Now the question arises whether R, the residual to be disposed in
the environment, can also be modeled as an input. Using the materials
balance, we obtain Y = F(Y + R, N) by replacing the variable M, i.e.,
output can be interpreted as an implicit function of R and N. Let us
call this function G. Then we get
(5) Y = G(R, N).
Using the properties of F, we can prove that G is defined on
[R.sup.2.sub.+] and has the usual properties of a production function
(all proofs have been relegated to an Appendix):
RESULT A: If, given the materials balance (1), F satisfies
Condition F, then a production function G (equation 5) exists and
satisfies Condition G,
which is given by
Condition G
(6a)
G is twice continuously differentiable on [R.sup.2.sub.+].
(6b) G(0, N) =0.
(6c) For every Y > 0 there is (R, N)
such that Y = G(R, N).
(6d) 0 < [G.sub.R] and 0 < [G.sub.N] for (R, N) >> 0.
(6e) G is strictly concave in (R, N)
for (R, N) >> 0.
Again, we have positive and decreasing marginal products and strict
concavity. Emissions R are a necessary input to production. In other
words, G is a production function and R can be interpreted as an input.
The material input is then determined by the materials balance M = Y + R
= G(R, N) + R. Thus, we obtain a formal justification of the view that
emissions can be modeled or interpreted as an input of the production
process. Two aspects need to be emphasized: First, the production
function G satisfies the standard properties of nonlinear production
functions. Especially, it can be of the Cobb-Douglas type (see below).
This fact is important compared to the first case in which the
production function F has to obey an additional, nonorthodox
restriction. Second, since the modeling is based on the materials
balance, another input, materials, is in the background which has to be
taken into account when describing the technology by means of the
function G. Consequences of these observations will be considered in the
"Discussion" section.
Since the marginal product of R is always strictly positive, we can
invert G for any fixed N and obtain an emission function
(7) R = H(Y, N).
R now depends on output Y and the nonmaterial factor. It is defined
on the domain D = {(Y, N) | Y [member of] y(N), N [member of]
[R.sub.+]}, where y(N) denotes the range of G for fixed N, i.e., y(N) =
{Y = G(R, N) | R [member of] [R.sub.+]}. The range y(N) can be a bounded
subset of [R.sub.+] since Y can be limited by N (e.g., in a chemical
production process the output Y can be limited by the reactor volume N).
We can establish:
RESULT B: If, given the materials balance (1), G satisfies
condition G, then an emission function H (equation 7) exists and
satisfies condition H,
which is given by
Condition H
(8a) H is twice continuously differentiable on D.
(8b) H(0, N) = 0. For every Y > 0 there is
N such that Y [member of] y(N).
(8c) For every Y > 0 there is N such that Y [member of] y(N).
(8d) 0 < [H.sub.y] and [H.sub.N] < 0 for (Y, N) >> 0.
(8e) H is strictly convex in (Y, N) for Y, N >> 0 (i.e.
[H.sub.YY] > 0, [H.sub.NN] > 0 and [H.sub.YY] [H.sub.NN] -
[H.sup.2.sub.YN] [greater than or equal to] 0).
In this case, emissions R increase in output Y and they increase at
an increasing rate. At the same time, emissions decrease in the
nonmaterial input N, and they decrease at a decreasing rate. Thus, H(Y,
N) is an emission and an abatement function simultaneously, where the
marginal abatement effect of N is decreasing. Intuitively, this reflects
the circumstance that in the function G(R, N), the input R can be
substituted by N, but only at a decreasing rate. The material input is
again determined by the materials balance M = Y + R = Y + H (Y, N).
Up to now, we have proved that the description of the technology by
means of (3) and the materials balance (1) also implies the
representations (5) and (7). It is not clear whether (5) or (7) also
imply the production function (3). Replacing R in (7) by means of the
materials balance one can demonstrate:
RESULT C: If, given the materials balance (1), the emission
function H satisfies Condition H, then a production function F (equation
3) exists and satisfies Condition F.
Thus, we obtain a "circle" and arrive again at the same
production function F we started from. The three representations of the
technology discussed here are equivalent.
Using the following terminology
Model F: Y = F(M, N), R = M - F(M, N), Condition F (equation 4),
Model G: Y = G(R, N), M = G(R, N) + R, Condition G (equation 6),
Model H: R = H(Y, N), M = Y + H(Y, N), Condition H (equation 8),
we can state:
THEOREM: Given the materials balance (1), environmental emissions
can be treated equivalently as a joint output of M in Model F, as an
input in Model G, and as a by-product of Y in Model H.
