
320 13. Perturbation Analysis of Matrix Models
where the contributions b
ij
can be written as the product of one term that
is a function only of i and another that is a function only of j (Caswell
1986).
The idea of a “contribution” must be interpreted carefully, since λ is
not actually composed of independent contributions from each of the a
ij
.
Consider the model for the human population of the United States, in which
the elasticity of λ to P
2
is 0.19 (Figure 13.5). We would say that survival
of age-class 2 contributes about 20 percent of λ. But if we eliminate this
transition, by setting P
2
= 0, we eliminate not 20 percent but 100 percent
of λ.WhenP
2
= 0, no one survives to reproduce and λ =0.Thusthe
“contributions” of the other vital rates to λ depend on the value of P
2
,and
vice versa.
Example 13.4 Elasticity in the desert tortoise
Figure 13.2 shows the elasticities of λ to changes in F
i
, P
i
,andG
i
for the desert tortoise (Doak et al. 1994). The total of the fertility
elasticities is only 0.043 (i.e., 4.3 percent). The elasticities to growth
(G
i
) sum to 25.8 percent and those to stasis (P
i
) sum to 69.9 percent.
The largest elasticity is e
77
; i.e., the elasticity of λ to the probability
(P
7
) of surviving and staying in size class 7.
Example 13.5 Elasticity in the teasel life cycle
Figure 13.6 shows the largest elasticities in the teasel life cycle (cf.
Figure 11.2). If the elasticities are interpreted as contributions, only
five arcs, shown by heavy arrows, contribute more than 5 percent to λ.
To a good approximation (73 percent of λ), the growth rate of teasel
can be described in terms of only three transitions: [flowering plants
→ medium rosettes → large rosettes → flowering plants]. Adding the
pathway [flowering plants → dormant seeds → large rosettes] adds
an additional 13 percent of λ.
13.2.3 Elasticities of λ to Lower-Level Parameters
The elasticity of λ to a lower-level variable x is
x
λ
∂λ
∂x
=
x
λ
i,j
∂λ
∂a
ij
∂a
ij
∂x
. (13.2.12)
This gives the proportional change in λ resulting from a proportional
change in x, but since there is no reason to expect that λ is a homoge-
neous function of x, the lower-level elasticities do not in general sum to 1,
nor can they be interpreted as contributions to λ.