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Ageing: Parental Care and Reproduction Strategies
John Thoms, Peter Donahue, Doug Hunter, Naeem Jan
To cite this version:
John Thoms, Peter Donahue, Doug Hunter, Naeem Jan. Ageing: Parental Care and Reproduction Strategies. Journal de Physique I, EDP Sciences, 1995, 5 (12), pp.1689-1695. �10.1051/jp1:1995224�.
�jpa-00247168�
Classification
Physics
,4bstracts02.50-1 05.20-y 87.10+e
Ageing: Parental Care and Reproduction Strategies
John
Tl~oms,
PeterDonal~ue, lJoug
Hunter and Naeem JanPhysics Department,
St. Fian< is Xavier University,Antigomsh,
Box 5000, Nova Scotia,B2G 2W5 Canada
(Receivedls August
199?à, received in final form andaccepted
18August 1995)
Abstract. Trie Penna
bitstring
mortel ofbiological ageing
bas beensuccessfully
used ta illustrate senescence due to mutation accumulation. We introduce several new factors includ- mg parental care whichproduces
a noticeable increase in trie fitness and life expectancy of triepopulation,
achanging reproductive
range which shows trie distinctrelationship
between senes-cence and
fertility,
andsemelparous
mdividuals whichproduce
several new observations suchas a
cyclic population.
1. Introduction
Altl~ough
there are niany diiferent types ofanimais,
triegeneral
pattern of their lives is trie sanie.ivitl~ tl~e
completion
ofpuberty,
weexperience
increasedpl~ysical
detenoration.However,
tl~e rate of tl~is deterioration diifers for eacl~species. Pl~ysical
detenoration witl~time,
rather tl~ansiniply growing aider,
is wl~at is nieantby
the termageing.
Yet the'Why?'
and tl~e 'Howl?' ofageing
remains somewhat of amystery.
However there is growing evidence which linkssenescence
(or ageing)
to thetheory
of mutation accumulation andreproduction
behaviouriii.
This
theory
asserts that ageing is the result offate-acting
deleterious mutations which ai-eweakly
selectedby
raturai selection atreproduction.
The presence of these 'bad' mutations in the individual are felt fate in lire and decrease theability
of theorganism
to carry ont its normalfunctions;
thusmaking
theorganism
moresusceptible
tainjury,
disease, and then death.Having explored
aspects of thistheory
[3], we nowstudy
morecloseljr
therelationship
between
ageing
andreproduction
behaviour:namely semelparous individuals,
which breedonly
once,iteroparous individuals,
which breedrepeatedly, genetic
inheritance ofreproduction
information,
and thereproduction
effort ofparental
cane.2. General Model
We
give
a briefdescription
of the mortel of mutation accumulation used in Durstudy.
A modified PennaI?i 'bit-string'
mortel is used. The mortel has either 3? or 64 genesrepresenting
an
individual,
which may be either 'On' or 'Off'il
or0).
At the start wegenerate
a randomg
Les Editions dePhysique
19951690 JOURNAL DE
PHYSIQUE
I N°12sequence of states to represent
optimal
fitness for the environment. Given apopulation
weincrement the age, 1, of each individual in the
population by (a year)
and this isrepresented by
theexpression
of the i~~ gene. Thenewly expressed
gene iscompared
to itscounterpart
in theoptimal
sequence. Ifthey
agree, then this represents a'good'
gene; if trot, then thisis considered a deleterious
hereditary
mutation. TheHaniming
distance or total deleterious niutations between the activesegnient
and thecorresponding segment
of theoptimal
sequence is used to compute a deathprobability.
We also allow at each timestep
which we refer to as a year, witlt aprobability
of0.01,
for each individual toacquire
a deleterious somatic mutation. Note that this unit of time isspecies dependent
andrepresents
a convenient intervalrepresenting
an observable
change
in theorganism.
A somatic mutation is one that is detriniental to theorganism,
but is trotpassed
on to theofispring.
A Fermi function
involving
the average number of mutations b(hereditary plus somatic),
the actual number of mutations of the individual concemed a, and T, which
plays
the rote ofan inverse
temperature,
is used [3] tocompute
a deathprobability
pdi~~
exp(T(/ a))
+ ~~~This death
probability
is thencompared
with a random numberranging
from zero to one.If the random number faits to exceed the death
probability
then the mdividual is removed from thepopulation.
