Abstract
A mathematical model for the purpose of analysing the dynamic of the populations of infected hosts anf infected mosquitoes when the populations of mosquitoes are periodic in time is here presented. By the computation of a parameter λ (the spectral radius of a certain monodromy matrix) one can state that either the infection peters out naturally) (λ≤ 1) or if λ > 1 the infection becomes endemic. The model generalizes previous models for malaria by considering the case of periodic coefficients; it is also a variation of that for gonorrhea. The main motivation for the consideration of this present model was the recent studies on mosquitoes at an experimental rice irrigation system, in the South-Eastern region of Brazil.
Malaria, epidemiology. Culicidae. Population dinamics. Ecology, vectors.
Resumo
Desenvolveu-se um modelo matemático para analisar a dinâmica das popu-lações de indivíduos e mosquitos infectados quando as popupopu-lações de mosqui-tos são periódicas no tempo. Pela determinação de um parâmetro λ (o raio espectral de uma matriz de monodromia) pode-se estabelecer que a infecção termina naturalmente (λ ≤ 1) ou se λ > 1 que a infecção torna-se endêmica. O modelo generaliza, para o caso de coeficientes periódicos, modelos anteriores para malária; como também é uma variação de modelo para a gonorréia. A principal motivação para a consideração do modelo proposto foram os recen-tes estudos sobre mosquitos numa estação experimental de arroz irrigado, na região Sudeste do Brasil.
Malária, epidemiologia. Culicidae. Dinâmica populacional. Ecologia de vetores.
Periodic dynamic systems for infected hosts
and mosquitoes
Sistemas dinâmicos periódicos para hospedeiros e mosquitos infectados
W. M. Oliva and E. M. Sallum
Departamento de Matemática Aplicada do Instituto Superior Técnico da Universidade Técnica de Lisboa. Portugal (W.M.O.), Instituto de Matemática e Estatística da Universidade de São Paulo. São Paulo, SP - Brasil (E.M.S.)
Correspondence to: Elvia Mureb Sallum - Departamento de Matemática Aplicada do Instituto de Matemática e Estatística da Universidade de São Paulo. R. do Matão, 1010. Cidade Universitária - 05508-900 São Paulo, SP - Brasil. Fax: (011) 814.4135 E-mail: [email protected]
INTRODUCTION
A model was constructed for the purpose of analysing the dynamic of the populations of infected hosts and infected mosquitoes, when the populations of mosquitoes are periodic in time. A deterministic estimator λ was established to predict whether the infection will peter out naturally (when λ ≤ 1) or, if λ > 1, the infection will become endemic (see Appendix). In the model, incubation and immunity are neglected.
The special case of one patch of hosts and two patches of mosquitoes are considered and the main results concerning the dynamics are given (see Theorems A and B). The estimator λ is the spectral radius of the monodromy matrix C, corresponding to the periodic matrix A(t) of the linear system associated with the complete system (1). It is a non trivial matter to compute the matrix C as also to discover its spectral radius λ.
The case of one patch of hosts and one (resp. two) patch(es) of mosquitoes is studied and it is assumed that the populations of mosquitoes behave according to periodic step functions. The monodromy matrix C is the product of exponentials of computable matrices; moreover, using suitable changes of coordinates, it was possible to obtain explicitly all the exponentials that appear in the expression of C, so that its spectral radius can be easily determined.
The general case (system (*)) that can be used for any number of patches of hosts and mosquitoes is presented in the Appendix.
The main motivation for the construction of the model here presented as well as the applications made was the recent studies by Forattini et al.4 on
mosquitoes at an experimental rice irrigation system5, 6, 7, 8, 9.
The constant and periodic coefficients that appear in the equations of the mathematical model should be determined experimentally. If they are available, reasonable predictions about possible mosquito-borne diseases that can appear at irrigation systems can be made.
