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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�

(2)

J.

Phys.

I France 5

(1995)

1697-1703 DECEMBER1995, PAGE 169î

Classification

Physics

Abstracts

05.50+q 89.60+x 07.05Tp

Exact Results of trie Bit-String Model for Catastrophic

Senescence

T.J.P.

Penna(~)

and S. à~oss de

Oliveira(~*)

Instituto de Fisica, Universidade Federal Fluminense, Av. Litorânea

s/n,

Boa

Viagem,

24210-340

Niterôi, RJ,

Brazil

(Received

14

August

1995,

accepted

in final form 18

August 1995)

Abstract. We succeeded in

obtaining

exact results of trie

bit-string

mortel of

biological aging

for

populations

whose individuals breed

only

once. These results

ai-e in excellent agreement with those obtained

through

computer simulations. In addition, we obtaiu an expression for trie

minimum birth needed to avoid mutational meltdown.

1. Introduction

The

aging

is characterized

by

trie loss of

capabilities;

in an irreversible way,

predominantly

after trie

maturation,

for trie most of

species. Mary

factors can influence trie

aging

process:

biochemical processes, environment and so fortin.

Recently,

many efforts bave been directed towards an

evolutionary theory

of

aging [1-3].

Trie fundamental

question: Why people get

old ? has been

recently replaced by: ivhy

is the survival

probability

of an individual reduced

with

advancing

age ? The reason is the latter is more suited to be answered with the tools of

dynamics

of

population

and Mathematical

Physics methods,

as

suggested by

Rose

iii.

For

a review of Monte Carlo simulations in

biological

aging see, for instance, reference

[4].

The

theories of

evolutionary

aspects of aging fall in two classes:

optimality

the

optimal

life

strategy

is an

emphasis

on

early

maturation

tl~at,

due to

pl~ysiological

constraints. leads to a decrease in tl~e life span; and

genetic explanations

deleterious

(bad)

mutations for old age

are

subject

to a weaker selection tl~at tends to accumulate tl~em later in tl~e life time.

Sometimes,

aging effects are

displayed

in an amazing way, like in tl~e so-called

catastropl~ic

senescence. It is a well known fact tl~at

semelparous individuals,

1-e-, those wl~icl~ breed

only

once,

usually

present

catastropl~ic

senescence, that

is, tl~ey

aie

sl~ortly

after

reproduction [3].

Owing

to its commercial

i>alue,

tl~e Pacific salmon is one of tl~e most

important exaiuples.

The

catastrophic

senescence has been studied in a mortel of

optiniality (Partridge-Barton mortel) [3, si. Nevertheless,

if we

accept

that natural selection

pre,>ents

tl~e manifestation of deleterious

(" e-mail:

tjpp©if.uff.br

(** e-mail: suzana@if.uff. br

Q

Les Editions de

Physique

1995

(3)

1698 JOURNAL DE

PHYSIQUE

I N°12

mutations before

procreation,

it is easy to understand

why

tl~is

premature

senescence occurs:

after

reproduction,

tl~e individuum does not need to be

protected

anymore, since it is not

going

to

produce offspring

any

longer.

Tl~e

bit-string

mortel of life

l~istory, recently

introduced

[6, 7], specifically

makes use of a bal-

ance between

l~ereditary

mutations and

evolutionary

selection pressure.

Computer

simulations of tl~e

bit-string

mortel bave sl~own tl~at the

catastropl~ic

senescence can also be understood

~vitl~in the framework of mutation accumulation

theory. Furtl~ermore,

it was

possible

to show

that senescence is a direct result of tl~e age of

reproduction

[8].

Here,

we present

analytical

calculations whicl~ confirm that tl~e life

strategy

of

reproducing only

once leads to tl~e catas-

trophic

senescence. This paper is

organized

as follows: in Section

2,

we

briefly

describe the

bit-string

mortel. In Section

3,

we derive our

analytical

results and discuss them

by

companson

witl~

computer

simulations.

Finally,

m Section 4 we

present

ouf conclusions.

2. The Model

Consider an initial

population N(t

=

0)

of individuals eacl~ one cl~aracterized

by

a word of B bits. Tl~is word is related to tl~e

genetic

code of eacl~

individual,

since it contains tl~e

information of iv-hen tl~e effect of a deletenous mutation will take

place (bit

set to

one)

or not

(bit

set to

zero) dunng

the life of the individual. We can consider the time as a discrete variable

running

from to B years.

