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Mathematical modelling of mosquito dispersal in a heterogeneous environment Angelina Mageni Lutambi a,b,c,, Melissa A. Penny a,b , Thomas Smith a,b , Nakul Chitnis a,b a Swiss Tropical and Public Health Institute, Socinstrasse 57, P.O. Box CH-4002 Basel, Switzerland b University of Basel, Petersplatz 1, CH-4003 Basel, Switzerland c Ifakara Health Institute (IHI), Plot 463, Kiko Avenue, Old Bagamoyo Road, Mikocheni P.O. Box 78373, Dar es Salaam, Tanzania article info Article history: Received 6 January 2012 Received in revised form 21 November 2012 Accepted 26 November 2012 Available online 13 December 2012 Keywords: Mathematical model Mosquito dispersal Simulation Discrete space Repellents Dispersal distance abstract Mosquito dispersal is a key behavioural factor that affects the persistence and resurgence of several vec- tor-borne diseases. Spatial heterogeneity of mosquito resources, such as hosts and breeding sites, affects mosquito dispersal behaviour and consequently affects mosquito population structures, human exposure to vectors, and the ability to control disease transmission. In this paper, we develop and simulate a dis- crete-space continuous-time mathematical model to investigate the impact of dispersal and heteroge- neous distribution of resources on the distribution and dynamics of mosquito populations. We build an ordinary differential equation model of the mosquito life cycle and replicate it across a hexagonal grid (multi-patch system) that represents two-dimensional space. We use the model to estimate mosquito dispersal distances and to evaluate the effect of spatial repellents as a vector control strategy. We find evidence of association between heterogeneity, dispersal, spatial distribution of resources, and mosquito population dynamics. Random distribution of repellents reduces the distance moved by mosquitoes, offering a promising strategy for disease control. Ó 2012 Elsevier Inc. All rights reserved. 1. Introduction Mosquitoes transmit malaria, dengue, yellow fever, filariasis, and several other important diseases. Malaria, in particular, shows considerable spatial variation predominantly determined by cli- matic variation [25], intervention coverage, and human movement [39,55,60,62]. At local scales (i.e. from 100 m to 1 km), mosquito behaviour and ecology play an important role in determining the distribution of transmission [34]. Like other animals, mosquitoes can move in any direction, motivated by resource availability and other drivers of dispersal, but can only travel over limited dis- tances. Control interventions should consider locality and mosqui- toes’ ability to move, to achieve a high level of effectiveness in reducing the mosquito population. The impact of vector dispersal in the spread and control of dis- eases was first highlighted a century ago by Ronald Ross [53], but has received limited attention within the public health commu- nity. Ross stipulated that mosquito density within any area is al- ways a function of four variables, which include the reproduction rate, mortality rate, immigration, and emigration rates. A study by Manga et al. [38] also showed that the spatial variation in the distribution of resources used by mosquitoes affects their repro- duction and their rate of dispersal. This in turn contributes to var- iation in densities [10,24,37,58], human exposure to vectors, and the ability to control disease transmission [55]. The effects of re- source availability on transmission can be surprising. For instance, even the presence of non-productive larval habitats may affect bit- ing densities [34]. However, conducting experimental studies of mosquito dispersal [21–23,42] are challenging. Mathematical models play an important role in understanding and providing solutions to phenomena which are difficult to mea- sure in the field, but few models have incorporated dispersal or heterogeneity when modelling resource availability [17,34, 46,49,58,68] or varied the usual assumption of a closed vector pop- ulation [45,50,67]. Others have sub-divided the adult stage of the mosquitoes into different stages [45,50,54]. To investigate the ef- fects of dispersal and heterogeneity, a model should incorporate features of the mosquito life cycle, the feeding cycle, spatial heter- ogeneity in mosquito resources, and dispersal. Spatial models have commonly used the diffusion approach, which considers space as a continuous variable. Despite the exis- tence of diffusion models, which account for heterogeneity [51,63], it is difficult to explicitly incorporate the various factors that affect movement. For example, in areas where resources are located in patches or discrete locations, mosquito dispersal is more conveniently modelled using a metapopulation approach, in which the population is divided into discrete patches. In each patch, the 0025-5564/$ - see front matter Ó 2012 Elsevier Inc. All rights reserved. http://dx.doi.org/10.1016/j.mbs.2012.11.013 Corresponding author at: Swiss Tropical and Public Health Institute, Socinst- rasse 57, P.O. Box CH-4002 Basel, Switzerland. Tel.: +41 612848273; fax: +41 612848101. E-mail addresses: [email protected] (A.M. Lutambi), melissa. [email protected] (M.A. Penny), [email protected] (T. Smith), Nakul. [email protected] (N. Chitnis). Mathematical Biosciences 241 (2013) 198–216 Contents lists available at SciVerse ScienceDirect Mathematical Biosciences journal homepage: www.elsevier.com/locate/mbs
Transcript

Mathematical Biosciences 241 (2013) 198–216

Contents lists available at SciVerse ScienceDirect

Mathematical Biosciences

journal homepage: www.elsevier .com/locate /mbs

Mathematical modelling of mosquito dispersal in a heterogeneous environment

Angelina Mageni Lutambi a,b,c,⇑, Melissa A. Penny a,b, Thomas Smith a,b, Nakul Chitnis a,b

a Swiss Tropical and Public Health Institute, Socinstrasse 57, P.O. Box CH-4002 Basel, Switzerlandb University of Basel, Petersplatz 1, CH-4003 Basel, Switzerlandc Ifakara Health Institute (IHI), Plot 463, Kiko Avenue, Old Bagamoyo Road, Mikocheni P.O. Box 78373, Dar es Salaam, Tanzania

a r t i c l e i n f o a b s t r a c t

Article history:Received 6 January 2012Received in revised form 21 November 2012Accepted 26 November 2012Available online 13 December 2012

Keywords:Mathematical modelMosquito dispersalSimulationDiscrete spaceRepellentsDispersal distance

0025-5564/$ - see front matter � 2012 Elsevier Inc. Ahttp://dx.doi.org/10.1016/j.mbs.2012.11.013

⇑ Corresponding author at: Swiss Tropical and Pubrasse 57, P.O. Box CH-4002 Basel, Switzerland. Tel612848101.

E-mail addresses: [email protected]@unibas.ch (M.A. Penny), thomas-a.smith@[email protected] (N. Chitnis).

Mosquito dispersal is a key behavioural factor that affects the persistence and resurgence of several vec-tor-borne diseases. Spatial heterogeneity of mosquito resources, such as hosts and breeding sites, affectsmosquito dispersal behaviour and consequently affects mosquito population structures, human exposureto vectors, and the ability to control disease transmission. In this paper, we develop and simulate a dis-crete-space continuous-time mathematical model to investigate the impact of dispersal and heteroge-neous distribution of resources on the distribution and dynamics of mosquito populations. We buildan ordinary differential equation model of the mosquito life cycle and replicate it across a hexagonal grid(multi-patch system) that represents two-dimensional space. We use the model to estimate mosquitodispersal distances and to evaluate the effect of spatial repellents as a vector control strategy. We findevidence of association between heterogeneity, dispersal, spatial distribution of resources, and mosquitopopulation dynamics. Random distribution of repellents reduces the distance moved by mosquitoes,offering a promising strategy for disease control.

� 2012 Elsevier Inc. All rights reserved.

1. Introduction

Mosquitoes transmit malaria, dengue, yellow fever, filariasis,and several other important diseases. Malaria, in particular, showsconsiderable spatial variation predominantly determined by cli-matic variation [25], intervention coverage, and human movement[39,55,60,62]. At local scales (i.e. from 100 m to 1 km), mosquitobehaviour and ecology play an important role in determining thedistribution of transmission [34]. Like other animals, mosquitoescan move in any direction, motivated by resource availability andother drivers of dispersal, but can only travel over limited dis-tances. Control interventions should consider locality and mosqui-toes’ ability to move, to achieve a high level of effectiveness inreducing the mosquito population.

The impact of vector dispersal in the spread and control of dis-eases was first highlighted a century ago by Ronald Ross [53], buthas received limited attention within the public health commu-nity. Ross stipulated that mosquito density within any area is al-ways a function of four variables, which include the reproductionrate, mortality rate, immigration, and emigration rates. A study

ll rights reserved.

lic Health Institute, Socinst-.: +41 612848273; fax: +41

(A.M. Lutambi), melissa.nibas.ch (T. Smith), Nakul.

by Manga et al. [38] also showed that the spatial variation in thedistribution of resources used by mosquitoes affects their repro-duction and their rate of dispersal. This in turn contributes to var-iation in densities [10,24,37,58], human exposure to vectors, andthe ability to control disease transmission [55]. The effects of re-source availability on transmission can be surprising. For instance,even the presence of non-productive larval habitats may affect bit-ing densities [34]. However, conducting experimental studies ofmosquito dispersal [21–23,42] are challenging.

Mathematical models play an important role in understandingand providing solutions to phenomena which are difficult to mea-sure in the field, but few models have incorporated dispersal orheterogeneity when modelling resource availability [17,34,46,49,58,68] or varied the usual assumption of a closed vector pop-ulation [45,50,67]. Others have sub-divided the adult stage of themosquitoes into different stages [45,50,54]. To investigate the ef-fects of dispersal and heterogeneity, a model should incorporatefeatures of the mosquito life cycle, the feeding cycle, spatial heter-ogeneity in mosquito resources, and dispersal.

