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Submitted on 1 Jan 1991

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On a discrete approach to cell dynamics in context to immune response against HIV

R. Pandey

To cite this version:

R. Pandey. On a discrete approach to cell dynamics in context to immune response against HIV. Jour-

nal de Physique I, EDP Sciences, 1991, 1 (12), pp.1709-1713. �10.1051/jp1:1991228�. �jpa-00246448�

(2)

Classification

Physics

Abstracts

05.50 87.10

On

a

discrete approach to cell dynamics in context to immune response against HIV

R. B.

Pandey

Department

of

Physics

and Astronomy,

University

of Southem

Mississippi, Hattiesburg,

MS 39406-5046, U-S-A-

(Received

23 August 1991,

accepted

in

final form

2

September 1991)

Abstract. A network model of

interacting

cellular elements, such as

macrophages,

viruses, T4 cells, and T8 cells, is introduced to

study

the evolution of cell

population

in an

early

HIV infection in a cell mediated response. The mean field treatment leads to two fixed

points (describing

«

immunocompetence

» and «

immunodeficiency

») and a limit

cycle

in infected states of

period

two.

Using

a cellular automata rule for the nearest

neighbour

interaction, the

growth

of the cellular

population

is studied as a function of their initial concentration p; on

increasing

p, a crossover from an inununodeficient to an

immunocompetent

state occurs at a characteristic

value p~.

A considerable interest has been

recently

directed towards

studying

the immune response via theoretical models

[1-13].

In a

typical

immune response, the

antigen presenting

cells

(APC)

such as

macrophages,

dendritic

cells,

and B-cells

engulf

the invader

(the antigen),

process

it,

and return it to the cell membrane. As soon as the «

helper (T4) lymphocytes recognize

the

antigens

on the membranes' surface

they (T4 cells) begin

to

proliferate

with activated T4 cells

releasing

chemical

signals,

the

lymphokines (especially IL2).

With the presence of

IL2,

the T4

lymphocytes

not

only multiply themselves,

but also induce

specific cytotoxic (T8) lymphocytes

to

proliferate.

As

such,

isolated T4 cells are blind to free

antigens.

Suppressor

T8 cells inhibit the

production

of

lymphokines by

T4 cells in order to switch off the response. In AIDS

[14],

HIV viruses have an

ability

to escape such cell mediated attack

(as

well as humoral

aspect involving specific antibodies).

Conforrnational

complementarity

of the viral

protein (gp120)

and the surface receptor

(CD4)

of T4 cells

help

in fusion of the viral membrane with the T4 cell

leading

to release of viral cores into the interior of the T4 cell.

Production of new virus from infected cells results in death of the infected T4 cells. A discrete

approach

is used here to model the

growth

of the cellular

population

in this context. We would like to

point

out

that,

there have been numerous theoretical studies

by

a

variety

of models in recent years

[2, 9, 12, 15-17] although

with very little success in

understanding

the clinical

findings thoroughly

and

therefore,

apart from a new theoretical

study (see below),

one should not expect a

breakthrough

in this article either.

To describe the state of a

cell,

we

employ

a

simplified binary representation

that has been used

frequently

in recent years

[6-13]

in

modeling

the immune response where

logical

(3)

1710 JOURNAL DE

PHYSIQUE

I M 12

expressions [18]

are used to construct interactions among cellular elements. The

binary values,

0 » false

»)

and « I » true

»)

of a cell

type represent

the states in which the cell is in its low and

high

concentrations. Here, we consider

only

four cell types

macrophages (M),

virus or viral infected cells

(V),

T4

cells,

and T8 cells.

First,

we consider the « mean field » like interaction where the concentration of each cell

type

is described

by

one value for the whole

system.

