The
Englishman HARDY and the German WEINBERG could show that the frequency of
homozygotes and heterozygotes in a population stays constant for generations if
certain conditions are fulfilled. The HARDY-WEINBERG
law permits the theoretical
calculation of the frequency a certain genotype has in a given population
independent of the number of existing alleles.
The
Mendelian laws start out from two individuals (parents) and their offspring.
Hereditary traits as they have been described till now can only be understood
under controlled conditions. Ratios like 3:1 will hardly be discovered in
nature since every species has to be regarded as a group of populations in
which certain genotypes occur in certain amounts hard to capture. The frequency
of an allele can be very low and genetic combinations where it has part in will
inevitably be very rare.
The Englishman G. H. HARDY and the German W. WEINBERG showed independent of each other in 1908 and 1909 that the frequency of homozygotes and heterozygotes stays constant for generations, if
- the population is very large,
- the individuals can pair without limitations (if they belong to different sexes and live at the same place and at the same time, of course),
- there is no selection of certain alleles,
- no gene migration occurs and
- no mutations take place.
Derivative:
Given:
two pairs of alleles, A and a
Assumed: the frequency of A
shall be p = 0.9 (= 90%) that of a shall be q = 0.1 (= 10%)
From that follows: p + q = 1
In the
population, the genotypes AA, Aa and aa will thus be found. The produced germ
cells would either contain A or a. If they cross according to chance, it has to
be taken into account that germ cells containing A have the frequency p and
germ cells equipped with a the frequency q. These genotypes will accordingly
occur in the following generation with the following frequencies:
AA
= 0.9 x 0.9 = 0.81
Aa = 0.9 x 0.1 = 0.09
aA = 0.1 x 0.9 = 0.09
aa = 0.1 x 0.1 = 0.01
or, expressed mathematically: AA
= p2 ; Aa + aA = 2pq ; aa = q2
or: p2 + 2pq + q2 =
(p + q)2 = constant
Or, expressed in words: under
the conditions mentioned above, the original ratio of the alleles A and a will
be retained from generation to generation. There can be any number of alleles
per gene in a population. The genome of an individual is therefore just a
chance selection of the whole gene pool.
The Hardy-Weinberg law allows
the calculation of the heterozygous individuals' frequency. When two alleles
exist, it can never be larger than 0.5. The following picture shows the
quantitative relation between the frequencies of the alleles and those of the
respective genotypes (according to D. S. FALCOMER, 1960).
If an allele has a high
frequency, the relation of the genotypes will shift strongly in favour of the
respective homozygous genotype. But since the preconditions for Hardy-Weinberg
are usually not given, plant populations being often very small and
self-pollination being no exception, the law cannot be applied here. MENDEL
himself tackled this problem in his classic study in 1866 and asked how the
splitting ratios of subsequent generations would look, if the offspring of
every new generation would always be crossed with each other.
A
population with random mating results in an equilibrium distribution of
genotypes after only one generation, so that the genetic variation is
maintained f When the assumptions are met, the frequency of a genotype is equal
to the product of the allele frequencies AA:Aa: aa: p2 2pq q2
The
H-W equilibrium states that sexual reproduction does not reduce genetic
variation generation after generation; on the contrary, the amount of variation
remains constant if there are no disturbing forces acting against it. It
establishes the relationship for calculating genotype frequencies under random
mating and, in doing so, provides the foundation for many studies in population
genetics.
Hardy–Weinberg
equilibrium is impossible in nature.
·
Static
allele frequencies in a population across generations assume: random mating,
no mutation (the alleles don't change), no migration or emigration
(no exchange of alleles between populations), infinitely large population size,
and no selective pressure for or against any traits.
·
The
Hardy-Weinberg model, named after the two scientists that derived it in the
early part of this century, describes and predicts genotype and allele frequencies
in a non-evolving population.
·
The
model has five basic assumptions
·
The
population is large (i.e., there is no genetic drift);
·
There
is no gene flow between populations, from migration or transfer of gametes;
·
Mutations
are negligible;
·
Individuals
are mating randomly; and
·
Natural selection is not operating on the population. Given these
assumptions, a population's genotype and allele frequencies will remain unchanged
over successive generations, and the population is said to be in Hardy-Weinberg
equilibrium. The Hardy-Weinberg model can also be applied to the genotype
frequency of a single gene
Importance
·
The
Hardy-Weinberg model enables us to compare a population's actual genetic
structure over time with the genetic structure we would expect if the
population were in Hardy-Weinberg equilibrium (i.e., not evolving).
·
If
genotype frequencies differ from those we would expect under equilibrium, we
can assume that one or more of the model's assumptions are being violated, and
attempt to determine which one(s).
·
How
do we use the Hardy-Weinberg model to predict genotype and allele frequencies?
What does the model tell us about the genetic structure of a population?
The
starting point is generation 0. We have a gene with two alleles, A1 and A2. The
frequency of allele A1 is p and the frequency of allele A2 is q. The genotype
frequencies in generation 0 are for A1 A1 = p2, for A1 A2 = 2pq and for A2 A2 =
q2. If random mating occurs, the probability of any allele from the female
plant meeting any allele from the male plant will be the sameThe frequency of
occurrence of each genotype is given by the product of the frequency of each
allele in the genotype (e.g. for A1 A1 is p x p = p2).
|
|
Genotypes of G0 |
G0 |
Genotypes of G1 |
G1 |
||||||
|
Popul. |
A1A1 |
A1A2 |
A2A2 |
p |
q |
A1A1 |
A1A2 |
A2A2 |
p |
q |
|
Pop.1 |
0.6 |
0.2 |
0.2 |
0.7 |
0.3 |
0.49 |
0.42 |
0.09 |
0.7 |
0.3 |
|
Pop.2 |
0.49 |
0.42 |
0.09 |
0.7 |
0.3 |
0.49 |
0.42 |
0.09 |
0.7 |
0.3 |
|
Pop.3 |
0.4 |
0.6 |
0 |
0.7 |
0.3 |
0.49 |
0.42 |
0.09 |
0.7 |
0.3 |
An example of three population in Hardy Weinberg equillibrium
Population
genotype frequencies are given in rows. Generations (G0 and G1) are given in
columns. Again, we have one gene with two alleles, A1 and A2. The frequency of
allele A1 is p and the frequency of allele A2 is q. Genotype frequencies are
different for each population in generation 0 (e.g. the frequency of A1 A1 in
population 1 is 0.6; in population 2, 0.49; and in population 3, 0.4, and so on
for the other genotypes). We note, though, that the allele frequencies in the
three populations are similar in G0 (p = 0.7 and q = 0.3). In the next
generation, G1, if all requirements of the H-W principle are met, the genotype
frequencies in the three populations balance (now the frequency of A1 A1 is
0.49 in the three populations, and the same happens with the frequencies of A1
A2 and A2 A2 ). The allele frequencies are kept.
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