Anmdependent
term the Verhulst Factoril N(t)/K)
where K is thecarrying capacity
of the environment andN(t)
is thepopulation
at year t functions ma similar manner
removing
individuals when a second random number exceeds the Verhulst term.Ne~v organisms are introduced into the
population
eachhaving
the identicalgenetic string
of itsparent
but we allow withequal probability
for either0, 1,
or 2hereditary point
mutations at birth. This is cloneby simply switching
arandomly
selected gene of theparent
from itspresent state to the
opposite
state.3.
Ageing
audReproduction
Behaviour3.1. REPRODUCTION RANGE AND AGEING IN AN ÎTEROPAROUS POPULATION. TO SÎIOW
clearly
therelationship
between the mutation accumulationtheory
ofageing
andreproduction
range we present the results of two
separate
ruas in which ailparameters except
thereproduc-
tion range are
kept
constant. For both sets of data thepopulation
is monitored to ensure thatwe have reached the
steady
state. These results are for apopulation
whose members maxi-mum life span is 64 years.
Figure
shows thesteady
state age distribution for thereproductive
ranges of10-25 and 20-35. Note how the curve
representing
the olderreproductive period
hasan extended range when
compared
to theformer,
with the demise of thepopulation
now com-ing
at the end of the newfertility
range,35,
rather thon at 25. The correlation between ageingand the
fertility
of an individual isdearly
demonstrated.As the
reproductive
range is shiftedupward
for the same initial conditions the size of thesteady
statepopulation
decreases.Starting
with an initialpopulation of10000,
with halfbeing
identical to the
optimal
sequence we find for thereproductive
range of10-25 thepopulation
sizeis
just
over 8000. For that of14-29 it is under 6500 and for thereproductive
range of 20-35 thepopulation
size is close to 4200. We observe that the averagesteady
statepopulation
decreases almostlinearly
with increase in the minimal âge ofreproduction.
Also as thereproductive
range is shifted
upward
the fitness for anyparticular
age group also increases. For instance the average number of mutations for the age group of13-25 for thereproductive
range of 11-25 is 1.65 ascompared
to 0.23 for individuals in the same age group where thereproductive
rangeiooo
goo
Hep Range 10.25 ~
~
Hep Range20.35 +
800 ~
700 ~
~ 600 ~
o ~
~
é 500 ~
É
Î ~
fl 400 ~
~
~ +
~ + o
~ ~
+
~ ~
zoo ~
+
+ +
~ + o
+ + o
~ + +
+ Î
q
~ loo
~
~ ~ ~ +
+ + +
~
o 5 1° ~
ÀÎe ~~ ~~ ~~ ~~
Fig.
l. Trie age distribution of trieiteroparous population
where triereproductive
range is 10-25, and where it is 20-35. Ail other parameters arekept
constant. Note that as triereproductive
range is shiftedupward
the size of thesteady
statepopulation
isreduced,
while the fitness of thepopulation
mcreases.
of 20-35 an
improvement
of over80%.
Aplot
ofthe fitness in the range 13-25 shows asharp
decrease withincreasing
shift in thereproductive period, reaching
a minimum for values of thereproductive period
from 16-31 andgreater.
The average number of mutations with age and tl~e age at wl~icl~ deatl~ occurs show similarpatterns
for tl~e differentreproductive
ranges butare soniewl~at stretcl~ed to include tl~e end of tl~e
fertility
range.3.2. SEMELPAROUS REPRODUCTION.
Looking
at trie nature ofsenlelparous reproduction
habits,
we consider a mortel wl~ere each member of the initialpopulation,
whose maximum life span is 32 years, isgiven
asingle
age(ranging
from10-32)
at wl~ichthey
wouldgive
birtl~to 0-3
offspnng
withequal probability.
This âge at whichreproduction
occurs is thenpassed
on to their
offspring.
As seen inFigure 2a,
within 1000 years ail members of thepopulation
with
reproductive
ages other thon 10 l~ad died out,leaving
apopulation
of individuals wl~oreproduce simultaneously
every ter years, witl~ a aine year gap when no new individuals are boni(as
sl~own inFig. 2b). Naturally
this led to a 10 yearpopulation cycle
wl~icl~ is restrictedby
tl~e Verl~ulst factor.This
cycle migl~t
hâve been initiatedby
tl~e fact tl~at our initialpopulation
ail had an âge of 0 and tl~us ail tl~epeople
willreproduce
at ten years of age and tl~eiroffspring
willgive
birth at year
20,
and so on. To overcome this weassign
a random age to each member of the initialpopulation.