ONE PATCH OF HOSTS AND TWO PATCHES OF MOSQUITOES
A deterministic model is here presented with a view to describing the dynamic of the population of hosts and mosquitoes infected by malaria when there is a homogeneous group of hosts with a constant population H and two groups of mosquitoes of
dS= − εS (H − S)
+ (b'1f1I1 + b'2f2I2)
dt S
dI1 b1f1S = − δ1I1 + (V1 − I1)
dt VI
dI2 b2f2S = − δ2I2 + (V2 − I2)
dt V2
dS (H − S)
= − εS + (b'1f1I1 + b'2f2I2)
dt H
dI1 b'1f1S = − δ1I1 + (V1 − I1)
dt H
dI2 b'2f2S = − δ2I2 + (V2 − I2)
dt H
different types i = 1, 2, with population Vi= Vi(t) periodic in the time t with periodic T > 0.
Let us considere the following system of ordinary differential equations:
where:
H : population of hosts;
Vi= Vi(t) = Vi(t + T) : population of mosquitoes at instant t, periodic of periodic T > 0;
S = S(t) : population of infected hosts at instant t; Ii= Ii(t) : population of infected mosquitoes of type i at instant t;
δ i : death rate of mosquitoes of type i; ξ: cure rate of sick hosts;
b’i : bites by one mosquito of type i on hosts per unit of time;
bi = bi(t) : bites by mosquitoes of type i taken on one person, per unit of time, which is a periodic function with period T > 0;
f ’iIi : population of infected mosquitoes of type i which are infective;
fiS : population of infected hosts which are infective.
Since bi(t)H = b’iVi(t), the system above can be written as:
(1)
where H, ξ, b’i, δi , fi are positive constants and Vi = Vi(t) are continuous periodic functions of period T > 0.
That system (1) corresponds to a generalization of the Ross model (Lotka12) and of that of
Dye-Hasibeder2, 3 for malaria. Moreover it is also a
variation of the Aronson-Mellander1 model that
describes the dynamics of gonorrhea.
This describes the dynamic of malaria when we have one group of mosquitoes with a periodic population V = V(t) interacting with a homogeneous group of individuals of a fixed population H. It will be shown that for V = V(t) periodic with period T = 12 (months) with V(t) = Vi positive and constant, i < t < (i + 1), i = 1, ..., 12, the eigenvalues of the fundamental solution of the associated linear system can be computed directly showing their dependence on the data of system (2) that is, on the parameters ξ, δ, H, b’, f and on V=V(t).
Let us write (2) in the following form
For each i = 1, ..., 12 one considers øi(t) = e , the fundamental solution of
(2)’
If we make U = − δS − b’fI, (2)’ becomes
(3)
Since Ai= MAiM−1, with M =
one obtains
(4) øi(1) = e = Me M−1.
Let ø(t) be the matricial solution of = A(t)
such that ø(0) = Id . Then one can write
ø(T) = ø12(1)ø11(1)ø10(1)...ø2(1)ø1(1)
(5) = Me e e ...e e M−1.
So from (2)’ we have
(6) S− (trace Ai)S + (det Ai)S = 0
and so, from (6)
(7) S(t) = αe + βe
where the are the real eigenvalues of A(i) = Ai, j = 1, 2, i = 1, ..., 12. From (3),
S = (trace Ai)S − U
Theorem A
Let (S(t), I1(t), I2(t)) be a non zero solution of (1) such that 0 ≤S(t0) ≤H, 0 ≤Ii(t0) ≤Vi(t0), i = 1, 2, and some t0≥ 0. Then 0 < S(t) < H, 0 < Ii(t) < Vi(t), i = 1, 2, for all t > t0.
We may write (1) in a matricial form
˙
y = A(t)y + N(t, y), y = (S, I1, I2), where
Let ø(t) be the matricial solution of ˙y = A(t)y such that ø(0) = Id. The monodromy matrix C = ø(T) is positive (Aronson, Mellander1, Lemma 2) and, by
Perron’s theorem (Gantmacher10), it has a simple
positive eigenvalue λ such that
λ = max{Reλi : det(C− λiId) = 0}.
Theorem B
There are two possibilities for the non zero solutions (S(t), I(t)) = (S(t), I1(t), I2(t)) of (1) such that for some t0≥ 0, 0 ≤S(t0) ≤H and 0 ≤Ii(t0) ≤Vi(t0), i = 1, 2: a) If λ ≤ 1 then (S(t), I(t)) tends to the zero solution
as t → ∞ ;
b) If λ > 1, then there exists a unique T -periodic solution (S*, I*) such that for any t > t0 we have 0 < S*(t) < H and 0 < I*i(t) < Vi(t), i = 1, 2. In this case (S(t) − S*(t), I(t) - I* (t)) tends to zero as t → ∞ .