In a cell mediated response, we

attempt

to

incorporate

some of the main functions of cellular elements in which

macrophages (M) display antigenic component

of virus to the T4 cell ; cells

bearing

CD4

proteins (which

includes both T4 cells as well as

macrophages)

attract HIVS. T4 cells are killed

by

viruses whereas most

macrophages

are not, rather,

they provide

shelter to these viruses and act as a reservoir in a HIV infection. In coordination with T4

cells,

the T8 cells

proliferate

as

they

receive

lymphokine signals

from T4 cells and kill the viral infected cells. In our earlier

study [9],

the role of APCS was

completely ignored

inclusion of some of their functions not

only provides

a more realistic model but also

brings interesting

results. We propose a

following

set of intercell interactions :

M(t

+ I

=

M(t)

or V

(t)

V(t

+

Ii

=

(V(t)

or

(M(t)

or T4

(t))j

and

(not (T8 (iii j T4(t

+

Ii

=

(M(tj

or

T4(tjj

and

(not (V(tjjj

T8(t

+

Ii

=

T4(tj

and

(M(tj

and V

(iii

where the

growth

states of the four cell

types

at time

step

t + I are evolved from their

growth

states at

previous

time step t. The first

equation

describes the

growth

of activated

macrophage population

which will be in a

high

concentration state at time

step

t + I

(I.e. M(t

+ I

=

Ii

if

it was

already

in this state

(M(t)

=

I)

at time

step

t

(I.e.

the

macrophages

are self-

propagating)

or if a viral infected cell was present

(V (ii

=

I

),

or both are present in their

high

concentration state the presence of a virus activates

macrophages.

The second

equation represents

the virus

multiplication

in which the viruses grow

only

if the

cytotoxic

T8 cells are absent

(T8(t)

=

0) and,

in

addition,

at least one of the

remaining

cells

including

the virus itself is present at its

previous

time step. Note that

high

concentrations of T4 cells and

macrophages

enhance the viral

growth.

Proliferation of T4 cells is

accomplished

via the third

equation,

in which the virus must be absent

(V (11

=

0) and,

in

addition,

either

macrophage (along

with MHC

III

or T4 cells or both be present in their

high

concentration state at time

step

t, in order to

produce

T4 cells at time

step

t + I.

Finally,

the fourth

equation gives

the

growth

of

cytotoxic

T8 cells which are activated

by

T4 cells in order to kill viral infected cells

presented by macrophages.

Thus a T8 cell will

multiply (I.e. T8(t

+ I

)

=

Ii

if all other cell

types

(I.e.

T4

cells, macrophages,

and

viruses)

are

present

at

previous

time

step

t.

The overall immune-status is described

by

the

configuration

of the four

binary

cells. There

are sixteen

possible

such

configurations

but not all of them are stable. Let us

represent

the

configuration

of these cells in a

binary representation (M, V, T4, T8).

If we start with any of these sixteen

configurations randomly

we either end up in two fixed

points, (o000)

and

(1100),

or

get trapped

in a triad

cycle

of

configurations, (1000) (1l10) (l101).

In the first stable

immunological configuration,

0

=

(oooo),

since there is no

stimulatory

cell

present,

we call this a

«fully immunocompetent»

state which is also referred as the

« native » or «

unchallenged

state. This does not mean that there are no cells in the

body,

it

simply implies

that cells that were stimulated to grow

during

the immune response are no

longer

activated. On the other

hand,

in the second stable

configuration

12

=

(l100), only

macrophages

and viruses are present, where the

macrophages (in

the absence of other

(4)

stimulatory cells)

act as reservoir for HIV.

Therefore,

we call this fixed

point

the

fully

immunodeficient » state. We

interpret

the triad

cycle configurations

as follows : in

configur-

ation 14

=

II10)

all cells are present except

cytotoxic

T8 cells and therefore we call it an

« infected » state because the presence of

macrophages

and T4 cells may stimulate other cell types

including

T8 cells. The

configuration

13

=

(1101)

represents the state in which all cells

are present except T4 cells which orchestrate the functions of other cells in immune response, and therefore we call this

configuration

a «

severely

infected » state. On the other

hand,

in

configuration

8

=

(1000)

all cells are absent

except macrophages

and we call it a « suscept,

ible » state. Note that the

competition

between the viral attack and immune defense cells

leads to this limit

cycle

in which the immune system oscillates in a triad

cycle

of « infected »,

«

severely

infected », and «

susceptible

» states

periodically.

Opposite

to the infinite range interaction

just discussed,

now we consider the nearest

neighbour

intracellular interaction

[9]

with a

spatial

distribution

[19]

of cell

types.

For

simplicity,

we restrict ourselves here to a

simple

cubic lattice as a host medium.