Spatial models have commonly used the diffusion approach,which considers space as a continuous variable. Despite the exis-tence of diffusion models, which account for heterogeneity[51,63], it is difficult to explicitly incorporate the various factorsthat affect movement. For example, in areas where resources arelocated in patches or discrete locations, mosquito dispersal is moreconveniently modelled using a metapopulation approach, in whichthe population is divided into discrete patches. In each patch, the

A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 199

population is sub-divided into subgroups, corresponding to differ-ent states, leading to a multi-patch, multi-compartment system.

Several models using diffusion approaches [18,19] have incor-porated heterogeneity and have shown that the environment hasa strong influence on the distribution of disease vectors. However,none of them have included the aquatic stages of the mosquitoesor have provided a general and simple framework for modellingarbitrary spatial patterns of mosquito control interventions. Amodel framework that includes the aquatic stages and that parti-tions space into discrete locations allows us to capture the variousforms of spatial heterogeneity that exist in our environment.

In this paper, a mathematical model, that includes all of theabove features is developed and simulated to investigate the im-pact of dispersal and heterogeneous distribution of mosquito re-sources, such as hosts and breeding sites, on the spatialdistribution, dynamics, and persistence of mosquito populations.The distance a mosquito can travel from its place of emergenceor food source is a critical factor for vector control interventions,thus the model is used to project likely dispersal distances andconsiders how these might be changed by vector controlinterventions.

In the following sections, we develop and analyse a model formosquito population dynamics that does not consider movementof mosquitoes. We then develop a meta-population model for mos-quito movements with discrete space in hexagonal patches andcompare it to a continuous space model. We then combine thetwo models and run simulations of a spatially explicit model ofthe full mosquito life cycle to determine the effect of repellents.

2. Description of the basic model: mosquito dynamics withoutdispersal

Mosquito life begins with eggs, which hatch into larvae undersuitable conditions. The larvae develop into pupae that matureand emerge into adults (see Fig. 1). Female mosquitoes then feedon human or animal blood to provide protein for their eggs. Afterbiting, female mosquitoes rest while their eggs develop. Once eggsare fully developed, the females oviposit and then proceed to findanother blood meal thus completing the mosquito feeding cycle[12].

Ignoring the effects of hibernation and breaks in the reproduc-tive cycle, and assuming that eggs deposited at breeding sites pro-ceed through development immediately [56], we consider sixcompartments of the mosquito life cycle: eggs (E), larval (L), pupal

Fig. 1. Schematic representation of Anopheles mosquito life cycle and feeding cycle.Model states are Eggs (E), Larvae (L), Pupae (P), host seeking adults (Ah), restingadults (Ar), and oviposition site searching adults (Ao).

(P), host seeking adults (Ah), resting adults (Ar), and oviposition siteseeking adults (Ao) (Fig. 1). In contrast to other models [36], we dis-tinguish all of these stages because interventions may be applied toany one (or more) of them. Since only female mosquitoes are in-volved in the transmission of vector-borne diseases, this modelignores males. The six subgroups have different mortality and pro-gression rates. Each subgroup is affected by three processes: in-crease due to recruitment, decrease due to mortality, anddevelopment or progression of survivors into the next state. Theparameter b is the average number of female eggs laid during anoviposition and qAo

(day�1) is the rate at which new eggs are ovi-posited (i.e. reproduction rate). Exit from the egg stage is eitherdue to mortality, lE (day�1), or hatching into larvae, qE (day�1).In the larval stage, individuals exit by death or progress to pupalstage at a rate, qL (day�1). Assuming a stable environment, inter-competition for food and other resources for larvae may occur,leading to density-dependent mortality, lL2

L2 (day�1 mosqui-toes�1) or natural death at an intrinsic rate, lL1

(day�1). Pupaedie at a rate, lP (day�1) and survivors progress and emerge asadults at rate qP (day�1). In the adult stage, host seeking mosqui-toes die at a rate lAh

(day�1). Those surviving this stage, and if theyare successful in feeding, enter the resting stage at a rate qAh

(day�1). In the resting stage, mosquitoes die at a rate, lAr(day�1).

Survivors progress to the oviposition site searching stage at a rateqAr

(day�1). Oviposition site searchers die at rate lAo(day�1) and

after laying eggs return to the host seeking stage. These processesaccount for the dynamics of each subgroup over time. Althoughmosquitoes might require more than one blood meal to produceeggs [5], this model assumes the simple case where only one bloodmeal is enough for eggs to mature. Throughout this work, we usethe words oviposition sites and breeding sites interchangeably.

From the description above, we develop the following system ofdifferential equations to describe mosquito dynamics withoutmovement:

dEdt¼ bqAo

Ao � lE þ qE

� �E;

dLdt¼ qEE� lL1

þ lL2Lþ qL

� �L;

dPdt¼ qLL� lP þ qP

� �P; ð1Þ

dAh

dt¼ qPP þ qAo

Ao � lAhþ qAh

� �Ah;

dAr

dt¼ qAh

Ah � lArþ qAr

� �Ar ;

dAo

dt¼ qAr

Ar � lAoþ qAo

� �Ao;

with initial conditions Eð0Þ; Lð0Þ; Pð0Þ;Ahð0Þ;Arð0Þ, and Aoð0Þ. Mos-quito survival in each stage and the progression period from onestage to the next are assumed to be exponentially distributed. Thedefinitions of state variables and the associated parameters are gi-ven in Tables 1 and 2, respectively.

Since the system in Eq. (1) monitors populations in each stage ofmosquito development and because all model parameters (Table 2)are positive, there exists a region D such that

Table 1State variable definitions.

Variable Description

E density of eggsL density of larvaeP density of pupaeAh density of mosquitoes searching for hostsAr density of resting mosquitoesAo density of mosquitoes searching for oviposition sites

Table 2Description and values of parameters of the model. All parameters are positive and time is measured in days. For the model with dispersal, these parameters are patch dependent.

Parameter Description Units Baseline Range Source

b number of female eggs laid per oviposition - 100 50� 300 [56]qE egg hatching rate into larvae day�1 0:50 0:33� 1:0 [56,27],69qL rate at which larvae develop into pupae day�1 0:14 0:08� 0:17 [56],27,4,32,20qP rate at which pupae develop into adult/emergence rate day�1 0:50 0:33� 1:0 [56,27]lE egg mortality rate day�1 0:56 0:32� 0:80 [47]lL1

density-independent larvae mortality rate day�1 0:44 0:30� 0:58 [47]lL2

density-dependent larvae mortality rate day�1 mosq�1 0:05 0:0� 1:0 VariablelP pupae mortality rate day�1 0:37 0:22� 0:52 [47]qAh

rate at which host seeking mosquitoes enter the resting state day�1 0:46 0:322� 0:598 [13], EstimatedqAr

rate at which resting mosquitoes enter oviposition site searching state day�1 0:43 0:30� 0:56 [13]qAo

oviposition rate day�1 3:0 3:0� 4:0 [13]lAh

mortality rate of mosquitoes of searching for hosts day�1 0:18 0:125� 0:233 [13], EstimatedlAr

mortality rate of resting mosquitoes day�1 0:0043 0:0034� 0:01 [13]lAo

mortality rate of mosquitoes searching for oviposition sites day�1 0:41 0:41� 0:56 [13]

200 A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216

D ¼

E

L

P

Ah

Ar

Ao

0BBBBBBBB@

1CCCCCCCCA2 R6

8>>>>>>>><>>>>>>>>:

E P 0;L P 0;P P 0;Ah P 0;Ar P 0;Ao P 0

��������������

9>>>>>>>>=>>>>>>>>;; ð2Þ

where the model is mathematically and biologically meaningful andall solutions of the system (1) with non-negative initial data will re-main non-negative in the feasible region D for all time t P 0. Weuse the notation X0 to represent dX

dt here and denote the boundaryof D by @D.

Theorem 2.1. If the initial conditions of system (1) lie in region D,then there exists a unique solution for (1), EðtÞ; LðtÞ; PðtÞ;AhðtÞ;ArðtÞ,and AoðtÞ that remains in D for all time t P 0.

Proof. The right hand side of the system (1) is continuous withcontinuous partial derivatives in D, therefore (1) has a unique solu-tion that exists for all time. It remains to be shown that D is for-ward-invariant. We see from system (1) that if E ¼ 0, thenE0 ¼ bqAo

Ao P 0; if L ¼ 0, then L0 P 0; if P ¼ 0, then P0 P 0; ifAh ¼ 0, then A0h P 0; if Ar ¼ 0, then A0r P 0; and if Ao ¼ 0, thenA0o P 0. Therefore all solutions of the system of equations (Eq.(1)) are contained in the region D. h

3. Analytical results of the basic model without mosquitodispersal

3.1. Existence of equilibrium points

This section presents existence and stability results of the mod-el (Eq. (1)) of the steady states. An equilibrium point of a given asystem of equations ( _XðtÞ) (where X is a vector composed by statevariables) is a steady-state solution, where XðtÞ ¼ X� for all t.

Proposition 1. The model in (1) has exactly one equilibrium point on@D given by P0 ¼ ð0;0;0;0;0;0Þ. We label P0 the mosquito-freeequilibrium point.

Proof. Substituting Po into the right hand side of (1) shows that allderivatives are zero so Po is an equilibrium point of (1). Setting anyof E; L; P;Ah;Ar , or Ao equal to 0, we see that all other remainingstate variables must also be equal to zero for the system to be atequilibrium. Therefore, Po is the only equilibrium point on @D. h

Similar to White et al. [67], we define the population reproduc-tion number, R0, as the expected number of female mosquitoesproduced by a single female mosquito in her life time in the ab-sence of density-dependence. In [64], a method for computingthe reproduction number for epidemic models was developed.However, it can equivalently be used in ecological models wherenew births are treated as new infections. We determine the mos-quito population reproduction number for model (1) using thenext-generation technique [64].