In other words, Theorem B says that the infection peters out naturally when λ ≤ 1; or, if λ > 1, the infection becomes endemic if the initial number of infected cases in at least one group is positive.
As usual, it is a non trivial matter to obtain the matrix C = ø(T) and an expression for λ.
THE PERIODIC POPULATIONS OF MOSQUITOES AS STEP FUNCTIONS
One patch of hosts and one patch of mosquitoes
Let us consider the following system:
(2)
Ait
S S
= Ai where Ai = A(i)
I I
A
i
A
12 A11 A10 A2 A1
λi
1t λ
i
2t
λi
j
.
S S trace Ai − 1
= Ai , Ai= .
U U det Ai 0
A
i
1 0
δ 1
− −
b'f b'f
S I − ξ b'1f1 b'2f2
b'1f1V1
A(t) = − δ1 0 .
H b'2f2V2
0 − δ2 H
dS b'f I
= − ξS + (H − S)
dt H
dI b'f S
= − δI + (V(t) − I)
dt H
S S − ξ b'f
= A(t) + N(S, I) whereA(t) = .
I I b'f V(t)
− δ H
.
.
.
¨
..
.
.
S I
. .
For each i = 1, 2, ..., 12, one considers øi(t) = etA(i)
which is the fundamental solution of
(9)
If we make
(10) W = − δS − b'2f2I2
U = − 2δS − b'1f1I1 − b'2f2I2
system (9) becomes
S = TrA(i)S − U (11) U = [δ 2 + ∆
2A(i)]S + δU
(b'2f2)2
W = δξ + δ2− V
2 S + δU− δW
H
or
whereA(i) =
From (10) we see that A(i) = MA(i)M− 1 with M− 1 =
Let Φ(t) be the matricial solution of
such that I(0) = Id. Then, as above, one can write
(12) Φ(T) = Φ12(1)Φ11(1)...Φ2(1)Φ1(1)
= MeA(12)eA(11) ...eA(2)eA(1)M− 1.
Let us write the matrix A(i) of system (11) in the form
B(i) 0 A(i) =
* − δ
TrA(i) − 1
where B(i) = .
δ2+ ∆
2A(i) δ
so we have U = αλi
2e + βλ
i
1e and then
(8)
Finally we are able to obtain the eigenvalues of ø(T) that are those of the following matrix:
One Patch of Hosts and Two Patches of Mosquitoes
In this section we consider system (1) with δ1 = δ2 = δ and Vi=Vi (t) as a periodic step function, which is positive and constant during the month i, i = 1, 2, ..., 12, and periodic with period equal to T = 12 (months). We write
The three invariants (coefficients of the characteristic polynomium) of A(t) are:
det A(t) = − ξδ 2+δϕ(t)
TrA(t) = − ξ − 2δ (TrA(t) does not depend on t) ∆2A(t) = 2ξδ +δ 2− ϕ(t)
where
It is easy to check that (− δ ) is a eigenvalue of A(t), say λ3 = − δ . From the expressions of the invariants, the other two eigenvalues λ1 and λ2 satisfy.
λ1 + λ2 = − δ − ξ λ1λ2 = δξ − ϕ(t).
These two last equations imply that
Note that the three eigenvalues of A(t) are real and distinct; moreover, we have λ2 <− δ < λ1.
λi
1t λ
i
2t
1 λ2
12 − ie − λ
1
12 − ie e − e
λ2 12 − iλ
1 12 − i λ
1 12 − iλ
2
12 − i e − e λ
2
12 − ie − λ
1 12 − ie
λ2
12 − i λ 1 12 − i
11
Π
i=0 λ2
12 − i λ 1
12 − i λ 1
12 − i λ 2 12 − i
λ1 12 − i λ
2 12 − i
− ξ b'1f1 b'2f2 b'1f1
V1 − δ 0
A(t) = H .
b'2f2
V2 0 − δ
H
(b'1f1)2 (b' 2f2)
2
ϕ (t)= V1 + V2.
H H
(δ + ξ) 1
λj= − ± (δ − ξ)
2 +4ϕ (t), j = 1, 2.