First,

we

generate

a

simple

cubic lattice of size L*L*L and then we

place

four cell types at each lattice site.

However, only

a small fraction

p(I)

of these cell

types I(=

I

(Ml,

2

(V),

3

(T4),

4

(T8 ii

is

assigned

the

high

concentration state « I » while the rest, a fraction I

p(I)

of

cells,

is

assigned

the low concentration state «0». The

binary

states «0»

(empty)

and «I

(occupied)

of a cell type I at a site may also later

specify

the occupancy status of the site

by

cell

type

I.

Thus,

a lattice site can be either

empty

or

occupied by

each of the four cell

types

and the number of sites

initially occupied by

a cell type I is

N,

= p

(I)*

N where N is the total

number of lattice sites. Here we

study

how

N~

grows with time and how it

depends

on

interaction and other parameters relevant to immune

system.

In addition to the above basic intercell

interactions,

we consider an intersite intracell interaction as follows. A cell

type

I is selected at a

site,

say

j.

The

binary

state of this

cell,

say

c~(t),

at current time step t is then added to the

binary

states of the same cell type I at the

neighboring

six sites. If this sum of seven

binary

states is

positive,

then a temporary

binary

state

c;(tl'

of

high

concentration (« I

»)

is

assigned

to the cell type I at the site

j,

otherwise

(I.e.

if the sum is

zero)

the temporary

binary

state of cell type I at site

j

remains in its low concentration state (« 0

»),

In other

words, c,(tl'

is the result of

logical

« or »

operation ii

5] of the seven lattice sites involved. The same

procedure

is used to

assign temporary binary

states to all other cell

types

at site

j.

With their

temporary binary

states, c,

(ii',

the four cells at this site

j

then interact

according

to intercell interaction discussed

above the

resulting

states are then

assigned

as states at time step t + I. This process of

selecting

a

site, evaluating

the intermediate cellular states

by taking

into account the intersite

intracell interactions for all cell types at this

site,

and then

assigning

final

binary

states to each cell

emerging

from the intercell interaction at the next time step is

repeated again

and

again

for each cell

type

at all lattice sites for a number of time

steps

in which the

growth

and

decay

of each cell type reaches their

steady

state value, To obtain a reliable estimate of the

steady

state

populations

of each cell types, we use several

independent

runs.

The computer simulation is

performed

on a

Cray

XMP and YMP machine where a

multispin

code

[15]

is used for

storing

the lattice sites. The status of a lattice site where a cell

type

is in its

high

I

»)

or low 0

»)

concentration state is described

by

a

single

bit of a 64- bit word

using

« yes » and no »

logic description. Samples

of two different

sizes,

64*64*64

and

192*192*192,

are used to generate data for the

population

of each cell type, in which 5

independent samples

are used to find their average values. The maximum

speed

was found to be about 152

steps

per site per microsecond per YMP processor and was about 33

percent

slower on the XMP.

On a 64*64*64

lattice,

the lowest

possible

initial concentration of a cell

type

I is

(5)

1712 JOURNAL DE

PHYSIQUE

I M 12

p(I )

= 0.000005 in which

only

one site is

occupied by

a cell type I. With the nearest

neighbor

interaction

(of

the cellular

automata)

rule described

above,

intercell interaction leads to a

steady

state in which the number of

macrophages

and T8 cells

approach

a maximum value

(typically

the size of the

sample,

I-e- all sites are

occupied by

at least these two cell

types)

the number of viral infected cells

(virions)

and T4 cells oscillate about their mean values say

N~

and

NT4.

A

typical

variation of the

population growth

of

virus,

T4 cells and T8 cells with

equal

initial concentration for all cells

except

that of virus which started at one site

only,

is

shown in

figure

I. We observe

that,

the

steady

state

population

of virus is

larger

than that of the T4

cells,

if the initial concentration of defensive host cells

(T4 cells,

T8 cells and

macrophages)

is lower than a characteristic value

P~(I)

above which the

steady

state

population

of T4 cells is

larger

than that of the virus. This exhibits a crossover from an

«immunodeficient» state to an

«imrnunocompetent»

state at

p~(I).