Defining x as a set of all state variables (E; L; P;Ah;Ar ;Ao) in themodel, then x ¼ ðx1; x2; . . . ; xiÞT for i ¼ 1;2; . . . ; 6. The system in(1) can be written in the form of dxi

dt ¼ FiðxÞ � ViðxÞ, where Fi isthe rate of new recruitment (birth of eggs) in a compartment,Vi ¼ V�i � Vþi , with Vþi being the rate of transfer of mosquitoes intoa compartment and V�i is the rate of transfer of mosquitoes out ofthe compartment. For this model, F, and V are given by:

F ¼

bqAoAo

0

0

0

0

0

2666666666664

3777777777775;

and

V ¼

lE þ qE

� �E

lL1þ qL

� �Lþ lL2

L2 � qEE

lP þ qP

� �P � qLL

lAhþ qAh

� �Ah � qPP � qAo

Ao

lArþ qAr

� �Ar � qAh

Ah

lAoþ qAo

� �Ao � qAr

Ar

266666666666664

377777777777775:

To obtain the next generation operator, FV�1, we calculateFij ¼ @Fi

@xj

���P0

and Vij ¼ @Vi@xj

���P0

to obtain

F ¼

0 0 0 0 0 bqAo

0 0 0 0 0 00 0 0 0 0 00 0 0 0 0 00 0 0 0 0 00 0 0 0 0 0

2666666664

3777777775; ð3Þ

and

A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 201

V ¼

lE þ qE

� �0 0 0 0 0

�qE lL1þ qL

� �0 0 0 0

0 �qL lP þ qP

� �0 0 0

0 0 �qP lAhþ qAh

� �0 �qAo

0 0 0 �qAhlArþ qAr

� �0

0 0 0 0 �qArlArþ qAr

� �

2666666666664

3777777777775:

ð4Þ

The population reproduction number, R0, is the spectral radiusof the next generation operator, qðFV�1Þ. This value is given by

Ro ¼bY

j

qj

ljþqj

� �

1�Y

Ai

qAilAiþqAi

� � : ð5Þ

where j ¼ E; L; P;Ah;Ar;Ao and i ¼ h; r, and o. qj

ljþqjis the probability

that a mosquito in stage j will survive to the next stage. The valueQAi

qAilAiþqAi

� �2 ð0;1Þ for all i is the probability that an adult mos-

quito survives the feeding cycle. Although density-dependent mor-tality of larvae affects mosquito population, R0 does not depend ondensity-dependent mortality of larvae.

Theorem 3.1. The system of Eq. (1) has a persistent positiveequilibrium solution Pe ¼ ðE�; L�; P�;A�h;A

�r ;A

�oÞ, with its components

given by

E� ¼bqAo

A�olE þ qE

;

L� ¼lL1þ qL

� �Ro � 1ð Þ

lL2

;

P� ¼ qLL�

lP þ qP;

A�h ¼qPP�R0

lAhþ qAh

� �B1

; ð6Þ

A�r ¼qAh

A�hlArþ qAr

;

A�o ¼qAr

A�rlAoþ qAo

;

with R0 given in Eq. (5) and B1 ¼ bQ

jqj

ljþqj

� �for j ¼ E; L; P;Ah;Ar;Ao,

which exist in the interior of D if R0 > 1.

Proof. Substituting Pe ¼ ðE�; L�; P�;A�h;A�r ;A

�oÞ into (1) shows that Pe

is an equilibrium point of (1). If Ro > 1, we see that all componentsPe are positive. Thus, Pe exist in the interior of D if Ro > 1. h

3.2. Stability of the equilibrium points

Theorem 3.2. The mosquito-free equilibrium is locally asymptoticallystable when Ro < 1 and unstable otherwise.

Proof. Let the new births in the ecological model (1) be equivalentto new infections in the epidemic models studied in van den Dries-sche and Watmough [64]. The matrices FðxÞ;VðxÞþ, and VðxÞ� sat-isfy the assumptions A(1)–A(5) [64]. Thus, this theorem is astraightforward application of Theorem 2 given in [64]. h

Theorem 3.3. The persistent equilibrium is locally asymptotically sta-ble whenever Ro > 1 and unstable when Ro < 1. When Ro ¼ 1; Pe ¼ Po.

Proof. Let JPebe the Jacobian matrix of system (1) at the mosquito

persistent equilibrium given by

JPe¼

� lE þ qE

� �0 0 0 0 bqAo

qE � lL1þ qL

� ��U 0 0 0 0

0 qL � lP þ qP

� �0 0 0

0 0 qP � lAhþ qAh

� �0 qAo

0 0 0 qAh� lAr

þ qAr

� �0

0 0 0 0 qAr� lAr

þ qAr

� �

26666666666664

37777777777775;

ð7Þ

where U ¼ 2ðlL1þ qLÞ Ro � 1ð Þ. To obtain the eigenvalues of JPe

,we solve detðJPe

� kIÞ ¼ 0. We use the concept of block matricesto compute this determinant. Let J ¼ JPe

� kI be a block matrixgiven by

J ¼A BC D

ð8Þ

with the following components:

A ¼�ðlE þ qEÞ � k 0 0

qE �ðlL1þ qLÞ �U� k 0

0 qL �ðlP þ qPÞ � k

0B@

1CA;

B ¼0 0 bqAo

0 0 00 0 0

0B@

1CA;C ¼

0 0 qP

0 0 00 0 0

0B@

1CA;

and

D ¼�ðlAh

þ qAhÞ � k 0 qA0

qAh�ðlAr

þ qArÞ � k 0

0 qAr�ðlA0

þ qA0Þ � k

0B@

1CA:

It follows from the concepts of block matrices thatdetðJÞ ¼ detðAD� BCÞ. But in this case, BC is a zero matrixleading to detðJPe

� kIÞ ¼ detðJÞ ¼ detðADÞ ¼ 0. By solving the equa-tion, we obtain three of the eigenvalues given by k1 ¼ �ðlE þ qEÞ;k2 ¼ �ðlL1

þ qLÞ �U, and k3 ¼ �ðlP þ qPÞ. When Ro > 1; k2 < 0,which forms the necessary condition for a stable equilibrium point.When Ro < 1; k2 > 0; Pe is unstable. The remaining three eigen-values are given by the roots of the following equation:

a0k3 þ a1k

2 þ a2kþ a3 ¼ 0; ð9Þ

where

a0 ¼ 1;

a1 ¼ lAhþ qAh

� �þ lAr

þ qAr

� �þ lAo

þ qAo

� �;

a2 ¼ lAhþ qAh

� �lArþ qAr

� �þ lAh

þ qAh

� �lAoþ qAo

� �þ lAr

þ qAr

� �lAoþ qAo

� �;

a3 ¼ lAhþ qAh

� �lArþ qAr

� �lAoþ qAo

� �� qAh

qArqAo

¼ lAhþ qAh

� �lArþ qAr

� �lAoþ qAo

� � B1

Ro

� �; ð10Þ

where B1 ¼ bQ

jqj

ljþqj

� �for j ¼ E; L; P;Ah;Ar;Ao. It remains to be

shown that when Ro > 1, the eigenvalues have negative realparts. The roots of the polynomial in Eq.(9) are difficult to calculateexplicitly, but it is clear from (9) that a0 > 0; a1 > 0; a2 > 0, anda3 > 0 always. By the Routh–Hurwitz criteria [41] we need toshow that a1a2 � a3 > 0 for all roots of Eq. (9) to have negative realparts.

202 A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216

a1a2 � a3 ¼ ðlAhþ qAh

Þ þ ðlArþ qAr

Þ þ ðlAoþ qAo

Þh i½ðlAh

þ qAhÞðlAr

þ qArÞ

þ ðlAhþ qAh

ÞðlAoþ qAo

Þ þ ðlArþ qAr

ÞðlAoþ qAo

Þ�� ðlAh

þ qAhÞðlAr

þ qArÞðlAo

þ qAoÞ � qAh

qArqAo

¼ ðlAhþ qAh

Þ2½ðlArþ qAr

Þ þ ðlAoþ qAo

Þ�

þ ðlArþ qAr

Þ2½ðlAhþ qAh

Þ þ ðlAoþ qAo

Þ�

þ ðlAoþ qAo

Þ2½ðlAhþ qAh

Þ þ ðlArþ qAr

Þ�þ 2ðlAh

þ qAhÞðlAr

þ qArÞðlAo

þ qAoÞ � qAh

qArqAo

¼ ðlAhþ qAh

Þ2½ðlArþ qAr

Þ þ ðlAoþ qAo

Þ� ð11Þ

þ ðlArþ qAr

Þ2½ðlAhþ qAh

Þ þ ðlAoþ qAo

Þ�

þ ðlAoþ qAo

Þ2½ðlAhþ qAh

Þ þ ðlArþ qAr

Þ�

þ ðlAhþ qAh

ÞðlArþ qAr

ÞðlAoþ qAo

Þ 1þ B1

Ro

:

From (11) we see that a1a2 � a3 > 0 for all values of Ro. Thus, theroots of (9) have negative real parts. Therefore, when Ro > 1, the sixeigenvalues have negative real parts and the persistent equilibriumpoint is locally asymptotically stable. Where, as whenRo < 1; k2 > 0. The persistent equilibrium point is unstable. Substi-tuting Ro ¼ 1 in (6) shows that at Ro ¼ 1; Pe ¼ Po. h

3.3. Sensitivity Analysis of R0

Sensitivity analysis determines the effects of parameters onmodel outcomes [11]. To carry out local sensitivity analysis, weuse a simple approach to compute the sensitivity index, which isa partial derivative of the output variable with respect to the inputparameters [11,12]. For the base reproduction number, R0, and pi,an input parameter, the sensitivity index can be computed as

