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Exact Results of the Bit-String Model for Catastrophic Senescence
T. Penna, S. Moss de Oliveira
To cite this version:
T. Penna, S. Moss de Oliveira. Exact Results of the Bit-String Model for Catastrophic Senes- cence. Journal de Physique I, EDP Sciences, 1995, 5 (12), pp.1697-1703. �10.1051/jp1:1995225�.
�jpa-00247169�
J.
Phys.
I France 5(1995)
1697-1703 DECEMBER1995, PAGE 169îClassification
Physics
Abstracts05.50+q 89.60+x 07.05Tp
Exact Results of trie Bit-String Model for Catastrophic
Senescence
T.J.P.
Penna(~)
and S. à~oss deOliveira(~*)
Instituto de Fisica, Universidade Federal Fluminense, Av. Litorânea
s/n,
BoaViagem,
24210-340
Niterôi, RJ,
Brazil(Received
14August
1995,accepted
in final form 18August 1995)
Abstract. We succeeded in
obtaining
exact results of triebit-string
mortel ofbiological aging
forpopulations
whose individuals breedonly
once. These resultsai-e in excellent agreement with those obtained
through
computer simulations. In addition, we obtaiu an expression for trieminimum birth needed to avoid mutational meltdown.
1. Introduction
The
aging
is characterizedby
trie loss ofcapabilities;
in an irreversible way,predominantly
after trie
maturation,
for trie most ofspecies. Mary
factors can influence trieaging
process:biochemical processes, environment and so fortin.
Recently,
many efforts bave been directed towards anevolutionary theory
ofaging [1-3].
Trie fundamentalquestion: Why people get
old ? has beenrecently replaced by: ivhy
is the survivalprobability
of an individual reducedwith
advancing
age ? The reason is the latter is more suited to be answered with the tools ofdynamics
ofpopulation
and MathematicalPhysics methods,
assuggested by
Roseiii.
Fora review of Monte Carlo simulations in
biological
aging see, for instance, reference[4].
Thetheories of
evolutionary
aspects of aging fall in two classes:optimality
theoptimal
lifestrategy
is anemphasis
onearly
maturationtl~at,
due topl~ysiological
constraints. leads to a decrease in tl~e life span; andgenetic explanations
deleterious(bad)
mutations for old ageare
subject
to a weaker selection tl~at tends to accumulate tl~em later in tl~e life time.Sometimes,
aging effects aredisplayed
in an amazing way, like in tl~e so-calledcatastropl~ic
senescence. It is a well known fact tl~at
semelparous individuals,
1-e-, those wl~icl~ breedonly
once,
usually
presentcatastropl~ic
senescence, thatis, tl~ey
aiesl~ortly
afterreproduction [3].
Owing
to its commerciali>alue,
tl~e Pacific salmon is one of tl~e mostimportant exaiuples.
Thecatastrophic
senescence has been studied in a mortel ofoptiniality (Partridge-Barton mortel) [3, si. Nevertheless,
if weaccept
that natural selectionpre,>ents
tl~e manifestation of deleterious(" e-mail:
tjpp©if.uff.br
(** e-mail: suzana@if.uff. brQ
Les Editions dePhysique
19951698 JOURNAL DE
PHYSIQUE
I N°12mutations before
procreation,
it is easy to understandwhy
tl~ispremature
senescence occurs:after
reproduction,
tl~e individuum does not need to beprotected
anymore, since it is notgoing
to
produce offspring
anylonger.