2 2
S S
U = A(i) U
W W
TrA(i) − 1 0 δ2+ ∆
2A(i) δ 0 .
(b'2f2)2
δξ + δ 2 − V
2 δ − δ
H
1 0 0
− 2δ − b'1f1 − b'2f2 . − δ 0 − b'2f2
S S
I1 = A(t) I1 .
I2 I2
1 λi
2e − λ
i
1e e − e
e = λi
2 – λ
i
1 λ
i
1 λ
i
2 (e − e ) λ
i
2e − λ
i
1e
λi
2 λi1 λi1 λ
i 2
λi
2 λi2 λ
i 2 λi 1 Ai .
√
. . . . . . . . . S SI1 = A(i) I1
I2 I2
. .
For x = (x1, ..., xn) and y = (y1, ..., yn) we denote x ≤ y (x < y) if, for all i, xi ≤ yi ( xi < yi ). With the same arguments used in Aronson, Mellander1 one can state:
I) If y(t) and z(t) are non-zero solutions of (*) such that for some t0 ≥ 0 we have 0 ≤y(t0) ≤z(t0) ≤c(t0) with y(t0) ≠z(t0), then 0 < y(t) < z(t) < c(t) for all t > t0.
For fixed t0 ≥ 0 one considers the map f (y0) = y(t0 + T, t0, y0) for 0 ≤y0≤c(t0). When t0 = 0 we take the sequence of positive numbers c(0) = c0 > c1 > c2 > ... > cn > ... > 0, where cn = f0(cn- 1) and Q = lim cn≥ 0. When Q = 0 we have lim y(t, t0, y0) = 0 for 0 ≤y0≤c(t0). If Q≠ 0 we have y(t) = y(t, 0, Q) positive, periodic with period T > 0 and, by I), Q > 0.
Let Φ(t) the matrix solution of ˙y = A(t)y, Φ(0) = Id; since A(t) = (aij(t)) is irreducible with aij(t) ≥ 0 for i≠j, then the matrix C = Φ(T) is positive and so, by Perron's theorem, it has a simple positive eigenvalue λ = max{Reλi; det(C − λiId) = 0}.
As in theorem 1 of Aronson, Mellander1 one has
analogously:
II) If λ < 1, there exists K > 0 such that | y(t)| ≤ Kλ |y(t0)|for all t ≥t0 ≥ 0 and any solution y(t) = y(t, t0, y0) of (*) such that 0 ≤y0≤c(t0).
Consider now the case λ > 1. Let E(t0) = {y ∈ IRn : 0 ≤y≤c(t0)}, ω > 0 eigenvector of Ctcorresponding to λ, v(t0)t= ωtΦ(t
0)
− 1 and E
θ(t0) = {y ∈E(t0): v(t0)
t y ≥θ}. We claim that for θ > 0 sufficiently small we have f (Eθ(t0)) 傺Eθ(t0) where 0 ≤t0≤T. In fact
v(t0)tf
(y) = λv(t0)
ty + ϕ(t
0, y) where
ϕ(t0, y) = λwt
∫
Φ− 1 (s) N(s, y(s, t0, y))ds ; and
v(t0)tf
(y) − v(t0)
ty = (λ − 1)v(t
0)
ty + ϕ(t
0, y) ≥ (λ −
1)vty + ϕ(t
0, y), where 0 < v≤v(t0) for all t0 ∈ [0, T].
Since
is continuous on the compact set
{(t0, y) | t0∈ [0, T], y ∈E(t0)}, then there exist δ > 0 and N > 0 such that v(t0)tf
(y)
≥v(t0)ty + N | y | for t
0 ∈ [0, T] and | y | ≤ δ.
Using the Brower fixed point theorem (Hönig11) one
concludes that f has a fixed point in Eθ(t0). Then
eB(i) 0
eA(i)= ,
* e− δ
and also
eB(12)eB(11)...eB(1) 0
M− 1Φ(T)M= .
* e− 12δ
The eigenvalues of Φ(T) are e−Tδ together with the eigenvalues of eB(12)eB(11)...eB(1). So we only need
to compute eB(i) for i = 1, ..., 12. For that one has to
solve the system
or, equivalently, to solve the second order equation
(13) S− TrB(i)S + detB(i)S = 0.