Pa

Sens

itivi

ty In

dex

bρL

μL1

ρAh

μAh

ρE

1 2 3 4 5 6−1

−0.5

0

0.5

1

Pa

Parti

al R

ank

Cor

rela

tion

Coe

ffici

ent

bρL

μL1

ρE ρAh

μAh

1 2 3 4 5 6−1

−0.5

0

0.5

1

Fig. 2. Sensitivity Analysis of Ro . A: Local sensitivity analysis. Normalized sensitivity indicGlobal sensitivity analysis. Partial Rank correlation coefficients showing the ranking of p

@R0=@pi. The normalized sensitivity index, XR0pi

, of Ro, with respectto parameter pi at a fixed value, p0 [11,12] is

XR0pi¼ @R0

@pi� pi

R0

����pi¼p0

: ð12Þ

Using the parameter values presented in Table 2, we compute thesensitivity indices using Eq. (12). In Fig. 2A we show the impactof each parameter on the reproduction number. The number of fe-male eggs laid per oviposition, b, is the most important parameterin the model (XRo

b ¼ 1:00), indicating a maximum impact on modeloutcomes. Increasing or decreasing b by 10%, for example, can in-crease or decrease Ro by 10%. The parameters with the next highestsensitivity indices are qL and lL1

. If the development rate from lar-val to pupae stage (qL) is increased, we observe a decreased risk ofdying of larvae (lL1

) and vice versa. A 10% increase (or decrease) inqL, for example, increases (or decreases) Ro by 7:6%, while a similarincrease (or decrease) of lL1

in Ro decreases (or increases) Ro by7:6%. Other important parameters with higher indices are qAh

andlAh

. Similar to qL and lL1, these parameters indicate an equal but

opposite impact on Ro. Increasing qAhcan lead to an increase in

Ro. Increasing lAh, however would decrease Ro.

Local sensitivity analysis shows the effect of one parameterwhile all others are kept constant. Global sensitivity analysis esti-mates the effect of one parameter on the output, while allowing allother parameters to vary, enabling the identification of interac-tions [11]. Here, we used SaSAT software [26] to carry out the glo-bal sensitivity analysis of the mosquito population reproductionnumber. The Latin Hypercube Sampling Method (LHS), a type ofstratified Monte Carlo sampling [6], was used to sample the inputparameters using the parameter value ranges provided in Table 2.Due to the absence of data on the distribution function of theparameters used in our model, a uniform distribution for all inputparameters was chosen. The sets of input parameter values sam-pled using the LHS method were used to run 5000 simulations.

rameters

μE

ρP

μP

ρAo

μAo

ρAr

μAr

A

7 8 9 10 11 12 13

rameters

μE

ρP

μP

μAo

ρAo

μAr

ρAr

B

7 8 9 10 11 12 13

es of R0 to parameters evaluated at the baseline parameter values given in Table 2. B:arameter influence on R0.

A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 203

To identify input parameters with the greatest influence on Ro, wecomputed the Partial Rank Correlation Coefficients between the in-put parameters and our output variable using the SaSAT software.

In Fig. 2B, we present the results of the partial rank correlationcoefficients for each of the parameters. Again, results show thatbirth parameter, b, has the highest influence on the mosquito pop-ulation reproduction number. Next to b are the parameters associ-ated with the larvae stage, followed by the egg development rateand the parameters related to the host seeking stage. Parametersrelated to the resting stage of the mosquitoes show the lowestinfluence on Ro.

In general, we find that mortality rates are negatively correlatedto the population reproduction number, while development ratesare positively correlated. Because the population reproductionnumber gives information on the stability of the equilibrium pointand the persistence of the mosquito population, increasing param-eters that are positively correlated to the reproduction numberwould result in the persistence of the mosquito population.

4. Modelling movement

4.1. Continuous space model

Traditional methods of modelling diffusion have involved theuse of the heat equation in which the domain is assumed to be con-tinuous. If we assume that the movement of individual mosquitoesis similar to that of Brownian motion, then we can define the rateof change of mosquito density at time t at location ðx; yÞ;Mðx; y; tÞas

@Mðx; y; tÞ@t

¼ D�r2Mðx; y; tÞ ð13Þ

where ðx; yÞ 2 R2;r represents the partial derivative in 2-dimensional space and r2M ¼ @2M=@x2 þ @2M=@y2, and D� is thediffusion coefficient (metres2 time�1). We assume that the initialconditions are given by Mðx; y; 0Þ ¼ Kdðx; yÞ, where dðx; yÞ is the 2-dimension Dirac delta function, dðx; yÞ ¼ 0for x2 þ y2 – 0 andR1�1R1�1 dðx; yÞdxdy ¼ 1. Therefore,

R1�1R1�1 Mðx; y; 0Þdxdy ¼ K rep-

Fig. 3. A Schematic representation of a landscape division into hex

resents an initial condition of K mosquitoes released at the origin.The standard solution to the heat Eq. (13) is given by:

Mðx; y; tÞ ¼ K4pD�t

exp �ðx2 þ y2Þ4D�t

ð14Þ

for t > 0 and ðx; yÞ 2 R2. We convert our solution to polar coordi-nates with

x ¼ r cos h and y ¼ r sin h; implying that r

¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffix2 þ y2

pand dxdy ¼ rdrdh: ð15Þ

Using (14) and (15) we obtain

Mðr; h; tÞ ¼ K4pD�t

exp � r2

4D�t

ð16Þ

for r P 0 is the radial distance measured from centre. The mosquitodensity at a given distance, r from the centre is obtained fromMðr; tÞ ¼

R 2p0 Mðr; h; tÞrdh, which gives

Mðr; tÞ ¼ Kr2D�t

exp � r2

4D�t

: ð17Þ

Although partial differential equations (PDEs) are a good way ofmodelling dispersal [18,19], their analysis is usually limited tonumerical simulations when modelling environmental heteroge-neity. Discrete approaches offer a better and simpler way of mod-elling heterogeneity [2,3,29], specifically when resources such ashosts and breeding sites are variable across regions. In the nextsection, we develop a mosquito dispersal model which considersdiscrete space and describes how we model heterogeneity in re-sources and its influence on mosquito dispersal.

4.2. Discrete space model spatial structure

We let N be the set of all patches and n be any patch in N. Weconstruct the model by dividing 2-dimensional space into a setof discrete hexagonal patches (Fig. 3). We label the hexagonal gridwith a coordinate system, ði; jÞ, where 1 6 i 6 n and 1 6 j 6 m rep-resent the locations of the centre of the patches and i; j 2 N.

agonal patches. Model equations (Eq. (36) apply in each patch.

204 A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216

We define the neighbourhood, Nði; jÞ, (Fig. 3) of an index patchas an ordered set of six patches given by

Nði; jÞ ¼ fði; jþ 1Þ; ði; j� 1Þ; ðiþ 1; jÞ; ði� 1; jÞ; ði� 1; jþ 1Þ; ði� 1; j� 1Þg ð18Þ

when j is even or

Nði; jÞ ¼ fði; jþ 1Þ; ði; j� 1Þ; ðiþ 1; j� 1Þ; ði� 1; jÞ; ðiþ 1; j

þ 1Þ; ðiþ 1; jÞg ð19Þ

when j is odd. We assume periodic boundary conditions so thatpatch ði;0Þ ¼ ði;mÞ and ð0; jÞ ¼ ðn; jÞ.

4.3. Dispersal in a homogeneous landscape

Mosquitoes disperse while searching for hosts or ovipositionsites, causing a link between patches. A given fraction of adultssearching for hosts and a fraction of adults searching for oviposi-tion sites leave their original or current patches of residence, whileothers stay behind. We assume that dispersing adults move fromtheir current patch to enter any of the other six nearest neighbour-ing patches (Fig. 3) and that long-range dispersal is achievedthrough a repeated single patch movement. That is, patch jumpingis precluded.

Mosquitoes can detect host odour [33,44], but it is unclearwhether they have the learning capacity they would need to enablethem to return to particular hosts or breeding sites [1]. We makethe simplifying assumption that mosquitoes do not preferentiallyreturn to their previous locations, so that movement is a Markovprocess. In the case where all patches have similar characteristics(i.e. a homogeneous landscape), the mosquitoes disperse equallyto each of the six neighbouring patches surrounding the currentposition (Fig. 3) and the dispersal parameter is the same for allpatches. If we let D > 0 (per time) be the rate at which mosquitoesmove from one patch to a neighbouring patch, we can compute itsvalue from:

D ¼ D�

Að20Þ

where D� is the diffusion coefficient in the absence of all other fac-tors affecting flight. The area A (in metres2) of a hexagon is given by:

A ¼ffiffiffi3p

L2

2; ð21Þ

with L (in metres) being the patch size defined as the measurementfrom the centre of one patch to the centre of the neighbouringpatch. We let Mði;jÞ be the number of free flying mosquitoes in patchði; jÞ. We let mosquitoes move from patch ði; jÞ (a source or indexpatch) to a neighbouring patch n 2 Nði; jÞ. We define the movementrate from patch ði; jÞ to a neighbouring patch n to be Dði;jÞ=n and themovement rate from the neighbouring patch to the index patch tobe Dn=ði;jÞ. For a homogeneous environment, Dði;jÞ=n ¼ Dn=ði;jÞ ¼ D.Assuming that mosquitoes do not reproduce or die during dispersal,the dynamics of free-flying mosquitoes in any patch ði; jÞ can be rep-resented as

dMði;jÞ

dt¼X

n2Nði;jÞDMn �

Xn2Nði;jÞ

DMði;jÞ ð22Þ

with initial conditions Mði;jÞð0Þ. The first term represents mosquitoesmoving into the patch and the second term represents mosquitoesmoving out of a patch. The movement model in (22) is biologicallyand mathematically meaningful in the domain X ¼ Mði;jÞ 2 Rnm, suchthat Mði;jÞ P 0.