Tl~e mdividuals whoreproduce
at ages other tl~an ten died out onceagain,
but this time there are several groups of
people giving
birth in each year of the ten yearquasi periodic cycle. (ie.
One groupgiving
birth at10, 20, 30...,
anotl~ergiving
birth atIl, 21,
31..and so
on.)
As time went onl~owever,
ail tl~e groups died outexcept
for one, as seen in tl~e birtl~s witl~ timegrapl~
inFigure
3. Tl~is group exl~ibits tl~e saine ten yearcycle
as tl~e previousrun of this
type (Fig. 2b).
Thephenomenon displayed
inFigure
3 where one groupeventually
dominates the
population
is very similar to that found in the modified Ehrenfest um mortel [4]in which an
equal
number of10 different coloured balls areplaced
into an urn. Half of the balls1692 JOURNAL DE
PHYSIQUE
I N°1220
15
w1
(
wé 10
9
~
oe
o
o zoo 400 600 800 looo
Year
&)
loooo
,Number OfBinhf
, j , PoiulationwithTimfl
1, .; il ') Il
ÎÎ 'Î )(
lÎ Î1
>' 1.
'>
8000
;
~~ ~ ~~
~ ~
"
".
~
"
2000
o
15000 15010 15020 15030 15040 15050 15060
Year
b)
Fig. 2. Trie average age of reproduction with time for
a semelparous population. Age of reproduc- tion for trie initial
population
israndomly
set to bea
surgie
year m trie range la 32. A combination of trie number of births per year and triepopulation
size with time(in years),
for trie timeperiod
of15000 to 15060.
are tlien removed followed
by doubling
the number of balls of each colour in trie um. Thisprocedure
is thenrepeated by
removing half the balls andcontinuing
the process. With timeonly
one colour of theoriginal
10 remains.Having
arigid siitgle
year ofreproduction
would al1&>ays lead to the type ofpopulation
and birthcycle
(lescnbed above. Therefore wegive
each individual asingle
age at which toreproduce,
but hm,e this âge chosenrandomly
to be10,
ii, or12,
for both the initialpopulation
and theiroffspnng.
This gai>e a much more uniformpopulation
over time and dia7000
g
à 4000
à
3
~
fl 3000
~
=
2000 ''
'.>.~ f"'
~
i wJ'Îj 'Î "
1000 j j' i
w'.
~
'" ~
"~.' ~4) '
', ~.' [ ~"N~
~
o 2000 4000 6000 8000 loooo 12000 14000 16000 18000 20000
Year
Fig.
3. Trie number of births per year recorded for 20000 years. Each fine represents a different reproductive group.(See text)
net exhibit the 10 year birth
cycle
frein our earlier runs.Catastrophic
senescence is observed if the value of T in the Fermitype
deathprobability
is increased. Tplays
the rote of the inversetemperature
whichcorresponds
to trie tolerance of the environment to1&>ards differences of an mdividual from the average fitness. We found thatby increasing
the value of Tthereby decreasing
the tolerance of the environment from 10 to 100 extreme senescence is observed afterreproduction.
This result confirms the main conclusion of Penna et ai.[si.
We consider another variance of the mortel where each individual is
given
asingle
âge at whichthey
wouldgive
birth(10, ii,
or12).
At this time ho1&>ever,90%
of the children were given tl~e age ofreproduction
as tl~eirparent
witl~ tl~eremaining 10%
given a random âge ofreproduction.
Tl~eresulting steady
statepopulation
bas an average âge ofreproduction
of 10.56 and an average age of deatl~ of 12.21. In tl~esteady
state, births teckplace
every year,as
opposed
to ailbeing
in tl~e same year, so thepopulation
dia not follow alongterm penodic cycle.
~vl~en tl~is rua isrepeated
witl~ cl~ildrenha,>mg
a99%
chance ofreproducing
at tl~esame age as tl~eir parent, the average of age of
reproduction drops
to 10.16 and the a,>erage age of death faits to 11.67.Agoni
thepopulation
showed nolongterm periodic cycle,
and not ail tl~e births occured in the same year. Tl~egreater
trie chance ofhaving
a birtl~ at trie same age as theirparent
triestronger
tl~etendency
tov>ard senescence after trie age ofreproduction.
3.3. PARENTAL CARE IN AN ITEROPAROUS POPULATION. Trie above results ai-e observed
for mortels wl~icl~ dia net take into account
reproduction
effort.By reproduction
effort we mean tl~e energy devoted to secunng mates, toreproducing
wl~ich isdependent
on the prospects for futurereproduction
-, and investment in tl~e
offsprmg
after birtl~(parental care).