Since the characteristic roots of (13) are the eigenvalues of B(i), that is,
δ + ξ 1
λi
j = λj(i) = − ± (δ − ξ)
2 + 4ϕ(i),
2 2
j = 1, 2, and i = 1, ..., 12, then, as we did in section 3.1, eB(i) is given by the second member of equality (8).
APPENDIX
Let us consider the following system
y1 = − α1y1 + (c1(t) − y1)(β11(t)y1 + β21(t)y2 + ...+ βn1(t)yn)
(*)
yn = − αnyn+ (cn(t) − yn)(β1n(t)y1 + β2n(t)y2 + ...+ βnn(t)yn)
which can be written as
y' = A(t)y + N(t, y) where
− α1 + c1β11 c1β21 ... c1βn1
A(t) = c2β12 − α2 + c2β22 ... c2βn2
c
nβ1n cnβ2n ... − αn+ cnβnn Assume αi to be positive constants; ci = ci(t) to be positive continuous periodic functions of period T > 0; βji = βji(t) to be non negative continuous periodic functions of period T > 0 such that A(t) is an irreducible matrix (Gantmacher10), for all t.
Moreover, assume there exists ε > 0 such that βji(t) ≥ ε for all t provided that βji(t) are not identically zero.
S S
= B(i)
U U
t0
n→∞
t→∞
t − t0 T
t0
t0
t
0
t + T
ϕ(t0, y)
if y ≠ 0 Φ(t0, y) = |y |
0 if y =0 t0
t0
t0 .
√
…
.
.
.
¨
.are bounded functions (see Aronson, Mellander1, Th. 2).
Given a compact set K傺 E(t0), one considers a point x0, 0 < x0 <c(t0), such that x0 < y(t0 + T, t0, y0)< c(t0) for all y0 ∈K. Since there are constants M(x0) > 0 and N > 0 such that for all y0 ∈K we have
|y(t, t0, y0) − y(t, t0, Q)|≤M(x0)e− a(t − ), t≥ t 0 + T
and
|y(t, t0, y0) − y(t, t0, Q)|≤N, t0≤ t≤ t0 + T, then one has the following result.
III) For λ > 1, system (*) admits a unique non zero periodic solution y(t, t0, Q), which has period T, and a constant a > 0 such that for each
compact set K 傺 E(t0) there corresponds a constant MK> 0 and we have
| y(t, t0, y0) − y(t, t0, Q) |≤Mke− a(t − ) for all t≥ t 0 ≥0.
Moreover, as in theorem 3 of Aronson, Mellander1
we state:
IV) For λ = 1 there is a constant L > 0 such that for any solution y(t, t0, y0) = y(t) of (*) with 0 ≤y0 ≤ c(t0), t0 ≥0, we have
| y(t) |≤ provided t ≥ t0. For any two solutions y(t) = y(t, t0, y0) and z(t) =
y(t, t0, z0) of (*) such that 0 < y0, z0 < c(t0),one has
D+u(t) ≤− (u− 1) min(ψ
z, ψy) < 0 for t ≥ t0 ≥ 0
where u(t) = max {max { , }} and ψ(y) = k
(see Aronson and Mellander1; Lemma 5, [1]).
So, one can conclude that for θ > 0 sufficiently small, f : Eθ(t0) →Eθ(t0) has only one fixed point Q, and then f : E(t0) →E(t0) has only one fixed point Q > 0, besides the origin, that corresponds to a periodic orbit of period T > 0 for system (*).
For y(t) = y(t, t0, y0) with 0 ≤y0 ≤c(t0) and z(t) = y(t, t0, Q) we have
u(t) − 1 ≤eu( )(u(t 0) − 1)e
− p(t)e− a(t − )
where a = ψz(t)dt and p is continuous and T
-periodic, T > 0. So, for each x0 > 0 sufficiently close to the origin, there exists a constant M(x0) > 0 such that
|y(t, t0, y0) − y(t, t0, Q)| ≤ M(x0)e− a(t − )
for all y0, x0 ≤ y0 ≤c(t0) and all t ≥ t0 ≥ 0 because the ck(t) yk zk
zk yk
j = 1 n
min ∑ βjm(t)yj(t)
1 ≤m ≤ n
t0
t0
t0
T
∫
1 T
0
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t0 t0
K
1 + (t − t0)