Theorem 4.1. If initial conditions lie in region X, the movement Eq.(22) has a unique solution that exists and remains in X for all timet P 0.

Proof. The right hand side of Eq. (22) is continuous with a contin-uous partial derivative in region X and therefore (22) has a uniquesolution. We then show that X is forward-invariant. If Mði;jÞ ¼ 0,then M0

ði;jÞ ¼P

n2Nði;jÞDMn P 0 for all ði; jÞ. Thus, the solution to Eq.(22) is enclosed in X and a unique solution exists for all t. h

4.4. Dispersal in a heterogeneous landscape

Differences in the distribution of resources creates heterogene-ity on the grid, since patches may have different degrees of attrac-tiveness to mosquitoes. In this section, we describe howheterogeneity and differences in patch attractiveness to mosqui-toes during movement is incorporated.

4.4.1. Dispersal with heterogeneity in host availabilityThe number of hosts is allowed to differ between patches across

the grid, introducing heterogeneity. Because of the neighbour toneighbour dispersal nature of this model, movement of mosquitoesfrom one patch to other patches is only affected by the patchesbordering each neighbourhood. We therefore calculate and usethe proportion of hosts in each set of seven patches relative to eachother, using the number of hosts on the particular patch and on itssix neighbours. However, we assume that host distribution acrosspatches is constant over time.

We recall that N is a set of patches on the grid, n is any patch inN, and Nði; jÞ is a set of neighbours given by (18) and (19) of an in-dex patch ði; jÞ. We also let ci;j be a set of seven patches sharingboundaries, that is, patch ði; jÞ and its 6 neighbours. ci0 ;j0 is a set ofseven patches sharing boundaries made up of patch n0 and its sixneighbours, of which one is patch ði; jÞ. For easy reference, weuse the following notations:

� Hn is the population of hosts in patch n� Hij

T is the total population of hosts in ci;j

� Hn0 is the population of hosts in patch n0

� Hi0 j0

T is the total population of hosts in ci0 ;j0

� �Hijn is the proportion of hosts in patch n 2 ci;j out of all hosts in ci;j

� �Hijn0 is the proportion of hosts in patch n0 2 ci;j out of all hosts in

ci;j

� �Hi0 j0

n is the proportion of hosts in patch n 2 ci0 ;j0 out of all hosts inci0 ;j0

� �Hi0 j0

n0 is the proportion of hosts in patch n0 2 ci0 ;j0 out of all hosts inci0 ;j0

We calculate the total number of hosts over these seven patchessharing boundaries from

HijT ¼

Xn2ci;j

Hn; ð23Þ

and the proportion of hosts in each n 2 ci;j from

�Hijn ¼

Hn

HijT

ð24Þ

withXn2ci;j

�Hijn ¼ 1 ð25Þ

Mosquitoes are attracted to odours released by hosts[15,33,44,61]. This leads to mosquitoes being less likely to leavethe patch if their current patch is a home to many hosts and likely

Fig. 4. Diagrammatic representation of mosquito movement between an index patch (source patch ði; jÞ) and a neighbouring patch (ði0; j0Þ ¼ n0 2 Nði; jÞ) where Nði; jÞ is definedby Eqs. (18) and (19).

0.16

0.16

0.2

0.2

0.2

0.20.24

0.24

0.24

0.28

Proportion of hosts in current location

Prop

ortio

n of

hos

ts in

nei

ghbo

ur lo

catio

n

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

Fig. 5. Behaviour of the dispersal function in Eq. (26) at D ¼ 0:2; k ¼ 0:5, and �H 2 ½0;1�.

A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 205

to move out of the patch if there are few hosts. To mimic this phe-nomenon, we use a decreasing exponential function to model themovement rate. If ði; jÞ is a source patch and its neighbours(Fig. 4), and if we take into account the availability of hosts in eachof the patches contained in ci;j, we can define the movement out ofa patch i; j to a neighbour patch n0 as

bHði;jÞ=n0 ¼ De

�k �Hijn��Hij

n0

� �: ð26Þ

Here, k is a constant parameter for the decay function and �Hijn0

isthe proportion of hosts in patch n0 contained in ci;j, which is ob-tained from

�Hijn0¼ Hn0

HijT

: ð27Þ

The function in Eq. (26) (its behaviour is shown in Fig. 5) repre-sents different possible characteristics of two patches sharingboundaries as follows:

� If �Hijn >

�Hijn0

, then 0 < bHði;jÞ=n0 < D. This condition establishes that

the source patch ði; jÞ contains more hosts compared to patchn0. The patch is therefore more attractive to mosquitoes com-pared to its neighbour and will tend to retain mosquitoes; fewmosquitoes will tend to move away from it.

� If �Hijn ¼ �Hij

n0 , then bHði;jÞ=n0 ¼ D. This implies that the two patches

have equal attractiveness to mosquitoes.� If �Hij

n <�Hij

n0 , then bHði;jÞ=n0 > D. Here, patch ði; jÞ is less attractive to

mosquitoes because it has fewer hosts compared to patch n0.The dispersal rate out of the patch is high as more mosquitoeswill migrate out to patches that are more attractive.

Similarly, the movement of mosquitoes from patch n0 to patchði; jÞ (Fig. 4), where both n0 and ði; jÞ are contained in ci;j, is modelled.In this respect, Hi0 j0

T is calculated using a different set of neighbour-ing patches, ci0 ;j0 . In other words, it is the total number of hosts in n0

and its six neighbours, of which one of them is patch ði; jÞ. We cal-culate it using

Hi0 j0

T ¼Xn2ci0;j0

Hn: ð28Þ

Therefore, we model the movement rate from any neighbouringpatch n0 into patch ði; jÞ (as shown in Fig. 4) using

bHn0=ði;jÞ ¼ De

�k �Hi0 j0n0��Hi0 j0

n

� �ð29Þ

where

�Hi0 j0

n ¼Hn

Hi0j0

T

; ð30Þ

206 A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216

and

�Hi0 j0

n0 ¼Hn0

Hi0 j0

T

: ð31Þ

In general, the movement rate from patches with relatively lowattraction is higher compared to patches with higher attractionand vice versa. To summarise, we re-write the general movementmodel presented in Eq. (22) as

dAhði;jÞ

dt¼

Xn02Nði;jÞ

bHn0=ði;jÞAhn0

0@

1A� X

n02Nði;jÞbHði;jÞ=n0

0@

1AAhði;jÞ; ð32Þ

to describe the dynamics of host seeking mosquitoes in the absenceof new recruitment and deaths in any of the patches. Here, the dis-persal rate takes into account the dependence of dispersal on hostsavailability.

4.4.2. Dispersal with heterogeneity in oviposition site availabilityAnother form of heterogeneity is imposed by the availability

of oviposition sites in an area. Mosquitoes searching forbreeding sites for egg laying are attracted by the availability ofbreeding sites [43]. We incorporate this in a manner similar to thatfor hosts.

If Bci;jis the number of oviposition sites in a patch and �Bci;j

is the proportion of oviposition sites in a patch relative to itsneighbours, the movement rate out of the index patch ði; jÞ isexpressed as

bBði;jÞ=n0 ¼ De

�k �Bijn��Bij

n0

� �ð33Þ

and the movement rate into the patch from neighbouringpatches:

bBn0=ði;jÞ ¼ De

�k �Bi0 j0n0��Bi0 j0

n

� �ð34Þ

Similarly, the movement rate of mosquitoes from a patch is higher ifthere are few breeding sites (B) in the patch. We represent themovement of mosquitoes searching for oviposition sites in the fol-lowing equation

dAoði;jÞ

dt¼

Xn02Nði;jÞ

bBn0=ði;jÞAon0

0@

1A� X

n02Nði;jÞbBði;jÞ=n0

0@

1AAoði;jÞ: ð35Þ

Since the density of breeding sites is affected by seasonalvariations, as temporal sites are created due to rainfall forexample, their distribution changes over time. However, in thismodel, for simplicity, we consider only permanent breeding sites.So the initial distribution of breeding sites does not change overtime.

4.5. Full dispersal model equations

In Section 2, we studied the dynamics of mosquito populationsin each stage of the mosquito life cycle within a single patch. Weextend this model to incorporate dispersal processes. If we allowhost seeking and oviposition site searching mosquitoes to movebetween patches, then we can combine the system of equationsin Eq. (1) for patch ði; jÞ and the movement terms in (32) and(35) to form the following system of equations:

dEði;jÞdt¼ bði;jÞw

Bði;jÞqAoði;jÞAoði;jÞ � lEði;jÞ þ qEði;jÞ

� �Eði;jÞ

dLði;jÞdt¼ qEði;jÞEði;jÞ � lL1ði;jÞ þ lL2ði;jÞLði;jÞ þ qLði;jÞ

� �Lði;jÞ

dPði;jÞdt¼ qLði;jÞLði;jÞ � lPði;jÞ þ qPði;jÞ

� �Pði;jÞ

dAhði;jÞ

dt¼ qPði;jÞPði;jÞ þ wB

ði;jÞqAoði;jÞAoði;jÞ � lAhði;jÞþ wH

ði;jÞqAhði;jÞ

� �Ahði;jÞ

�X

n02Nði;jÞbHði;jÞ=n0

0@

1AAhði;jÞ þ

Xn02Nði;jÞ

bHn0=ði;jÞAhn0

0@

1A ð36Þ

dArði;jÞ

dt¼ wH

ði;jÞqAhði;jÞAhði;jÞ � lArði;jÞ

þ qArði;jÞ

� �Arði;jÞ

dAoði;jÞ

dt¼ qArði;jÞ

Arði;jÞ � lAoði;jÞþ wB

ði;jÞqAoði;jÞ

� �Aoði;jÞ

�X

n02Nði;jÞbBði;jÞ=n0

0@

1AAoði;jÞ þ

Xn02Nði;jÞ

bBn0=ði;jÞAon0

0@

1A

with initial conditions Eði;jÞ; Lði;jÞ; Pði;jÞ;Ahði;jÞ;Arði;jÞ;Aoði;jÞ P 0 at timet ¼ 0. Here, H and B represents hosts and breeding sites respec-tively. The state variables and some of the parameters carry thesame meaning as in system (1) (see Tables 1 and 2). The individualequations in system (36) describe the evolution of eggs, larvae, pu-pae, host seeking, resting, and oviposition site searching mosquitoesin patch ði; jÞ.

