Transcript Slide 1

Mathematical Epidemiology of
infectious diseases
Chapter 1
Section 1.1 until 1.3.3
Marieke Jesse and Maite Severins
Theoretical Epidemiology
Faculty of Veterinary Science
Utrecht
Consider a virgin closed population and assume that at least one disease-causing
organism is introduced in at least one host.
Then the following questions arise:
•
Does this cause an epidemic?
•
If so, with what rate does the number of infected hosts increase during
the rise of the epidemic?
•
What proportion of the population will ultimately have experienced
infection?
1.2 Initial growth
1.2.1 Initial growth on a generation basis
R0 (the basis reproduction ratio):
The expected number of secondary cases per primary case in a ‘virgin’ population
This ratio is a threshold parameter; in the sense of an epidemic, if
R0 < 1 : the number of infected decreases and the disease dies out
R0 > 1 : an epidemic can occur.
The probability p that contact between a susceptible and an infective leads to
transmission depends on the time elapsed since the infective was itself infected.
Assume:
1
0 if   T1

 p if T1    T2
0 if T  
2

0  p 1

p
0
T1
time of infection
the time since infection took place (age of infection)
Infectious period = T2 – T1= ΔT
R0  pc(T2  T1 )
where c is the expected number of contacts per unit of time
T2

1.2.2 Influence of demographic stochasticity; introducing a branching
process on a generation basis.
The growth of the infectious population is modelled as if newly infected individuals
were offspring of the infected. Thus the growth of the infectious population can be
described as a normal reproduction process that has branching like a family tree.
Consider the finite (sub)population of infected individuals from a generation
perspective and assume that individuals reproduce independently from each other,
the number of offspring for each being taken from the same probability distribution
{q k }k 0 . This means that any individual gets k offspring with probability qk and
that :

q
k 0
k
1
The expected number of offspring R0 can be found from {qk} as

R 0   kqk
k 1
In words: Ro equals the sum of the number of offspring times the chance to this
number of offspring.
Assume q0 > 0, so there is a positive probability that an individual will not
produce any offspring.
Now start the process with one individual then,
q0 is the probability that a population will be extinct after one generation.
Let zn denote the probability that the population will be extinct after n steps.
Then clearly z1 = q0 and it can be shown (book) that zn can be recursively
computed from the following equation:
zn  g ( zn1 )
where

