mdr2+4rsdrdsDrs2

• The additive × additive variance:

VAA=14r<s(aa)rs2+rss(aa)rs(aa)rsDss+12rsrs(aa)rs(aa)rs(Drrss+DrsDrs+DrrDssDrsDrs)

• The additive × dominance variance:

VAD=18rs(ad)rs2+12rs(ad)rs(ad)srDrs+2rss(ad)rs[(ad)rsDss2+(ad)ssDssDrs+(ad)srDrsDss+14(ad)ssDrs]+8rsrs(ad)rs(ad)rsDrsrsDss

• The dominance × dominance variance:

VDD=r<s(dd)rs2(11616Drs4)+rss'(dd)rs(dd)rs'(Dss'216Drs2Drs'2)+4rsr's'(dd)rs(dd)r's'(Drsr's'2Drs2Dr's'2)

• The covariances: Cov(A, D) = Cov(A, AA) = Cov(A, DD) = Cov(D, AD) = Cov(D, DD) = Cov(AA, AD) = Cov(AD, DD) = 0, and

Cov(A,AD)=rsarDrs[4(ad)rsDrs+(ad)sr]4rsr'ar'(ad)rsDrsDr'sCov(D,AA)=r<s(dr+ds)(aa)rsDrs4rsr'dr'(aa)rsDrr'Dr'sCov(AA,DD)=r<s(aa)rs(dd)rs(12Drs8Drs3)+rss'(aa)rs(dd)rs'(2Drs'Dss'8DrsDrs'2)+2rsr's'(aa)rs(dd)r's'(Drsr's'Dr's'DrsDr's'2)

where (aa)sr = (aa)rs and (dd)sr = (dd)rs for r <s.

In this presentation, we utilized the assumption of no crossing-over interference which results in the third order linkage disequilibrium of three loci being zero, i.e. Drss' = 0. It may be instructive to show this result.

Drst=E(xrxsxt)=E((zrpr)(zsps)(ztpt))=E(zrzsztprzsztzrpsztzrzspt+prpszt+przspt+zrpsptprpspt)=E(zrzszt12zszt12zrzt12zrzs+14)

Let r1 be the recombination frequency between loci r and s, r2 be that between s and t, and r12 be that between r and t. Under the assumption of no crossing-over interference, for loci r, s, t in this order, we have E(zrzszt) = 12(1 - r1)(1 - r2), E(zrzs) = 12(1 - r1), E(zszt) = 12(1 - r2), and E(zrzt) = 12(1 - r12). Since the assumption of no crossing-over interferene implies r12 = r1 + r2 - 2r1r2, thus Drst = 0.

E. Partition of genotypic variance for the general two-allele model with linkage disequilibrium

Detail of each component of equation (19) for the general two-allele model is presented here.

• The additive variance:

VA=2r=1mpr(1pr)ar2+2rsarasDrs

• The dominance variance:

VD=r=1mpr2(1pr)2dr2+rsdrdsDrs2

• The additive × additive variance:

VAA=2r<s(aa)rs2[(12pr)(12ps)Drs+2pr(1pr)ps(1ps)]+2rss'(aa)rs(aa)rs'[(12pr)Drss'+2pr(1pr)Dss']+12rsr's'(aa)rs(aa)r's'(Drr'ss'+Drs'Dr's+Drr'Dss'DrsDr's')

• The additive × dominance variance:

VAD=2rs(ad)rs2[(12ps)2Drs2+(12pr)(12ps)ps(1ps)Drs+pr(1pr)ps2(1ps)2]+2rs(ad)rs(ad)srDrs[2(12pr)(12ps)Drs+pr(1pr)ps(1ps)]+2rss'(ad)rs{(ad)rs'[Drss'2+(12pr)Drss'Dss'+pr(1pr)Dss'2]+(ad)ss'[2(12ps)Drss'Dss'+ps(1ps)Dss'Drs']+(ad)s'r[2(12pr)Drss'Drs+pr(1pr)DrsDss']+(ad)s's[(12ps)2DrsDss'+(12ps)ps(1ps)Drss'+ps2(1ps)2Drs']}+2rsr's'(ad)rs(ad)r's'(Drsr's'Dss'+Drss'Dsr's')