In other words, we have presented various descriptions of the
nonlinear production process and emissions. Furthermore, we have
demonstrated how to derive one from another. Since the representations
are equivalent, their information content is the same.
Discussion
In this section, we want to discuss the significance of the
framework presented above. We consider some implications and clarify the
relationship of our approach to the literature.
Consequences and Extension
Firstly, the imposition of the materials balance implies
restrictions on the functional form of feasible production functions
F(M, N). It is not an easy task to find such functions directly.
However, the results of the preceding section allow us to generate this
type of production function indirectly: Starting from a production
function G(R, N) with standard properties, we can try to recover F(M, N)
explicitly. The following example demonstrates this point:
Suppose that Y = G(R, N) = [R.sup.1/2][N.sup.1/2]. Inserting the
materials balance R = M - Y and solving for Y yields Y = F(M, N) = (MN +
[N.sup.2]/4).sup.1/2] - N/2.
This production function F(M, N) satisfies Condition F (equation
4). In particular, the marginal product [F.sub.M](M, N) is bounded by
unity (whereas [lim.sub.R [right arrow] 0][G.sub.R](R, N) = [infinity].
We can similarly derive the corresponding emission function R = H(Y, N)
= [Y.sup.2]/N. This example highlights, especially, that the
Cobb-Douglas form is admissible for G(R, N) but not for F( M, N).
Even if it is not possible to recover the function F explicitly,
using the function G(equations 6) and (1) assures that the basic
implications of the materials balance are respected. Thus treating
emissions as an input--as it is frequently done in the literature--is
not only an admissible, but also a convenient approach, as it avoids
finding appropriate functions F.
Secondly, our framework allows us to solve a problem, which is
often neglected: The literature in general employs the approach Y = G(R,
N) without referring to the materials balance. This formulation makes
sense when there is a strictly positive "price" [w.sub.R] of
emissions (e.g., a tax). But whenever [w.sub.R] = 0, it is optimal for a
firm to use an infinite quantity of R since its marginal product is
strictly positive by assumption (except in the case of fixed
coefficients, which we do not consider in this paper). Obviously, this
implication is unrealistic. In other words, in the usual framework, it
is impossible to explain the finite level of emissions in the
laissez-faire situation. This contradiction is solved if the materials
balance is imposed. Then the level of emissions R is bounded by the
quantity M and will therefore be finite if M has a positive price. More
specifically, the problem of profit maximization is well defined since R
is linked to M. For example, for Model G, we obtain the profit function
(9) [PI] = pY - ([w.sub.M] M + [w.sub.N] N + [w.sub.R]R) = pG(R, N)
- ([w.sub.M](G(R, N) + R) + [w.sub.N] N + [w.sub.R] R) = (p -
[w.sub.M])G(R, N) - ([w.sub.N]N + ([w.sub.M] + [w.sub.R])R)
where p denotes the price of Y and [w.sub.M] and [w.sub.N] are the
prices of M and N. Even if [w.sub.R] = 0, the accounting for the
materials balance implies that the firm has to "pay the price
[w.sub.M]" for R. We get an analogous result for Model H. Thus our
model is able to explain the finiteness of R.
Thirdly, our framework can be extended to the production of a
certain type of nonmaterial output, namely final energy. It is the type
of energy mentioned above as one of the nonmaterial inputs in the
production of desired material outputs. However, final energy (e.g.,
electricity) is itself in most cases the result of a transformation
process, namely the transformation of primary energy (e.g., coal). These
energy transformation processes obey, in addition to the materials
balance principle, the energy balance principle according to which the
primary energy input equals the final energy output plus the
transformation loss (all measured in energy units, e.g., Joules). By
redefining symbols appropriately (M = primary energy, Y = final energy,
R = transformation loss), the conditions (1) and (2) can hence
alternatively be interpreted as properties of processes that produce
final energy from primary energy (where Condition (1) in this case
stands for energy balance, rather than materials balance). These
processes, described by Y = F(M, N), also involve substitutability since
more final energy can be produced from a given amount of primary energy
by using more of the nonmaterial input (thus raising the transformation
efficiency). However, as in the case of material production, Y < M
and [F.sub.M] < 1 for M > 0.
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