g ( z )   qk z k
k 0
In words: g(z) is the sum of chances to a certain number of offspring times the
number of generations before the population goes extinct for all branches.
This function g(z) is called a generating function, in the book some properties of
this function are stated as exercise 1.5.
The function g(z) increases and so does the sequence zn which has a limit
z  limn zn
z
: probability that the population started by the first individual will go extinct.
When:
•
•
z  1
, the population goes extinct with certainty;
0  z  1
We want to relate
, there exists a probability1  z that the population will not go
extinct
z to R0,
•
R0  1
implies
•
R0  1
gives
and we expect that:
z  1
and
0  z  1
This is going to be proved in exercise 1.7
Exercise 1.7
z is the smallest root in [0,1] of the equation z  g (z ) (see fig and proven in ex. 1.6)
Here we will show that z  1 for R0 < 1.
Look at the function z  g (z ) , this function has at most two zeros, since -g’’(z) < 0.
From exercise 1.5 we know that :
• g(1) = 1
• g’(1) = R0
• g(0) = q0 > 0
• g’’(z) > 0
g
R0< 1
z=g
Since R0<1,
g(z)
z  g ( z )  0 for z slightly larger than 0
and for z slightly less than 1.
Thus the function has two roots or no
roots on the interval [0,1). Two is
impossible because of second
derivative, thus only one root at
z = 1 therefore z = 1 is the smallest
root and z  1 for R0< 1.
z1 z2 z3 z∞
z
Conclusion:
Even in the situation where the infective agent has the potential of exponential
growth, i.e. R0 > 1, it still may go extinct due to an unlucky (for the parasite)
combination of events while numbers are low. The probability that such an extinction
happens, when we start out with exactly one primary case, can be computed as a
specific root of the equation z  g (z )
The probability z that the introduction of an infected host from outside does
not lead to an epidemic can be expressed in terms of the parameters.
Therefore function g (or, equivalently, the probabilities qk) has to be derived.
The probabilities depends on the used probability distrubtions, e.g. Poisson or
binomial.
It is important to notice that although the basic reproduction number R0 remains
the same, the probability z depends on the function g(z).
Conclusion: different kinds of transmission models yields different values for z
though the basis reproduction number Ro remains the same.
1.2.3 Initial growth in real time
So far we have looked at initial growth on a generation basis and found a threshold
occurring by a parameter R0 and that for R0 above this threshold, there exists a
positive probability z that introduction of one primary case does not lead to
explosive exponential growth.
For simple models the values for R0 and z can be determined explicitly in terms
of the parameters of the model. However, measuring growth on a generation basis
is not possible in real life because it does not correspond to our observations,
where the infection generations overlap.
What is observed during the initial phase of a real epidemic is exponential growth
as follows:
I (t )  Ce rt
for some growth rate r > 0, constant C > 0 were,
I(t), is the prevalence, the number of cases notified up to time t,
The incidence, i(t), is the number of new cases per unit of time, which is
proportional to dI/dt and can be computed as follows:
T2
i(t )  pc i(t   )d
T1
Explanation (also ex 1.13):
New cases at time t result from contacts with individuals that are infectious. The
individuals that are infectious at time t were themselves infected maximally T2-T1
time ago. The infectious individuals make contact at rate c with success
probability p.
Draw picture of infectious!
Trying to solve r from the previous equation is rather difficult, therefore the
substitution below is used.
Substitute the Ansatz i(t )
the characteristic equation
 kert
T2
in the previous equation, then r should satisfy
1  pc e d
r
T1
Conclusion:
•
The above equation gives the exponential growth rate of the model
•
Whereas there is an explicit formula for R0, there is not one for r
•
r > 0 iff R0 > 1 and r < 0 iff R0 < 1
in words: there is growth in real time iff there is growth on a
generation basis
A high value of R0 does not necessarily imply a high value of r.
• R0 = pc(T2-T1) depends only on the difference T2-T1 (Δ T)
• in the equation for r the magnitude of T1 and T2 are important (r depends on
absolute values of T1 and T2)
Example (ex. 1.15):
Choose T1*, T2*, T1** and T2** such that T2*-T1*=T2**-T1**, for example, take
T1**=T1*+2 and T2**=T2*+2. Then R0* = R0** because delta T remains the same.
 r
 r (  2 )
Now draw the graph of
and e
then it can be seen that the growth
rate for the second one (the blue line) is bigger than for the other one, so r* < r**
e
Now take T2* slightly bigger, then
R0*>R0** and r* < r**
R0 depends on the length of the time interval
that individuals are infectious, r depends on
how fast after infection an individual
becomes infectious to others. (demographic
methaphor)
e-r(τ)
e-r(τ+2)
τ
Now we have answered two of our questions initially asked:
•
Does this cause an epidemic?
•
If so, with what rate does the number of infected hosts increase during the
rise of the epidemic?
One question still remains:
What proportion of the population will ultimately have experienced infection?
1.3. The final size
1.3.1 The standard final-size equation
In a closed population and with infection leading to either immunity or death, the
number of susceptibles decreases and must therefore have a limit.
• Will the number of susceptible be zero at infinity? or
• Will some fraction of the population never get infected?
sS/N
s ()
1  s()
the proportion s of susceptibles S in a total population of size
N
the proportion of susceptibles at the end of the outbreak
the final size of the epidemic; it gives the fraction of the
population that became infected sooner or later
Result: s () is a root of the final-size equation:
ln s()  R0 (s() 1)
For
R0  1  root s()  1
R0  1   root 0  s()  1
Conclusion:
• a certain fraction
• this fraction
s ()
escapes from ever getting the disease
s () is completely determined by R0
• the larger R0 is, the smaller the fraction
s ()
1.3.2 Derivation of the final-size equation
Ex. 1.21
S
I
R
the size of the subpopulation of susceptibles
the size of the subpopulation of infectives
the size of the subpopulation of removed
Force of infection

