Transcript materials

Predicting
Naturalization vs.
Invasion in Plant
Communities using
Stochastic CA Models
Margaret J. Eppstein1 & Jane Molofsky2
1Depts. of Computer Science and Biology
2Dept. of Botany
What makes some plant species invasive in some communities?
Lots of theories, e.g.:
Enemy Release Hypothesis
(Keane & Crawley, 2002)
Evolution of Increased Competitive Ability
(Blossey & Notzold, 1995)
Biotic Resistance Hypothesis
(Elton, 1958)
Propagule pressure (number and frequency)
(Von Holle & Simberloff, 2005; Lockwood et al, 2005)
Despite the many important advances in understanding potential
causes of invasiveness, it remains unclear how the various
ecological influences interact, or how to predict invasiveness.
Lots of recent evidence that local intra- and inter-specific
positive and negative feedbacks in plant communities
can drive population dynamics and affect biodiversity
(e.g, Wolfe & Klironomos, 2005; Reinhart & Callaway, 2006)
Pollinators (+)
Predators (-)
Symbionts (+)
Pathogens (-)
Soil chemistry (+ or -)
Emphasis has been on changes in feedbacks between
native and invasive ranges of a species
Standard Lotka-Volterra competition models
ignore frequency dependent feedback effects
on population growth rates
Nj

dNi
 ri  Ni 1    ij 1  d j 
dt
Ki
 j 1..s

  di Ni

Frequency independent
population growth rate
Classic theoretical ecology:
•Mean field assumptions (space ignored)
•Equilibrium conditions emphasized
We develop a model incorporating the influences of:
•propagule pressure,
•frequency independent components of growth,
•frequency dependent feedback relationships,
•resource competition, and
•spatial scale of interactions.
This model can be used to explore complex
influences of spatially localized frequency
dependence and competitive interactions on
population dynamics.
We extend standard Lotka-Volterra competition equations
Nj

dNi
 ri  Ni 1    ij 1  d j 
dt
Ki
 j 1..s

  di Ni

to include frequency dependent growth rates.
Nj 

  i    ij  ij
 Ki
Ki 
dN i
j 1.. s


dt


Nj 

Nk 
  ij N j 
  i    ij  ij
 N i      j    jk  jk
Ki 
Kj 
j 1.. s
j i  
k 1.. s


Nj

 N i 1    ij 1  d j 
Ki
 j 1..s

  di N i

In an example community of annual plants (di =1)
where competition is for space (Ki=Kj=Nk,k) and
all species require the same amount of space per
individual (ij=1), this reduces to:
Assume dispersal is
proportional to species density
Frequency
independent
component
t
H
 i 
where
i
Habitat quality
dNi

dt
H it Dit N i
t
t
t
H
D
F
 j j i
j 1.. s
t

F
 ij
j 1.. s
represents frequencydependent habitat quality
(nonlinear functions could be
Frequency
substituted here…)
dependence
j
Alternate model implementations:
deterministic
H, D computed over
Field for
the Mean
neighborhood
(4th order
Runge-Kutta)
each
cell
t
t
H
D
i
i
Fi t 1 
t
t
H
D
 j j
j 1.. s
stochastic
Mean Field
Local
Neighborhoods
(global neighborhood)
(overlapping 33 cells)
Spatially-Explicit Models
(Stochastic Cellular Automata)
100100 cells each
Probability of occupancy of a cell at next time step
Stochastic Cellular Automata Model (shown for 2 species)
Stochastic probability that cell at
Pi
t 1
x 
x is occupied by species i at time t+1
H it  x 
H1t  x 
1H
D1t  x 
Dit  x 
iH
1D
iD
 H 2t  x 
Species specific Interaction neighborhoods  i
2H
D2t  x 
2D
H
Species specific Dispersal neighborhoods 
D
i
x
Neighborhoods can vary in
size, shape, distribution
e.g., uniform square neighborhood
 of size 3  3
For the results shown here, we assume uniform
square neighborhoods of various sizes, that are
species-symmetric and same for dispersal and
frequency dependent interactions.
Habitat quality Hi
If maximum habitat quality is identical between two species…
Frequency Fj
…then invasiveness is a function of
relative net frequency dependence of species
and neighborhood size
(smallest absolute frequency dependence wins, but rate
of invasion also controlled by neighborhood size)
Summary of Invasiveness predictions by
frequency dependence 12 quadrants
+- Resident positive, Exotic negative:
Medium Invasiveness
Smallest scale highest invasion success
Smallest scale slowest invasion to extinction
0.5
M
0
L




-0.5
H
coexist
VH
-1
Smaller neighborhoods
-1
reduce region of co-existence
low
-0.5
-- Resident negative, Exotic negative:
Exotic becomes established and coexists.
0
22
+0.5
+1
invasiveness
+1
quadrant map
H M
11
Reddish shaded
regions show
where|1|>|2|,
so Species 2 has a
chance to invade.
++ Resident positive, Exotic positive:
Least invasive
Smallest scale highest invasion success
Smallest scale slowest invasion to extinction
medium
high
very high
-+ Resident negative, Exotic positive:
Most invasive region
Intermediate scale highest invasion success
Smallest scale fastest invasion to extinction
Example: Single propagule of exotic in +- quadrant
(invader negative)
  0.8,   0.1
11
Tight clusters of
invaders expand
22
+1
*
0.5
11
 