To observe tl~is effect tl~ebitstring
mortel isadapted
to inclttde tl~econcept
ofparental
care.This is tl~e first time to ouf
knowledge
that anyone lias studied the effects ofparental
care.Parental care is introduced into trie mortel trot 1&:ith trie parents receiving any
davantage,
but with theiroffspnng doing
so. Trie mdividual whose parent is still olive evades triepopulation
size check of the Verhulst factor.
However,
thisplaces
older members of thepopulation
at1694 JOURNAL DE
PHYSIQUE
I N°121600
NO Parental Care o
+ With Parental Care +
1400 +
+
+
+
© +
i~
~ ° +
É
Î
~ o
Z ~
o
+ o
o o
+
o +
o ~
o
~
°
o +
°
o ~
o $ +
° o
0 5
Fig.
4. Trie age distribution of trie iteroparouspopulation
with and without triereproduction
effort ofparental
care. Note that trie introduction ofparental
care increases both thesize of the steady state
population
and the bfe expectancy.a
disad,>antage
sincethey
will be now morelikely
eliminatedby
the Verhulstfactor; yet
themajor
result observed from the introduction ofparental
care is the noticeable increase in lifeexpectancy
and in the overall fitness of thepopulation.
Note the difference between the age distributiongraphs
inFigure 4,
withoutparental
cane, and of the caseincorporating parental
care. The average number of mutations for the age group of13-25 without
parental
care [3]is
I.Il, whereas,
m the trialincluding parental
care it is0.48;
a70% improvement.
For therun 1&,ith
parental
care the âge at death curve is less dramatic than trie run withoutparental
care, with the second
peak being
more of abump
followedby
asharp
decline at the end of thefertility
range. This data is collected from triestudy
where each individual has a maximumlifespan
of 64 and areproduction
range of10 25. For an initialpopulation of10000,
thesteady
state iteroparouspopulations
for the two cases differby 6000,
with thesteady
statepopulation being
15000 withparental
care and 9000 withoutparental
care.4. Conclusion
We have shown that the modified Penna
bitstring
mortel for mutation accumulationtheory
ofageing
is well suited to sholv- therelationship
between senescence andreproductive
behavior.The
relationship
betweenfertility
and ageing isclearly displayed,
with the demise of the popu- lation commg at the end of thereproductive
range.Also,
we bave illustrated the trend towardpopulation cycles
forsemelparous
species withngidly
mhented ages ofreproduction,
and the overcommg of this trend when the age ofreproduction
is allowed to varyslightly.
With the introduction ofparental
cane into themortel,
we observe an increase in the life expectancy and overall fitness of the mdividuals in thepopulation.
Future areas ofstudy
on the mechanismsof agemg and
reproduction
may mdude the introduction of achanging
environment, and apopulation
whichreproduces sexually.
Acknowledgments
We welcome the
opportunity
to thank Professor Stauffer and his associates at KoInUniversity,
as well as Professor Penna and his collaborators at Universidade Federal
Fluminense,
forkeep-
mg us informed of their work and also for their
encouragement.
We areobligated
to Rachel Bland for her comments andsupport.
This research issupported
inpart by
NSERC of Canada and a UCRgrant
from St. Francis XavierUniversity.
References
iii
RoseM.R.,
EvolutionBiology
ofAging, (Oxford
Univ. Press Oxford1991)
and see referencestherem for earlier hterature; Charlesworth B., Evolution m
Age-structured Populations,
2ndedition,
(Cambridge
Univ.Press, Cambridge 1994);
Stauffer D., Braz. J.Phys.
24(1994)
900.[2] Penna
T.J.P.,
J. Stat.Phys.
78(1995)
1629; Bernardes A.T. and Stauffer D., submitted(1995);
Penna T.J.P. and Stauffer D., Int. J. Med.
Phys.
C 6(1995)
233; Moss de OliveiraS.,
Penna T.J.P. and StaufferD., Physica
A215(1995)
298; Vollmar S. andDasgupta S.,
J.Phys.
I France 4(1994)
817.[3] Thoms J., Donahue P., Jan N., J.
Phys.
I France 5(1995)
935.[4] Johnson N-L- and Kotz
S.,
Urn Models and theirApplications:
AnApproach
to Modem DiscreteProbability, (Wiley,
New York1977).
[5] Penna T.J.P., Moss de Oliveira S. and Stauffer D., to appear m Rapid Communications m
Phys.
Reu..