Tl~e
bit-string
mortel of lifel~istory, recently
introduced[6, 7], specifically
makes use of a bal-ance between
l~ereditary
mutations andevolutionary
selection pressure.Computer
simulations of tl~ebit-string
mortel bave sl~own tl~at thecatastropl~ic
senescence can also be understood~vitl~in the framework of mutation accumulation
theory. Furtl~ermore,
it waspossible
to showthat senescence is a direct result of tl~e age of
reproduction
[8].Here,
we presentanalytical
calculations whicl~ confirm that tl~e life
strategy
ofreproducing only
once leads to tl~e catas-trophic
senescence. This paper isorganized
as follows: in Section2,
webriefly
describe thebit-string
mortel. In Section3,
we derive ouranalytical
results and discuss themby
compansonwitl~
computer
simulations.Finally,
m Section 4 wepresent
ouf conclusions.2. The Model
Consider an initial
population N(t
=
0)
of individuals eacl~ one cl~aracterizedby
a word of B bits. Tl~is word is related to tl~egenetic
code of eacl~individual,
since it contains tl~einformation of iv-hen tl~e effect of a deletenous mutation will take
place (bit
set toone)
or not
(bit
set tozero) dunng
the life of the individual. We can consider the time as a discrete variablerunning
from to B years.Hence,
if at time t = i the i~~ bit in tl~e wordequals
one, it is considered tl~at tl~e individual will suffer tl~e effects of a deleterious mutationin that year and all
following
years. The mutations arehereditary
in tl~e sensetl~at,
at tl~e birth of a newindividual, they
are transmitted to tl~is new individual except for M bits(M
will be called mutation rate,
hereafter), randomiy
chosen. These mutations concorrespond
to either an additional deleterious mutation or acleaning
of a deleterious mutationpresent
at theparent's
genome. We can interpret this new mutation as a point mutation(if
we areconsidenng
asexual
reproduction)
or a recombination of theparent's
genome in sexualreproduction.
An individual will aie due to aging effects if the number of deleterious mutations tl~at were relevant up to its age isequal
to a tl~resl~old T.Competition
betiv-een tl~e individuals of apopulation
for food and space, forexample
are introduced
taking
into accourt anage-independent
Verhulstfactor,
wl~icl~gives
to eacl~individual a
probability
x =il Ntot(t)/Nmax)
ofstaying
alive.Nmax
means tl~e maximum size of tl~epopulation.
Eacl~surviving
individualgenerates,
at tl~ereproduction
age R, boffspnngs.
As stressed in reference[9],
tl~e fact of individuals breedonly
once in their lifetimesis tl~e fundamental
ingredient
toexplain
tl~ecatastropl~ic
senescence.3.
Analytical
Calculations and ResultsThe relevant parameters in our calculations are:
. B
genotype lengtl~,
inbits;
. b birth
rate;
. R the
reproduction
age;. x the Verhulst
factor;
. iv number of deletenous mutations added at birth.
. T tl~resl~old
starting
from ~vl~ich tl~e mutations lead to deatl~.N°12 BIT-STRING MODEL FOR CATASTROPHIC SENESCENCE 1699
Let us assume tl~at tl~e system bas reacl~ed an
equilibrium
state(tl~is liypotl~esis
isplausible
since
computer
simulations bave sl~own tl~at it al1&,aysoccurs).
Since tl~e age distribution andtl~e
population
arestationary,
we can consider tl~e Verl~ulst factor as constant. In tl~iswork,
for tl~e sake ofsimplicity,
we assumeonly
deleterious mutations at birtl~ witl~ T=
1,
1-e-, tl~e effects ofjust
one deleterious mutation isenougl~
to cause tl~e deatl~ of an individual. Tl~e extension for different values of T isstraigl~tforward, altl~ougl~
we bave learned fromprevious
computersimulations results tl~at it is trot
important
for tl~ecatastropl~ic
senescenceexploration.
Let us consider one bas Jh~ individuals with zero age, after trie
stationary
state has been reacl~ed. Theprobability
of a deleterious mutation to appear at agiven
age is(tif/B), for
agesbeiow
R,
since in this case we con be sure that theparent
bas no mutations up to age R(T
=
1)
and tl~e mutations at birtl~ are
randomly
cl~osen(we
areconsidering
tl~e case AI «B).
