Models of Populations
by John Maynard Smith Presented by Elena Fanea
CPSC 605 December 8, 2002
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Models of Populations by John Maynard Smith Presented by Elena Fanea CPSC 605 December 8, 2002 The Message Simple models of population growth and evolutionary change can explain the answer to some important questions Questions ? 1. 2. How
by John Maynard Smith Presented by Elena Fanea
CPSC 605 December 8, 2002
Simple models of population growth and evolutionary change can explain the answer to some important questions
1.
process be ?
population ?
Models of population growth Selection in an asexual population The accuracy of replication Genetic drift in finite populations
Population growing asexually by binary fission Ex: bacteria contains x individuals at time t r·dt = Probability of division in dt r = const - intrinsic rate of increase
rt t
Æ
d
Logarithmic growth
Malthus fi Darwin & Wallace – natural selection K=carrying capacity
˜ ¯ ˆ Á Ë Ê - ⋅ = K x rx dt dx 1
Logistic Equation
x K1 y K2 Populations limited by different resources They will coexist indefinitely => no selection
˜ ˜ ¯ ˆ Á Á Ë Ê - ⋅ =
1 1
1 K x x r dt dx
˜ ˜ ¯ ˆ Á Á Ë Ê - ⋅ =
2 2
1 K y y r dt dy
Populations have the same resources
˜ ˜ ¯ ˆ Á Á Ë Ê +
=
1 1
1 K y x x r dt dx
˜ ˜ ¯ ˆ Á Á Ë Ê +
=
2 2
1 K y x y r dt dy
K1>K2 => x until x+ y = K1 y 0
x selectively eliminates y
Natural selection replacement IIF The two types are limited by the same factors (are competing for resources)
Replication process Exact Too inaccurate No evolution
Critical accuracy Q depends on:
particles In practice, evolution is unlikely if Q<1/2
Practical implication -> genome's size limited
A genome of n nucleotides, u =error of replication/nucleotide Q=(1-u)n @ e –nu => nu<1
Error rates
u non-enzymic replication 10-1-10-2 RNA replication (without “proof-reading” ) 10-3-10-4 DNA replication (with “proof-reading”) 10-9-10-10
Population of replicating RNA molecules S- optimal sequence, unique, produces copies at rate R >r Q-the probability to produce an exact copy of itself
RQx dt dx =
1 1
1 x Q R rx dt dx ⋅
=
1 1 1
x x D rx Rx dt x x d +
= +
If deaths = births, can optimal molecules survive?
( )
p r Rp x x rx Rx D
= + + = 1
1 1
( )
[ ]
1 x p r Rp RQ dt dx ⋅
( )
p R r p Q
= fi 1
at equilibrium
R r Q @
p=proportion of optimal molecules
=fluctuations of proportions of different kinds
fl type a - no selection - type A ‡ p - frequencies - q Np - # of individuals - Nq
Next generation p’, q’ – frequencies E(p’)=p – expected value - unchanged E(q’)=q V=E(p’-p’)2 => V=E(p’-p)2 – variance s(p’)=V1/2 –standard deviation
Family size has a Poisson distribution Each offspring was assigned randomly to one parent, independently Has a probability p of being a The probabilities of 0, 1, 2…N offspring of type a : pN, NpN-1q, N(N-1)/2pN-2q2, …, qN
Standard deviation Variance Mean Frequencies of a individuals Number of a individuals The binomial theorem: Npq
N pq
Npq Np p N pq
Each new individual is equally likely to be produced by any one of the N parents After 2N generations, all will descend from the same individual Standard error >= N
No natural selection=>fluctuant frequencies Population => fluctuations One type will ultimately become fixed, by chance
Simulation
Mathematical models can describe Population growth Selection in an asexual population The accuracy of replication Genetic drift in finite populations And many other aspects of evolution
John Maynard Smith – Evolutionary Genetics,
second edition, Oxford University Press, 2000 chapter 2