The name is absent



Proposition 5 The optimal combined loading c approaches 2 [ — B] — r if σv → ∞

Proof: Recall the equation that implicitly defines c in Proposition 3 (using ∆σ2 = σ22 — σU21 )

k1



+r


1φ (⅜r )


■' φ(X-^ )

v      σv


[Bkr + 2Xcr + r2 + ∆σu2] = 0


Since 0 < Φ() < 1 and 0 < φ() < we know that c has to be bounded for σv ≥ 1. Hence,
Xc c is bounded as well and the ratio -c approaches zero for σv → ∞ and limσv→∞ c =

k Γ1 Ï2 "I      r

2 Lδ    Bi     2.

The intuition is as follows: as uncertainty in the random element of pollutant loading v in-
creases, the manager’s actions have less and less influence on which state the environmental sys-
tem will be in, and the probability that the system will be in either state approaches one half.
Thus, the optimal loading includes a term that approaches
r/2, representing the expected addi-
tional pollutant loading as
σv → ∞. The next period’s expected state variable again equals the
target level
2 [ɪ — B]. The right graph of Figure 1 shows that the next period’s expected state vari-
able approaches the flat horizontal line
2 [∣ — B] if σv increases. It is reasonable to ask whether
an increase in uncertainty
σv gives less incentive for precaution and always increases the optimal
loading. As the next proposition shows, such monotonicity of behavior is not found. To the con-
trary, for all possible parameter assumptions one can find a critical value
Xc such that an increase
in
σv will decrease the optimal loading, increasing precaution as uncertainty increases.

Proposition 6 For all values of parameters B, k, r, δ, and σv, there exists a critical level Xc such
that an increase in the variance σ
V2 decreases the optimal loading c.

Proof: We will show that there exists a critical level for which -dc- is negative. Consider Xc =
v

, [1 -Β]+2σ2-2rσv [1-Φ(1)]-φ(1)[Bkrr2∣∆σU]
2[
(1)∣σ, ]                       .

It is shown in the Appendix that the the optimal combined loading under these parameters is

------

= ф(1) and φ (⅛-r') = ф(1).


(⅛*)


cc = Xc — σv . This simplifies equations as Φ

Using this result in the derivative obtained after totally differentiating the equation that implic-

itly defines cc gives (for a derivation see the Appendix):

dcc


—rφ(1)

v


σv+φ(1) r+2σv [Bkr+


, [1 -B]+2σ,-2rσυ [1 -Φ(1)]-φ(1 )[ Bkr +-r2+∆σU ]


[(1)+σ, ]


r + r2 + ∆σu2]


10




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