the probability per unit of time for a susceptible to
become infected, this is proportional to I
tranmission rate (the constant of proportionality of the force of infection)
Assumptions
•
Infected individuals become immediately infectious
•
Infected individuals have a constant probability per unit of time α to
become removed
The model used is a SIR model, also called compartmental model
S
dS
   SI
dt
dI
  SI  I
dt
dR
 I
dt
I

R
Since the population is closed,
SI R N ,
where N denotes the total population size.
Therefore one of the equations of the system is redundant.
Determine R0:
• infectious period 1/α
• transmission rate β
• # susceptibles in the beginning equals N
→ R0 = βN/α
Determine the (initial) growth rate r of the I population
The equation
dI
 ( S   ) I
dt
gives the initial growth rate if one replaces S by N.
So the initial growth rate
r  N  
If r = 0, then R0 =1
Threshold condition for Nthreshold = α/β.
If
• N < Nthreshold then R0<1
• N > Nthreshold then R0>1
It can be shown that

ln S  S  I

is a conserved quantity,
by concidering dI/dS and seperating variables (see page 182 of the book), this
quantity is indepent of time
Since this quantity is independent of time, assuming that R0 >1 when time runs
from   to   we have:


ln S ()  S ()  I ()  ln S ()  S ()  I ()


and
S ()  N
Both before and after the epidemic the number of infected will be zero, therefore:
I ()  0
and
I ()  0
Using the previous equations we get:


ln S ()  S ()  ln N  N


This identity can be re-written as:
S () N  S () 
ln

 1

N
  N

Realizing that
S (  )
s ( ) 
N
and
Results in the final size equation:
N
R0 

ln s()  R0 (s() 1)
Drawing the phase protrait of the reduced (S, I) system on page 16:
setting dS/dt = 0 gives nullclines: S=0 and I=0
dI/dt = 0 gives nullclines: I=0 and S = α/ß
Given that the conserved quantity always hold we can say:

ln S  S  I  C


I  ln S  S  C

This gives the phase portrait shown on page 185. The number of susceptibles at
the peak of the infection is at α/ß, since here the derivative of I while I  0
Overshoot phenomenon:
The root, s () , of the final size equation becomes smaller when N increases.
Why does the fráction of susceptibles at the end of the epidemic become smaller
with increasing population size? This is due to the overshoot-phenomenon:
When an epidemic starts with a larger number of susceptibles, the number of
infected at the peak of the epidemic will be very large. Large enough to infect a
huge number of susceptibles even though the epidemic is decreasing.
In exercise 1.21 (viii) The SIR model of page 15 is reformulated in terms of
fractions of individuals. It is important to pay attention to the dimensions of the
parameters and to think carefully about the new interpretation of them
Until now we have assumed that parameters p and c are constant. This need
not be true during a real epidemic.
Let’s introduce:
 p if T1    T2
A( )  
0 otherwise
Think of AIDS and influenza
In the last part of section 1.3.2, also assumptions regarding the contact rate (c)
are made more explicit and related to the validity of the final size equation.
Until now we have assumed that the contact rate is a constant. Does the final
size equation still hold when this is not the case, for example when the contact
rate is proportional to the population density?
It is shown that the final size equation hold when the disease doesn’t cause any
death, i.e that it interferes in no way with the contact process. Or if, the disease
has a high mortality, the final size equation hold when the contact intensity is
proportional to the population density.