• The dominance × dominance variance:

VDD=r<s(dd)rs2{[(12pr)(12ps)Drs+pr(1pr)ps(1ps)]2Drs4}+rss'(dd)rs(dd)rs'{[(12pr)Drss'+pr(1pr)Dss']2Drs2Drs'2}+14rsr's'(dd)rs(dd)r's'(Drsr's'2Drs2Dr's'2)

• The covariances:

Cov(A,D)=0Cov(A,AA)=2r<s(aa)rsDrs[(12pr)ar+(12ps)as]+rsr'ar'(aa)rsDr'rsCov(A,AD)=2rsarDrs[(ad)rsDrs+pr(1pr)(ad)sr]+2rsr'ar'(ad)rsDrsDr'sCov(A,DD)=2r<s(dd)rsDrs2[(12pr)ar+(12ps)as]+2rsr'ar'(dd)rsDrsr'DrsCov(D,AA)=2r<s(aa)rsDrs[pr(1pr)dr+ps(1ps)ds]+2rsr'dr'(aa)rsDrr'Dr'sCov(D,AD)=2rsdrDrs(12pr)[Drs(ad)rs+pr(1pr)(ad)sr]+2rsr'dr'(ad)rsDr'rsDr'sCov(D,DD)=r<s(dd)rsDrs2[(12pr)2dr+(12ps)2ds]+2rsr'dr'(dd)rsDr'rs2Cov(AA,AD)=2r<s(aa)rsDrs{(ad)rs[(12pr)ps(1ps)+2(12ps)Drs]+(ad)sr[(12ps)pr(1pr)+2(12pr)Drs]}+2rss'(aa)rs{(ad)ss'[(12ps)Dss'Drs'+2Drss'Dss']+(ad)s's[2(12ps)DrsDss'+ps(1ps)Drss']}+rsr's'(aa)rs(ad)r's'(Drss'Dr's+Drr's'Dss'+Dr'ss'Drs')Cov(AA,DD)=2r<s(aa)rs(dd)rs[2(12pr)(12ps)Drs2+pr(1pr)ps(1ps)DrsDrs3]+2rss'(aa)rs(dd)rs'[2(12pr)Drss'Drs'+pr(1pr)Drs'Dss'DrsDrs'2]+12rsr's'(aa)rs(dd)r's'(Drsr's'Dr's'+Drr's'Dsr's'DrsDr's'2)Cov(AD,DD)=2rs(ad)rs(dd)rsDrs(12ps)[(12pr)(12ps)Drs+pr(1pr)ps(1ps)]+2rss'(ad)rs{(dd)rs'Drss'[(12pr)Drss'+pr(1pr)Dss']+(dd)ss'Dss'(12ps)[(12ps)Drss'+ps(1ps)Drs']}+rsr's'(ad)rs(dd)r's'Drss'Drsr's'

where (aa)sr = (aa)rs and (dd)sr = (dd)rs for r <s.

The result in Appendix D for the F2 model with pr = 1/2 for r = 1, ..., m and also assuming Drss' = 0 is a special case of the results presented here. There is a difference, by a factor -2, on the specification of v variable for dominance effect for the F2 model and the general two-allele model, which carries over to the comparison of results in Appendix D and E.

Contributor Information

Tao Wang, Email: taowang@mcw.edu.

Zhao-Bang Zeng, Email: zeng@stat.ncsu.edu.

Acknowledgements

We are grateful to Bill Hill and Bruce Weir for very helpful discussions and comments and to Wei Zou, Sheng Feng, Sheng-Mao Cheng and Jessica Maia for checking some results. This work was partially supported by NIH GM45344 and by the National Research Initiative of the USDA Cooperative State Research, Education and Extension Service, grant number #2005-00754.

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