The

population

of

macrophages

remains constant at its maximum value

(I.e.

the size of the

sample)

and that of

the T8 cells also remains constant but at a lower value

depending

upon its initial

concentration. The relaxation time to

approach

the

steady

state

population depends

upon the initial concentration of host cells in which the lower the

concentration,

the

longer

the time it takes to reach the

steady

state. Note the difference in results from the mean field treatment of the

preceding

section. Instead of two stable fixed

points

and an

oscillatory

state with the infinite range

interaction,

here in the n-n-

interacting model,

we observe

only

two states

(I.e.

« imrnunodeficient » and «

immunocompetent »)

which

depend

upon the initial concentration

O.75 t/l

d

m CJ

>

~ O.5

d

z o CJ

O.25

O

O-05 O.06 O.09 O-12 O-15

P

Fig.

I- Concentration of viruses

((+)

maximum,

(*) minimum),

and T4 cells

((O)

maximum,

(x) minimurn)

with respect to the

population

of T8 cells

(*,

on the

top) (I.e.

the concentration of virus

=

number of viral infected

cells/number

of T8

cells)

versus initial concentration of host cells

(T4

cells, T8 cells and

macrophages).

A 64*64*64

sample

with 5

independent

runs is used to evaluate the

steady

state

populations of the four cell type ; number of macrophages reach their maximum value (I.e. the size of the

sample).

(6)

of the cell

types suggesting

that this

spatial approach

is more

appropriate

than the mean field

approach. Thus,

the

simple

model

presented

here does capture some of the essential features of the HIV

infection, especially

the decline of T4 cell

populations.

We

hope

to

incorporate

more realistic factors in our continued efforts to understand

complex

issues in immune response in HIV infection.

The author would like to thank Dietrich Stauffer for discussion and valuable

suggestions.

The financial

support

and

computer

time

provided by

HLRZ

during

a summer visit to HLRZ Juelich where this work was done

partial support

from a Research

Corporation

grant

(#

C-

2903)

is also

acknowledged.

References

ill

ATLAN H., Bull. Math. Biol, sl

(1989)

247.

[2] «Theoretical

Inununology

», Part One and Two, Ed. A. S. Perelson

(Addison-Wesley, 1988).

[3] COOPER L. N., Proc. Natl. Acad. Sci. 83

(1986)

9159.

[4] BEHN U. and VAN HEMMEN J. L., J. Stat.

Phys.

s6

(1989)

533.

[5] KURTEN K., J. Stat.

Phys.

s2

(1988)

503.

[6] KAUFMAN M., URBAIN J. and THOMAS R., J. Theor. Biol. l14

(1985)

527.

[7] WEISBUCH G. and ATLAN H., J.

Phys.

A 21

(1988)

L-189.

[8] DAYAN I., STAUFFER D. and HAVLIN S., J.

Phys.

A 21

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2473.

[9] PANDEV R. B, and STAUFFER D., J.

Phys.

France s0

(1989)

1;

PANDEY R. B., J. Stat. Phys. 54

(1989)

997.

[10]

NEUMANN A. U., Physica A 162

(1989)

1.

ii Ii CHOWDHURY D. and STAUFFER D., J. Stat. Phys. s9

(1990)

1019.

[12] PANDEY R. B. and STAUFFER D., J. Stat.

Phys.

61

(1990)

235.

[13] KOUGIAS C. F. and SCHULTE J., J. Stat.

Phys.

60

(1990)

263.

[14]

Sci. Am.

(special issue)

2s9

(1988)

; for recent

developments

see, LAYNE S. P. et al., J.

Virology

6s

(1991)

3293

REDFIELD R. R. et al., N.

Engl.

J. Med. 324

(1991)

1677 ; KONTIO S., J. Immunological Meth. 139

(1991)

257.

[15]

MCLEAN A. R. and KIRKWOOD T. B. L., J. Theor. Biol. 147

(1990)

177.

ii 6] SIEBURG H. B., MCCUTCHAN J. A., CLAY O. K., CABALERRO L. and OSTLUND J. J.,

Physica

D 4s

(1990)

208.

[17] NELSON G. W. and PERELSON A. S.,

preprint (1991).

[18] STAUFFER D., J.

Phys.

A 24

(1991)

909.

[19] PERELSON A. S. and WEISBUCH G.,

preprint (1991).

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