The progression from the oviposition site searching state, Ao, tothe host seeking state, Ah. is possible if and only if oviposition sitesearching mosquitoes have laid eggs. We introduce a parameterwBði;jÞ defined by:

wBði;jÞ ¼

1 if Bði;jÞ > 00 if Bði;jÞ ¼ 0;

(ð37Þ

to control this process, since laying eggs in a patch is possible only ifthe particular patch contains at least one breeding site. In patcheswhere Bði;jÞ ¼ 0, the initial conditions for Eði;jÞ; Lði;jÞ, and Pði;jÞ are 0.Similarly, the progression from host seeking to the resting stage ispossible if there are hosts in the patch [31]. As such, we define

wHði;jÞ ¼

1 if Hði;jÞ > 00 if Hði;jÞ ¼ 0:

(ð38Þ

Patches without hosts have initial conditions Arði;jÞ ¼ 0. All otherparameters are patch dependent and their definitions are summa-rised in Tables 2 and 3.

The total number of mosquitoes in each stage at time t over allpatches on the grid is given by the sum over all locations N. That is

SðtÞ ¼Xn2N

SnðtÞ !

ð39Þ

with SðtÞ representing the stage specific total number of mosquitoes(EðtÞ; LðtÞ; PðtÞ;AhðtÞ;ArðtÞ, and AoðtÞ). The solutions of Eq. (36) re-main nonnegative in the region

C ¼

Eði;jÞLði;jÞPði;jÞAhði;jÞ

Arði;jÞ

Aoði;jÞ

0BBBBBBBB@

1CCCCCCCCA2 R6nm

8>>>>>>>><>>>>>>>>:

Eði;jÞ P 0;Lði;jÞ P 0;Pði;jÞ P 0;Ahði;jÞ P 0;Arði;jÞ P 0;Aoði;jÞ P 0

��������������

9>>>>>>>>=>>>>>>>>;; ð40Þ

because movement always stops when there are no mosquitoes in apatch. The model is therefore mathematically and biologically wellposed.

Table 3Description of parameters and variables specific to the dispersal model.

Parameter Description Units

H number of hosts hostsB number of breeding sites breeding sites

bH dispersal rate of host seeking mosquitoes per time

bB dispersal rate of mosquitoes searching forbreeding sites

per time

bH� dispersal rate of mosquitoes in the presence ofrepellents

per time

L patch size metresD rate of movement per timek a constant parameter for the decay function dimensionlessD� diffusion coefficient metres2time�1

p repellents blocked ability of mosquitoes toenter a patch

dimensionless

/H a fraction measuring the strength of a repellentin in patch i; j

unitless

A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 207

Theorem 4.2. Assuming that initial conditions lie in C, the system ofequations for the mosquito population dynamics for all patches (36)has a unique solution that exists and remains in C for all time t P 0.

Proof. The right hand side of system (36) is continuous withcontinuous partial derivatives in region C. Thus, there exists aunique solution for (36). We show that region C is forward-invariant. From system (36) we see that if Eði;jÞ ¼ 0, then

E0ði;jÞ ¼ bði;jÞwBði;jÞqAoði;jÞAoði;jÞ P 0; if Lði;jÞ ¼ 0, then L0ði;jÞ ¼ qEði;jÞEði;jÞ P 0;

if Pði;jÞ ¼ 0, then P0ði;jÞ ¼ qLði;jÞLði;jÞ P 0; if Ahði;jÞ ¼ 0, then

A0hði;jÞ ¼ qPði;jÞPði;jÞ þ wBði;jÞqAoði;jÞAoði;jÞ þ

Pn02Nði;jÞb

Hn0=ði;jÞAhn0

� �P 0; if

Arði;jÞ ¼ 0, then A0rði;jÞ ¼ wHði;jÞqAhði;jÞ

Ahði;jÞ P 0; and if Aoði;jÞ ¼ 0, then

A0oði;jÞ ¼ qArði;jÞArði;jÞ þ

Pn02Nði;jÞb

Bn0=ði;jÞAon0

� �P 0. Therefore, all solutions

of the system of equations in (36) are contained in the region N anda unique solution exists for all t. h

System (36) is at an equilibrium if the right hand side is zero atall time t. Patch ði; jÞ is at a mosquito-free equilibrium ifEði;jÞ ¼ Lði;jÞ ¼ Pði;jÞ ¼ Ahði;jÞ ¼ Arði;jÞ ¼ Aoði;jÞ ¼ 0. However, given thecomplexity of the model, we do not show its stability or showthe existence of other invariant subsets and only run numericalsimulations of this model.

5. Numerical simulations

The model without dispersal (Eq. (1)) and the model with dis-persal (Eq. (36)) are both simulated using Matlab 7:10:0(R2010a)student version [40] and the ode45 solver for solving differentialequations is used. The 25 by 21 grid (see sketch in Fig. 3) is usedas a platform to simulate movement of mosquitoes between hex-agonal patches. To ensure that boundary conditions do not influ-ence results, periodic boundary conditions are used. This impliesa torus topology for the landscape, where edge patches are suchthat their nearest neighbours on the outside are patches on theopposing edges.

For model simulation and investigation, we use data on stagespecific mortality and development rates from the literature (seeA), summarised in Table 2. For mosquito dispersal, some studiesshow that mosquitoes can move up to 800 m a day [21]. Field stud-ies on mark release recapture experiments of Anopheles gambiaealso show that daily flight range from 200 to 400 m [42]. These re-sults indicate that mosquito dispersal distance is variable. Due tothese variations, in Section 6.1 we use our model platform (Sec-tion 4) and the movement rate D (Eq. (20)) to produce distributionsof dispersed mosquitoes by distance travelled in a day. However,for numerical illustration of the model with dispersal, we set the

distance from the centre of one patch to the centre of the neigh-bouring patch, L, to 50 m.

We run simulations with total numbers of 2700 eggs, 1900 lar-vae, 2000 pupae, 2400 host seeking adults, 1800 resting adults, and1200 oviposition site seeking adults, initially distributed across thegrid (Fig. 7). The distribution is based on the whether a patch con-tains breeding sites or hosts. Five scenarios are set up to simulatethe effect of different kinds of heterogeneity (Fig. 6). In the firstscenario, all patches contain hosts and breeding sites; the secondscenario simulates the case when hosts and breeding sites are ran-domly distributed on the grid. In the third scenario, all patchescontain breeding sites and hosts are only on one side of the grid;while in the fourth scenario, hosts are present in all patches, withbreeding sites being on one side of the grid. In scenario five, hostsand breeding sites are placed in clusters that are far apart fromeach other. Simulations are continued for each scenario until thetotal mosquito population over the entire grid for each of thestages and their spatial distribution reaches an equilibrium. The fi-nal time of analysis for the simulations for all results presented inthis work is 250 days, except where stated otherwise.

6. Model application, comparisons, and results

6.1. Dispersal distances

In this section, we use the dispersal model to estimate the dis-tance travelled by an average mosquito. The evolution of Eq. (22) issimulated on a homogeneous grid with uniform attractiveness tomosquitoes. The system is initialized with all mosquitoes placedat a single source patch. We then calculate the total number ofmosquitoes per patch and per neighbourhood, the average densityof mosquitoes per patch, and the average of the dispersal distanceafter time 1.

We let MnðtÞ be the average density of mosquitoes in a patch attime t, where n measures the distance from the source patch. Here,n is 0;1;2; . . . ;m, with n ¼ 0 being the source patch, n ¼ 1 beingthe nearest neighbouring patches (first ring of patches), n ¼ 2being the second ring of patches, n ¼ 3 being the third ring ofpatches, and so on (see Fig. 8). The total number of patches in eachof the rings is given by

Nn ¼6n for n P 11 for n ¼ 0:

�ð41Þ

The total number of mosquitoes that reached ring n after timet; PnðtÞ is

PnðtÞ ¼XNn

k¼1

CkðtÞ; ð42Þ

where Ck is the number of mosquitoes in patch k contained in n.From Eq. (42), we obtain the mosquito frequency distance travelledfrom the source patch for a particular time t. We present the resultsin Fig. 9A for t ¼ 1 day and different values of D.

The average density of mosquitoes per patch, after time t haselapsed, is obtained from:

MnðtÞ ¼PnðtÞNn

; ð43Þ

which gives the average density distribution presented in Fig. 9Bwhen t ¼ 1 day.