Hence,

if at time t = i the i~~ bit in tl~e word

equals

one, it is considered tl~at tl~e individual will suffer tl~e effects of a deleterious mutation

in that year and all

following

years. The mutations are

hereditary

in tl~e sense

tl~at,

at tl~e birth of a new

individual, they

are transmitted to tl~is new individual except for M bits

(M

will be called mutation rate,

hereafter), randomiy

chosen. These mutations con

correspond

to either an additional deleterious mutation or a

cleaning

of a deleterious mutation

present

at the

parent's

genome. We can interpret this new mutation as a point mutation

(if

we are

considenng

asexual

reproduction)

or a recombination of the

parent's

genome in sexual

reproduction.

An individual will aie due to aging effects if the number of deleterious mutations tl~at were relevant up to its age is

equal

to a tl~resl~old T.

Competition

betiv-een tl~e individuals of a

population

for food and space, for

example

are introduced

taking

into accourt an

age-independent

Verhulst

factor,

wl~icl~

gives

to eacl~

individual a

probability

x =

il Ntot(t)/Nmax)

of

staying

alive.

Nmax

means tl~e maximum size of tl~e

population.

Eacl~

surviving

individual

generates,

at tl~e

reproduction

age R, b

offspnngs.

As stressed in reference

[9],

tl~e fact of individuals breed

only

once in their lifetimes

is tl~e fundamental

ingredient

to

explain

tl~e

catastropl~ic

senescence.

3.

Analytical

Calculations and Results

The relevant parameters in our calculations are:

. B

genotype lengtl~,

in

bits;

. 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~.

(4)

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

is

plausible

since

computer

simulations bave sl~own tl~at it al1&,ays

occurs).

Since tl~e age distribution and

tl~e

population

are

stationary,

we can consider tl~e Verl~ulst factor as constant. In tl~is

work,

for tl~e sake of

simplicity,

we assume

only

deleterious mutations at birtl~ witl~ T

=

1,

1-e-, tl~e effects of

just

one deleterious mutation is

enougl~

to cause tl~e deatl~ of an individual. Tl~e extension for different values of T is

straigl~tforward, altl~ougl~

we bave learned from

previous

computer

simulations results tl~at it is trot

important

for tl~e

catastropl~ic

senescence

exploration.

Let us consider one bas Jh~ individuals with zero age, after trie

stationary

state has been reacl~ed. The

probability

of a deleterious mutation to appear at a

given

age is

(tif/B), for

ages

beiow

R,

since in this case we con be sure that the

parent

bas no mutations up to age R

(T

=

1)

and tl~e mutations at birtl~ are

randomly

cl~osen

(we

are

considering

tl~e case AI «

B).

For ages

beyond R,

we must take into account the whole

parent's l~istory,

and tl~is will be clone later. First

ignoring birtl~s,

we con

expect

tl~at tl~e number of individuals witl~ age 1 will be

Ni =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~e

reproduction

of trie individuals at age R. Since eacl~ individuum

produces

b

offsprings,

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 above

equation,

witl~

tif

=

No,

one can obtain tl~e

stationary

state condition

x~ fl

~ ~ ~

= i

(5)

~i

~~~+~

As we sl~ould expect, tl~is condition does not

depend

on k but

only

on tl~e

global

parameters

R, M,

b and B. For M

= 1 it reduces to

bx~(B R)/B

= 1.

For ages k >

R,

we must

garantee

tl~at no mutation occurred between ages R and k. The

probability

that no mutation has occurred until age

k,

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~e

stationarity

condition

satisfied,

we must bave

Nk>R

" 0.

(7)

(5)

lî00 JOURNAL DE

PHYSIQUE

I N°12

o i

S

(6)

N°12 BIT-STRING MODEL FOR CATASTROPHIC SENESCENCE 1701

ioo

c

~ io

u

0 2 3 4 5

M

Fig.

2. Minimum birth rate bm~,, us. mutation rate IV. Trie solid fines

correspond

to

analytical

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)

and

20(o).

In trie computer simulations, we cari

only

obtain trie

maximum integer value below which trie

population

vanishes

(mutational meltdown).

That is

whj,

these results are belo~v the theoretical results. trie do not present results for

larger

values of b because it would reqmre a

huge

number of time steps until trie population vanishes.

that tl~e mutational meltdowii does Rot

depend

on trie size of

population

at least for asexual

semelparous

species in contrast witl~ earlier

biological assumptions

tl~at tl~is effect occurs

only

on small

populations.

~Îe present in

Figure

2 some curves for

b,n,n

as a function of Jf.

For

comparison,

we

present

some results from computer simulations. However, siiice we bave 1&>orked

only

with

integer

values of

b,

tl~e tl~eoretical results should be considered as an upper limit. For

large

values of b

(typically

>

10)

and l~igl~ mutation rates

(fil

>

3),

tl~e number of time

steps

needed to reacl~ tl~e

equilibrium

is very

large.

For a more

precise

determination of

bm,n,

we tried an

exponential fit,

for

Ntot

us. t

(for

10000 < t <

100000),

and we cl~ecked trie

sign

of tl~e exportent to determine wl~ether the

population

would

eventually

vaiiisl~. Since tl~e

study

of

dynamical aspects

of tl~is mortel are Dot into the scope of this work, we present

only

the more reliable results.

Trie relevant

quantities

in aging studies are tl~e survival rates

Sk,

1-e-, trie

probabilities

of an

individual to survive to the next age.

Tl~ey

cari be

easily

obtained front

equation (8):

~~ ÎÎÎI

~

B~ kÎÎ Î

B

~i ~MÎ1~