0
  
-0.5
33 cell 
-1
-1
-0.5
0
 22
Out of
100 trials
+0.5
+1
Average takeover
time for invader is
longest at shortest
scale
Invader wins
Resident wins
Example: Single propagule of exotic in -+ quadrant
(e.g. after enemy release; residents negative, exotic positive)
Loose clusters of
invaders expand
+1
0.5
11
 
0
-0.5
1111 cell 
-1
-1
  
*
Very invasive: even a
slight frequency
dependent advantage
promotes invasion
11  0.5,  22  0.4
Note long takeover times! Non-0.5
+1
equilibrium
important.
 0 +0.5 dynamics
22
Out of
100 trials
Average takeover
time for invader is
longer at larger scale
Invader wins
Resident wins
HOWEVER, if we also consider differences in frequency
independent components , the picture changes.
Again, consider 2 idealized species:
S1 (resident community) and S2 (introduced exotic)
As with Lotka-Volterra competition equations,
4 outcomes are possible.
Consider species’ population growth rates r:
t
r
Pop growth rate i 
Fi t 1
Fi
t
Outcomes are governed by the 4 possible combinations of
signs of the pop growth rate differences , at the two
frequency extremes (not the 4 possible  quadrants)
1  r1 F 0.99  r2 F 0.99
1
1
 2  r2 F 0.01  r1 F 0.01
1
1
growth rate
differences at
frequency extremes
11
a) 1122 ::  
b) 1122 ::  
22
11
11
22
Conditional Invasion
Extirpation of S2
c) 1122 :: 
d) 1122 :: 
22
11
11
22
Naturalization
22
Invasion
Given almost any of the four possible combinations of signs
of net frequency dependence (the 12 quadrants), it
possible to end up in almost any of the 4 possible
invasiveness classes (the 12 quadrants)!
Invasiveness outcome quadrant
Net feedbacks
12:+- 12:++ 12:-+ 12:-12:+-



12:++
12:-+
12:--











Where net feedbacks are: 1  11  12 ,  2   22   21
Even if the resident community has net negative feedback (1<0)
Specifically,
the invasiveness
outcomes
are determined
While the introduced
exotic has
net positive
feedback (by
2>0)
both frequency dependent
andenemy
frequency
independent
(e.g., following
release),
components
all interacting
species: are possible.
all 4ofinvasiveness
outcomes
sign( i )  sign(  j   jj   i   ij )
Invasiveness outcomes change with the relative average
fitness of the resident and exotic.
Unstable equilibrium pt
H i is the habitat
(conditional invasion) suitability averaged
H1  H 2
Invasiveness is very sensitive
to perceived propagule
pressure
H1  H 2
H1  H 2
over all frequencies
H1  H 2
H1  H 2
a)
b)
c)
d)
e)
f)
g)
h)
i)
j)
Exotic is less fit
S1still
wins
but can
establish
(extirpation
of S2)
Although in naturalization
Stableexotic
equilibrium
pt
quadrant,
is still a threat
(naturalization)
S2 wins
(invasion)
Histogram of perceived propagule pressure
in cells with at least one propagule in its neighborhood
a)a)
Conditional
Invasion quadrant
9 propagules
introduced
b)
b)
Meanfield (M):
Can’t Invade
c)c)
Scattered (S):
Stochastic invasion
d)
d)
Clumped (C):
Likely to invade
Likelihood of early extirpation of exotic either increases or decreases
with perceived propagule pressure, depending on the quadrant.
Growth rate of exotic increases with its frequency
(in conditional invasion quadrant)
Growth rate of exotic decreases with its frequency
(in naturalization and invasion quadrants)
(Black arrows indicate direction of increasing perceived propagule pressure.)
Measure growth rates Experimental
in existing patches
of different
System:
densities of Phalaris, in both
native
and grass
introduced ranges.
Reed
Canary
Phalaris
This may be a practical
way arundinacea
to assess invasive
native to
Europe,
potential of newly introduced
exotic
plants, and/or to
invasive
in N. American
wetlands.
estimate range limits
of invasive
species.
Should predict
invasion quadrant
Should predict
naturalization quadrant
Conclusions
•Both frequency dependent and independent interactions have a big impact on
invasiveness.
•Its not the change in interactions from native to introduced ranges that
determines invasiveness, but the relative frequency dependent growth rates of
exotic as compared to resident community.
•Spatial scale of interactions dramatically affects community structure and
population dynamics.
•Understanding cluster formation and density and the relative inter and intraspecific dynamics in the interiors, exteriors, and boundaries of self-organizing
clusters of con-specifics can provide insights into mechanism governing
invasiveness.
•Importance of non-equilibrium dynamics in invasiveness; time scales of
environmental change may exceed time to equilibrium.
Conclusions continued…
•Measuring relative growth rates in small patches with different
frequencies of exotic species may help to predict invasiveness and/or
range limits of invader.
•We have developed a stochastic cellular automata model that facilitates
study of complex influences of spatially localized frequency dependent
and competitive interactions.
For more details:
Eppstein, M.J. and Molofsky, J. "Invasiveness in plant communities
with feedbacks". Ecology Letters, 10:253-263, 2007.
Eppstein, M.J., Bever, J.D., and Molofsky, J., "Spatio-temporal
community dynamics induced by frequency dependent interactions",
Ecological Modelling, 197:133-147, 2006.