We let S1 be the initial number of mosquitoes released from thesource patch and the weighted average distance travelled by onemosquito at time t;WdðtÞ, is

WdðtÞ ¼Pm

n¼0nPnðtÞS1

� �� L ð44Þ

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Fig. 6. Spatial arrangements of hosts and breeding sites on the grid showing the set up of scenarios. Scenario 1 (first row): all patches contain hosts and breeding sites.Scenario 2 (second row): random distribution of hosts and breeding sites. Scenario 3 (third row): all patches contain breeding sites but hosts on one side of the grid. Scenario 4(fourth row): all patches contain hosts but breeding sites are on one side of the grid. Scenario 5 (fifth row): clusters of hosts and breeding sites are far apart from each other.

208 A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216

where L is the patch size. We calculate the weighted average of thedispersal distance travelled by a mosquito in one day, Wdð1Þ.

In Fig. 9A we present the results of the frequency distributionof mosquitoes dispersed in a day by distance from source at dif-ferent values of the diffusion parameter. As expected, increasingvalues of D results in mosquitoes moving faster and reaching lar-ger distances. Fig. 9B shows the average density of mosquitoes

per patch by distance moved in a day. After one day, most mos-quitoes have moved, but the source still contains the highestdensity.

From simulations, the weighted mean distance travelled byeach mosquito per day (as calculated from Eq. (44)) is estimatedto be 43;79, and 103 m when L ¼ 50 m and mosquitoes are al-lowed to move at a rate, D, of 0:2;0:5, and 0:8, respectively.

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A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 209

6.2. Comparison between discrete and continuous space form of themodels

The nearest neighbours movement approach has been shown torelate closely to diffusion models [3,30]. To evaluate the effects of

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using discrete space, we compare the behaviour of the discretespace movement model (Eq. (22)) under homogeneous conditionsto that of the model that uses the diffusion approach (Eq. (13)). Bycomparing the behaviour of the two approaches, we calculate howfar a mosquito can travel in a day (and time is set to 1 day in the

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Fig. 10. Comparison between the discrete space Eq. (32) and continuous space Eq. (17) (obtained from Eq. (13)) models. A total number of 600 mosquitoes initially placed atthe source patch during the simulation of the discrete space model (with k ¼ 0:5) were also used in the continuous space version of the model (i.e. K ¼ 600). Mosquitoes wereallowed to move at the same rate (i.e. D ¼ 0:2) for both forms of the model and time was set to 1 day.

210 A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216

simulations for both models).Fig. 10 presents the results of the dis-crete (Eq. (22)) and continuous forms (Eq. (17)) of the model. Thescenario we compare to the diffusion model is such that all patchescontain mosquito resources, creating uniformity in attractivenessto mosquitoes between patches. The probability of a mosquito

moving in any direction is therefore the same. The two models pro-duce slightly different results. However, the distributions showsimilar properties in terms of the modelled mosquito trajectoriesbetween the discrete space and the continuous space models. Bothmodels show peaks in mosquito density near the point of release.

A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 211

The continuous model shows a higher peak and a higher rate of de-crease compared to the discrete model.

6.3. Spatial repellents

Spatial repellents can have different effects on mosquito dis-persal, and hence population dynamics, in different areas. These

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Fig. 11. Spatial population distribution of mosquitoes by scenario (Fig. 6) and stage. Scerow): random distribution of hosts and breeding sites. Scenario 3 (third row): all patchesall patches contain hosts but breeding sites are on one side of the grid. Scenario 5 (fifth rare a snapshot taken at day 250 when the whole system is at an equilibrium.

repellents can be non-physical barriers, such as the treating perim-eters with insecticides to protect populations from mosquito bites[8] by reducing the number of biting mosquitoes moving into thearea [9]. We use the dispersal model developed in this paper toevaluate the effect of including patches with spatial repellents onthe distance travelled by mosquitoes. We include a multiplicativefactor /ði;jÞ ¼ 1� pði;jÞ, where pði;jÞ 2 ½0;1� to account for the effect

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nario 1 (first row): all patches contain hosts and breeding sites. Scenario 2 (secondcontain breeding sites but hosts are on one side of the grid. Scenario 4 (fourth row):

ow): clusters of hosts and breeding sites are far apart from each other. These results

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Fig. 12. Population dynamics of mosquitoes across the grid by scenario and stage. Scenario 1: Both hosts and breeding sites were present in all patches. Scenario 2: Both hostsand breeding sites were randomly distributed across the grid. Scenario 3: Breeding sites were placed in all patches, hosts were clustered on one part of the grid. Scenario 4:Hosts were placed in all patches, but breeding sites were placed on one part of the grid. Scenario 5: Both hosts and breeding sites were placed on one part of the grid, far fromeach other. Fig. 6 shows the set up of the scenarios.

212 A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216

of spatial repellents on flying mosquitoes in some patches. Theparameter p can be interpreted as the blocked ability of mosqui-toes to enter into a patch. When pði;jÞ ¼ 1, the barrier in the patchacts as an obstacle which completely blocks movement and whenpði;jÞ ¼ 0, movement is not impeded. For host seeking mosquitoes,the dispersal rates from the source patch become:

bH�ði;jÞ=n0 ¼ /n0b

Hði;jÞ=n0 ð45Þ

and the dispersal rate into the patch changes to

bH�n0=ði;jÞ ¼ /ði;jÞb

Hn0=ði;jÞ: ð46Þ

We note that in this way of modelling spatial repellents, emergingadults are not chased away by the repellents unless they have en-tered the host seeking stage.

We set up two scenarios to simulate the effect of repellents,with pði;jÞ ¼ 0:8. In the first scenario, we place repellents in the sec-ond ring to source (i.e. n ¼ 2) to form a regular ring distribution. Inthe second scenario, we randomly distribute repellents over thepatches across the landscape. Results from these two scenarioswere compared with results produced under homogeneous condi-tions (without repellents in any of the patches).

The presence of repellents in patches placed at n ¼ 2 creates abarrier to mosquitoes (Fig. 9A). Most mosquitoes move away fromthe source and cluster in the first neighbourhood (n ¼ 1). Few mos-quitoes are observed in the second neighbourhood. The density ofmosquitoes for n > 2 are lower, compared to the scenario whenthere are no repellents. At larger distances from the source patch,the presence of repellents in patches near the source did not showany impact on mosquito dispersal.

The density of mosquitoes in the source patch is found to behigher when D is 0:8, with repellents placed in a ring of patches,

than at D ¼ 0:2 with no repellents. From n ¼ 1 to n ¼ 2, there isno major difference between the two scenarios. For n > 2, mos-quito density is smaller when D is set to 0:2, compared to whenrepellents are placed in a ring distribution. In this case, the repel-lent does not have a strong impact on the movement of mosquitoesand therefore the value of the movement rate has a substantial rolein controlling movement to other patches. When there are patcheswith repellents, the average number of mosquitoes dispersed perpatch (Fig. 9B) does not differ much from a scenario where theare no repellents. On the other hand, a small difference is observedfor n < 2.

A random distribution of repellents results in mosquitoes clus-tering in the source patch and in the nearest neighbourhoods. Few-er mosquitoes are observed clustering in the patches far from thesource patch compared to a situation when there are no repellents.

In the presence of spatial repellents, with D ¼ 0:8, the weightedmean distance moved is estimated to be 78 m when repellents areplaced at n ¼ 2 and 55 m when repellents are randomly distributedacross the landscape.

6.4. Impact of heterogeneity on spatial distribution

Fig. 11 shows the effect of heterogeneity on the spatial distribu-tion of larvae, host seeking, and oviposition site searching mosqui-toes when the system is at equilibrium. The populationdistribution is highly dependent on the distribution of both hostsand breeding sites. As expected, when all patches on the grid haveboth hosts and breeding sites, the entire grid become densely pop-ulated. Host seeking mosquitoes show a pronounced spread acrossthe grid when hosts and breeding sites are randomly distributed,compared to mosquitoes searching for oviposition sites. When

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Fig. 13. A comparison of time series plots between the model without (system (1)) and with dispersal ((36)) was simulated under parameter values given in Table 2. For themodel with dispersal, the average number of mosquitoes across all patches on the grid are plotted. Two scenarios were simulated for the dispersal model: hosts and breedingbreeding sites randomly distributed across the landscape (H and B random), and hosts and breeding breeding sites present in all patches (H and B in each patch).

A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 213

breeding sites are placed in all patches and hosts are clustered onone part of the grid, host seeking mosquitoes spread over a largerarea, compared to a scenario where hosts are present in all patchesand breeding sites are clustered on one side of the grid.

6.5. Impact of dispersal on population distribution

Mosquito dispersal becomes more important when the distri-bution of hosts and breeding sites on the grid is heterogeneous(Fig. 11). Clustering of host seeking mosquitoes towards patchescontaining both hosts and breeding sites is observed. However,when hosts and breeding sites are located in separate parts ofthe grid, the population dies out within a few days (given the as-sumed initial densities of mosquitoes for these simulations).

6.6. Impact of heterogeneity on the dynamics of the total population

Fig. 12 presents the dynamics of the total population (Eg. (39))over all patches on the grid. Heterogeneous distributions of breed-ing sites and hosts, to a large extent, reduces the population atequilibrium. When clusters of breeding sites and hosts are placedfar from each other, mosquitoes become unable to reproduce asdistances required to travel is increased. Hence, population extinc-tion is possible.