~~~

~~~~

Tl~e survival rate for age k

gives

tl~e

probability

that individuals alive at age k -1 survive

and reacl~ age k. In

Figure 3,

we compare tl~is expression for different values of b and R1&~itli computer simulation results. Tl~e

abrupt jump

to zero at k

= R is

clearly

seen.

(7)

lî02 JOURNAL DE

PHYSIQUE

I N°12

.-.-.-.-.-.-.-.-.-.-.-.-.-.-.-.-.-._._.

0.8 ~~~~~~~~~~

,

j~ce

~ Off lC

)

(

0.4

Ù7

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 sohd

bne),

R

= 20

(.

and dashed

hne)

and b

= 10, R

= II

(li

and dotted

fine).

We followed trie same strategy of averagmg as

adopted

in

Figure

1.

Again,

trie agreement between

theory

and computer

experiment is renlarkable.

4. Conclusions

Using simple

statistical arguments, we bave solved

analytically

tl~e

bit-string mortel,

for semel- parous

species

as tl~e Pacific salmon and

mayflies.

Dur results confirm tl~ose

presented

in reference

[9],

where it is claimed tl~at trie life

strategy

of

just

one

breeding attempt

leads to

catastl~rophic

senescence,

according

to tl~e mutation accumulation

tl~eory.

In

addition,

we can obtain an

analytical

expression for the

population

size of

semelparous

species as function of

mutation rate and

reproduction

age

(an exponential decay

for the same conditions of space and

food),

and tl~e minimum birtl~ rate to avoid mutational meltdown. Dur results also agree witl~ tl~ose found

by

Bernardes and

Stauffer, suggesting

tl~at trie mutational meltdown is not an effect of small

populations. Nevertl~eless,

we bave

found, by

computer

experiments,

tl~at tl~e time

required

for a

population

to vanisl~ con be very

large.

In this sense, we

suggest

tl~at it can be wortl~

studying

tl~e

dynamical aspects

of tl~e

bit-string mortel,

for botl~

semelparous

and

iteroparous

species.

As a final remark we wish to

point

out tl~at

altl~ough dealing

witl~

semelparous organisms,

tl~e extension for

iteroparous organisms (whicl~

breed

repeatedly)

is

straightforward,

but the

corresponding expressions

are too

lengtl~y

to be useful.

Acknowledgments

This work was motivated

by

a

question

raised

by

Naeem Jan about a

previous

paper. We

are

grateful

to hiin for bis interest in ouf work. Due of us

(TJPP)

is also

grateful

to Silvio Salinas and Nestor Caticl~a for

encouragement,

and tl~e otl~er

(SMO)

to P-M-C- de Oliveira for

important suggestions,

and to Hans J. Herrmann for bis

l~ospitality

at ESPCI wl~ere tl~is

work 1&,as concluded. Tl~is work is

partially supported by

Brazilian

agencies CNPq, CAPES,

FAPERJ and FINEP.

(8)

N°12 BIT-STRING MODEL FOR CATASTROPHIC SENESCENCE 1703

References

iii

Rose M.R., Trie

Evolutionary Biology

of

Aging (Oxford

Univ.

Press,

Oxford

1991).

[2] Charlesworth B., Evolution in

Age-structured

Populations, 2nd edition

(Cambridge

Univ. Press~

Cambridge 1994).

[3]

Partridge

L. and Barton

N-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

T.J.P.,

Moss de Oliveira S. and Stauffer

D., Phys.

Reu. E

(Rap.Comm.)(1995)

to appear.

[loi Lynch

M. and Gabriel

W.,

Evolution 44

(1990)

1725.

iii]

Bernardes A.T. and Stauffer D.,

(1995) submitted;

Bernardes

A.T.,

J.

Phys.

I France

(1995).

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