For agesbeyond R,
we must take into account the wholeparent's l~istory,
and tl~is will be clone later. Firstignoring birtl~s,
we conexpect
tl~at tl~e number of individuals witl~ age 1 will beNi =fif~ Ii j) =fifx
~~ j~). (1)
Analogously,
~~ ~~~ ~
B~11 ~~~ ~~ B~~ ~(B~~l)
~~ ~~~is tl~e number of individuals witl~ age 2. For
general
age k <R,
one bas~~ ~~~ ~~
~B~- i~ÎÎ
~~~Now,
we take into account tl~ereproduction
of trie individuals at age R. Since eacl~ individuumproduces
boffsprings,
tl~e number of individuals witl~ zero age will be b times tl~e number of age R in tl~e previous step:~~
~~~ ~~
~B~- iÎÎ
~~~~
Using
tl~e aboveequation,
witl~tif
=
No,
one can obtain tl~estationary
state conditionx~ fl
~ ~ ~= i
(5)
~i
~~~+~
As we sl~ould expect, tl~is condition does not
depend
on k butonly
on tl~eglobal
parametersR, M,
b and B. For M= 1 it reduces to
bx~(B R)/B
= 1.
For ages k >
R,
we mustgarantee
tl~at no mutation occurred between ages R and k. Theprobability
that no mutation has occurred until agek,
in the t~~=
1,
2. ancestor(parent,
grand
parent,etc.)
is(see Eq. (3)):
lk
~ ~§ B~-1+Î~~'
~ ~~~and this is a necessary condition for the individual to be still
olive,
to be fulfilled for all ancestors.However, except
for M =0,
this term goes ta zero as t increases. In tl~is 1&>ay, in order to bave tl~estationarity
conditionsatisfied,
we must baveNk>R
" 0.
(7)
lî00 JOURNAL DE
PHYSIQUE
I N°12o i
S
N°12 BIT-STRING MODEL FOR CATASTROPHIC SENESCENCE 1701
ioo
'Éc
~ io
u
0 2 3 4 5
M
Fig.
2. Minimum birth rate bm~,, us. mutation rate IV. Trie solid finescorrespond
toanalytical
results for R
= 5,10, là, 20 from trie bottom to trie top. Trie
symbols correspond
to computer sim-ulations R
=
5(D),10(O),15(li)
and20(o).
In trie computer simulations, we carionly
obtain triemaximum integer value below which trie
population
vanishes(mutational meltdown).
That iswhj,
these results are belo~v the theoretical results. trie do not present results for
larger
values of b because it would reqmre ahuge
number of time steps until trie population vanishes.that tl~e mutational meltdowii does Rot
depend
on trie size ofpopulation
at least for asexualsemelparous
species in contrast witl~ earlierbiological assumptions
tl~at tl~is effect occursonly
on smallpopulations.
~Îe present inFigure
2 some curves forb,n,n
as a function of Jf.For
comparison,
wepresent
some results from computer simulations. However, siiice we bave 1&>orkedonly
withinteger
values ofb,
tl~e tl~eoretical results should be considered as an upper limit. Forlarge
values of b(typically
>10)
and l~igl~ mutation rates(fil
>3),
tl~e number of timesteps
needed to reacl~ tl~eequilibrium
is verylarge.
For a moreprecise
determination ofbm,n,
we tried anexponential fit,
forNtot
us. t(for
10000 < t <100000),
and we cl~ecked triesign
of tl~e exportent to determine wl~ether thepopulation
wouldeventually
vaiiisl~. Since tl~estudy
ofdynamical aspects
of tl~is mortel are Dot into the scope of this work, we presentonly
the more reliable results.
Trie relevant
quantities
in aging studies are tl~e survival ratesSk,
1-e-, trieprobabilities
of anindividual to survive to the next age.