6.7. Impact of dispersal and heterogeneity on population dynamics

To evaluate the impact of dispersal and heterogeneity on popula-tion dynamics, we carried out numerical simulations using modelsboth without (system (1)) and with dispersal (system (36)). Whilemaintaining the same set up of multiple sources of mosquitoes(Fig. 7) for comparison purposes, we computed the average numberof mosquitoes at equilibrium across all patches on the grid for thedispersal model. The two models show slightly different equilibriumvalues (Fig. 13) (i.e. ð7339;577;93;194;206;26Þ for the model with-

out dispersal and ð7197;564;91;190;202;25Þ for the dispersalmodel when all patches have hosts and breeding sites). For ran-domly distributed mosquito resources, the average equilibrium va-lue across all patches on the grid was ð118;31;5;7;6;1Þ. Thiscorresponds to an equilibrium population, measured as number ofmosquitoes per km2, as ð33:2;2:6;0:4;0:9;0:9;0:1Þ � 105 whenhosts and breeding sites were present in all patches and approxi-mately ð54:374;14:380;2:314;3:257;2:630;0:333Þ � 103 when re-sources are randomly distributed across the grid.

7. Discussion

Mathematical models for evaluating the impact of the transmis-sion of vector borne diseases do not consider effects on vectormobility, despite evidence that the relative locations of mosquitobreeding sites and of human hosts profoundly affect transmissionof both malaria [14,59] and the dengue virus [28,65]. One reasonfor this is that, whereas spatial variation in biting rates is relativelyeasy to study, rates of movement of mosquitoes can only be stud-ied using challenging mark-recapture techniques, which providesparse data. Consequently, there is little evidence of the impactof heterogeneity in the distribution of resources used by mosqui-toes on the mosquito population size and its spatial distribution.The likely impact of interventions that may affect mosquito move-ment is thus even less well understood.

Our compartment model of the life cycle and feeding cycle ofmosquitoes incorporates spatial heterogeneity both in densitiesof breeding sites and of human hosts. It also incorporates mosquitomovement and can be used to predict the effects of interventionstargeting different stages of the mosquito life cycle. We considereffects on population size, on the spatial distribution of mosqui-toes, and on how far individual mosquitoes move. We use theexample of spatial repellents to illustrate how these parameterscan be affected by a relatively simple intervention.

214 A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216

In a homogeneous environment, the model without dispersalindicates that there is a linear relationship between populationreproduction numbers and both age-stage specific survival anddevelopmental rates of mosquitoes. This leads to straightforwardrelationships between the size of the mosquito population, devel-opmental rates from larvae to pupae, and mortality rates of larvae.However, when there are heterogeneities in resource availability,these linear relationships are disturbed, and have far-reachingthe effects on spatial distribution and population dynamics of mos-quitoes [66]. If breeding sites are eliminated from the neighbour-hoods of hosts or are not available in most patches, mosquitoessearching for breeding sites are forced to move longer distancesin search of oviposition sites, prolonging the feeding cycle[13,35] and increasing mortality during searching [54]. In general,environmental heterogeneity forces mosquitoes to move longerdistances and increases their mortality [54]. In our models, wecould eliminate mosquito populations by separating breeding sitesand hosts.

From the host’s perspective, living in proximity to mosquitobreeding sites increases exposure to mosquito bites and potentiallyalso to disease. Because the vector-host ratio is higher aroundbreeding sites [34], selectively eliminating breeding sites in areasof human habitation can prevent mosquitoes from using humanhosts for blood meals [24]. Similarly, a possible intervention strat-egy is to deploy interventions such as spatial repellents or bed netsaround breeding sites. However, our simulations suggest that sucha ring strategy for repellent deployment is advantageous only ifmosquito sources are few, clearly defined, and known. In situationswhere mosquito sources and households are scattered throughoutthe area, this strategy will not be feasible. However, even randomdeployment of repellents reduces the distance moved by mosqui-toes, making it more difficult for them to complete their life cycle,and hence has beneficial effects.

Spatial heterogeneity in resource availability can thus, on itsown, have complex effects on mosquito populations. Even rela-tively simple interventions, such as spatial repellents, can be de-ployed in a variety of ways in such environments. We have onlyjust begun to use our model to explore the implications of theresulting multiplicity of combinations of environments with inter-vention strategies. Analysing of the spatial effects of more complexinterventions, such as insecticide treated mosquito nets, whichhave simultaneous killing and repellent effects, will bring furtherchallenges.

Like any model, ours has limitations. Effects of wind, which caneither facilitate or prevent movement [7,16,33,51,57], were notincorporated. We chose to use a discrete hexagonal patches as arepresentation of space, rather than using a continuous space mod-el [51,63] because this makes it easier to model arbitrary spatialdistributions of resources. At the same time, this constrained themodelled mosquito movements to follow a limited set of trajecto-ries. We do not know what trajectories mosquitoes adopt in realityand strategies such as Levy flight [52] may well be used to optimizeforaging efficiency. An alternative approach to our discrete spacemodel is to use a PDE model for mosquito dispersal, for examplethat of Raffy and Tran [51,63]. Here attractiveness is representedvia chemotaxis or an advection term, taking into account bloodmeals, breeding sites, wind, etc. The advantage of the discretespace model proposed in this paper is that one can easily assessvector control strategies, as the discrete space enables easy repre-sentation of interventions that cover sets of households or villages.

The differences in the peaks and rates of decrease in mosquitodistributions by distances travelled indicate that the choice ofthe exponential movement rate in the discrete model does notforce the results to be the same as those produced by the continu-ous space approach. However, we could show that although thereare differences, mosquito distributions by distances moved have

similar properties (both models show peaks in mosquito densityin the regions close to the origin and are zero far away from the re-lease point) to those predicted by a continuous space diffusionmodel [48], and suggest that our results are broadly applicableno matter what foraging strategies mosquitoes may adopt.

We could also show that the various factors taken into accountby the model play an important role in the spatial distribution ofmosquitoes. The model could show realistic behaviours in simpletheoretical situations on an artificial landscape. Our model, to-gether with field data, could be used to determine areas of hightransmission within local settings, evaluate the community effectof interventions, and aid in developing possible and efficient vectorcontrol strategies, which can optimize the allocation of scarceresources.

Acknowledgement

The authors acknowledge the contributions of many colleaguesto this work, in particular the members of the malaria modellinggroup of the Swiss Tropical and Public Health Institute. We thankOlivier Briet for reading and providing valuable comments on ourmanuscript. We also thank Amena Briet for her careful readingand edits of the manuscript. The initial version of this work waspresented at the European Conference on Mathematical and Theo-retical Biology held in Krakow, Poland in June, 2011. Comments re-ceived from the participants are acknowledged. We alsoacknowledge the funding support provided by the Bill and MelindaGates Foundation through Swiss TPH and the Ifakara Health Insti-tute. The views expressed in this work are those of the authors.

Appendix A. Data for model parameters

Data for parameterizing the model was obtained from litera-ture. There is variability in the available data as study designsand conditions under which studies were carried out vary fromone place to another. A single value was chosen from a range ofvalues as baseline and used for the numerical simulation of themodel.

The development of mosquitoes in their early stages is a nonlin-ear process that depends on water temperature [27,50,17]. How-ever, for simplicity, we assume that the mean development timefor each stage is constant over time.

For Anopheles gambiae, the duration of egg development (fromoviposition to hatching into a larva) (1=qE) is about 2 days in fieldenvironments [56]. Under laboratory conditions and tropical areasthis period extends to 3 days [27,69,56]. In a study by [56], the lar-val period for mosquitoes of the Anopheles genus is found to be7 days. Other studies have shown that the larval stage may last(1=qL) between 6 to 10 days in field environments or 11 to 13 daysin laboratory conditions [27] or last between 7 to 15 days in tem-perate and tropical areas [4,32,20]. It has also been found that thepupal period (1=qP) lasts for 1� 2 days in field environments butunder laboratory conditions the pupal period lasts for about 2 days[27]. In tropical regions the pupal stage for Anopheles genus last be-tween 2 to 3 days [56].

We used mean mortality rates of 0:56� 0:28 for eggs,0:51� 0:14 for larvae instars I and II, 0:37� 0:14 for larvae instarsIII and IV, and 0:37� 0:15 for pupae [47]. The average of the twocategories of larvae for the density independent mortality of larvae,lL1¼ 0:44� 0:14. Larval mortality can be resolved into natural

mortality rates, lL1and density dependent mortality of larvae,

lL2. For our simulations, we allow lL2

to take any value between0 and 1.

Since the model details the adult mosquito life cycle via themosquito feeding cycle, we derive the estimates of most of the

A.M. Lutambi et al. / Mathematical Biosciences 241 (2013) 198–216 215

parameters from studies on the mosquito feeding cycle. The timespent while searching for hosts (1=qAh

) can be estimated. From[13], we can calculate qAh

¼ 0:46. Once mosquitoes survive thehost seeking stage and have successfully fed, mosquitoes rest forfood digestion and egg maturation. Using 1=qAr

¼ 2:33 days [13],which is qAr

¼ 0:43 per day, we can calculate the value of lAras

0:0043 given that the probability of surviving while resting is1� lAr

=ðlAr� qAr

Þ ¼ qAr=ðlAr

þ qArÞ ¼ 0:99 [13]. If mosquitoes

spend 1=qAo¼ 0:33 days ovipositing, then qAo

¼ 3 per day. The cor-responding probability of surviving the oviposition site searchingstage 1� lAo

=ðlAoþ qAo

Þ ¼ qAo=ðlAo

þ qAoÞ is 0:88 [13]. From this

probability, we obtain lAo¼ 0:41 per day. From [13] we see that

the probability of surviving the feeding cycle is pf ¼ 0:623. Fromour model, this probability can be calculated fromqAh

=ðlAhþ qAh

Þ� �

qAr=ðlAr

þ qArÞ

� �qAo

=ðlAoþ qAo

Þ� �

. Substitutingthe values for the survival probabilities of the oviposition sitesearch and resting given above in this section, we obtainqAh

=ðlAhþ qAh

Þ ¼ 0:72 as the probability of surviving during thehost searching. Thus, we obtain lAh

¼ 0:18 (Table 2).

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