Tl~ey
cari beeasily
obtained frontequation (8):
~~ ÎÎÎI
~B~ kÎÎ Î
B
~i ~MÎ1~
~~~~~~~
Tl~e survival rate for age k
gives
tl~eprobability
that individuals alive at age k -1 surviveand reacl~ age k. In
Figure 3,
we compare tl~is expression for different values of b and R1&~itli computer simulation results. Tl~eabrupt jump
to zero at k= R is
clearly
seen.lî02 JOURNAL DE
PHYSIQUE
I N°12.-.-.-.-.-.-.-.-.-.-.-.-.-.-.-.-.-._._.
0.8 ~~~~~~~~~~
,
j~ce
~ Off lC
)
(
0.4Ù7
o_2
°'°~
~ 10 lS 20 25
Age
Fig.
3. Survival rates us. age. Here, we present trie results for M = 1,b= 5, R
= II
(O
and sohdbne),
R= 20
(.
and dashedhne)
and b= 10, R
= II
(li
and dottedfine).
We followed trie same strategy of averagmg asadopted
inFigure
1.Again,
trie agreement betweentheory
and computerexperiment is renlarkable.
4. Conclusions
Using simple
statistical arguments, we bave solvedanalytically
tl~ebit-string mortel,
for semel- parousspecies
as tl~e Pacific salmon andmayflies.
Dur results confirm tl~osepresented
in reference[9],
where it is claimed tl~at trie lifestrategy
ofjust
onebreeding attempt
leads tocatastl~rophic
senescence,according
to tl~e mutation accumulationtl~eory.
Inaddition,
we can obtain ananalytical
expression for thepopulation
size ofsemelparous
species as function ofmutation rate and
reproduction
age(an exponential decay
for the same conditions of space andfood),
and tl~e minimum birtl~ rate to avoid mutational meltdown. Dur results also agree witl~ tl~ose foundby
Bernardes andStauffer, suggesting
tl~at trie mutational meltdown is not an effect of smallpopulations. Nevertl~eless,
we bavefound, by
computerexperiments,
tl~at tl~e timerequired
for apopulation
to vanisl~ con be verylarge.
In this sense, wesuggest
tl~at it can be wortl~studying
tl~edynamical aspects
of tl~ebit-string mortel,
for botl~semelparous
and
iteroparous
species.As a final remark we wish to
point
out tl~ataltl~ough dealing
witl~semelparous organisms,
tl~e extension for
iteroparous organisms (whicl~
breedrepeatedly)
isstraightforward,
but thecorresponding expressions
are toolengtl~y
to be useful.Acknowledgments
This work was motivated
by
aquestion
raisedby
Naeem Jan about aprevious
paper. Weare
grateful
to hiin for bis interest in ouf work. Due of us(TJPP)
is alsograteful
to Silvio Salinas and Nestor Caticl~a forencouragement,
and tl~e otl~er(SMO)
to P-M-C- de Oliveira forimportant suggestions,
and to Hans J. Herrmann for bisl~ospitality
at ESPCI wl~ere tl~iswork 1&,as concluded. Tl~is work is
partially supported by
Brazilianagencies CNPq, CAPES,
FAPERJ and FINEP.
N°12 BIT-STRING MODEL FOR CATASTROPHIC SENESCENCE 1703
References
iii
Rose M.R., TrieEvolutionary Biology
ofAging (Oxford
Univ.Press,
Oxford1991).
[2] Charlesworth B., Evolution in
Age-structured
Populations, 2nd edition(Cambridge
Univ. Press~Cambridge 1994).
[3]
Partridge
L. and BartonN-H-,
Nature 362(1993)
305.[4] Stauffer
D.,
Braz. J.Phys.
74(1994)
900;[5] Jan
N.,
J. Stat.Phys.
77(1995)
915.[6] Penna T.J.P., J. Stat.
Phys.
78(1995)
1629.[7] Penna T.J.P. and Stauffer D., int. J. Med.
Phys.
C6(1995)
233.[8] Thoms
J.,
Donahue P. and Jan N., J.Phys.
I France 5(1995)
935.[9] Penna