A MEAN FIELD MODEL FOR THE DEVELOPMENT OF RENEWABLE CAPACITIES CLÉMENCE ALASSEUR MATTEO BASEI CHARLES BERTUCCI AND ALEKOS CECCHIN

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A MEAN FIELD MODEL FOR THE DEVELOPMENT OF RENEWABLE
CAPACITIES
CLÉMENCE ALASSEUR, MATTEO BASEI, CHARLES BERTUCCI, AND ALEKOS CECCHIN
Abstract. We propose a model based on a large number of small competitive producers of
renewable energies, to study the effect of subsidies on the aggregate level of capacity, taking
into account a cannibalization effect. We first derive a model to explain how long-time equi-
librium can be reached on the market of production of renewable electricity and compare this
equilibrium to the case of monopoly. Then we consider the case in which other capacities of
production adjust to the production of renewable energies. The analysis is based on a master
equation and we get explicit formulae for the long-time equilibria. We also provide new numer-
ical methods to simulate the master equation and the evolution of the capacities. Thus we find
the optimal subsidies to be given by a central planner to the installation and the production in
order to reach a desired equilibrium capacity.
1. Introduction
As electricity production is responsible for around a third of worldwide CO2emission, its
decarbonization is of course a huge challenge. As such, the share of electricity produced from
renewable capacities such as hydro, wind, photovoltaic is widely growing. However, to achieve
decarbonization objectives, this share must still grow in a very large proportion. In 2021, the
share of all renewable production had reached 30%1. But many new investments are required
in order to achieve a net-zero economy by 2050 as 90% of global electricity generation should
come from renewable sources at that point2.
Electricity market is characterized by the constraint that production must be equal to the
consumption at any time. In case of non respect of this constraint, the system can incur a power
outage whose consequences might be highly problematic. For example, the total economic cost
of the August 2003 blackout in the USA was estimated to be between seven and ten billion
dollars [15]. As electricity can hardly be stored, hydro storage is limited in size, and developing
a large fleet of batteries is still highly costly, the power production capacity must be high enough
to cope with major peak load events, which can reach extreme levels compared to the average
load. The consequence of such constraints on the production system is that some power plants
are used rarely (only during extreme peak load) but remain necessary for the system security,
and insuring their economical viability with energy markets only is not guaranteed. This ques-
tion has already motivated a great amount of economic literature under the name of missing
money [19]. That’s also why some regulators took the lead on this matter through "strategic"
reserves (see for example [10]) or by the design of capacity remunerations (see for example [12]
for a review of theoretical studies and implementations of capacity remuneration mechanisms).
Renewable energies have low variable costs so their introduction has made electricity prices
lower, see for example [11] or[21]. This effect is also sometimes referred as the cannibalisation
Date: May 20, 2023. Second version.
2020 Mathematics Subject Classification. 91A16, 91B50, 49N80.
Key words and phrases. Energy transition, mean field equilibrium, master equation, optimal incentives.
C. Alasseur acknowledges support from FIME and ANR ECOREES (project ANR-19-CE05-0042). C. Bertucci
acknowledges a partial support from the FDD Chair. A. Cecchin benefited from the support of LABEX Louis
Bachelier Finance and Sustainable Growth (through project ANR-11-LABX-0019), ECOREES ANR Project,
FDD Chair and Joint Research Initiative FiME.
1https://www.iea.org/reports/global-energy-review-2021/renewables
2https://www.iea.org/reports/net-zero-by-2050
1
arXiv:2210.15023v2 [math.OC] 25 May 2023
2 CLÉMENCE ALASSEUR, MATTEO BASEI, CHARLES BERTUCCI, AND ALEKOS CECCHIN
effect (see [23]). This could reinforce the lack of incentives to invest in new capacities. To which
level and at which rhythm new renewable capacity would develop in electricity markets is a
key issue to regulators. Indeed, regulators can remove barriers by modifying the market design
such as the rules of the markets, the level of competition or by providing financial incentives to
the new capacities. The model we develop in this paper intends to provide explicit elements to
guide regulators in such issues.
We based our model on MFG (Mean Field Games) approach to represent numerous renew-
able producers who can decide to invest in new capacities. The use of MFG to analyse power
system is not new. For example, it has been used to study how consumers can optimise their
flexilibities against a dynamic price, see [14] for EV (Electrical Vehicle) charging, [16], [18] or
[5] for micro-storages or [17] or [7] for TCL (Thermostatic Control Load).
MFG are dynamic games involving an infinite number of small players. Such problems have
been studied for a long time in Economics and a mathematical framework has been proposed
in [20, 22]. One of the key feature of the MFG theory is that it provides a tool to analyze the
effect of an aggregate shock (or common noise) on the system, by means of the so-called master
equation. When it is well posed, this equation, usually set on the set of probability measures
[13], contains all the information on the MFG. In several situations, the master equation can
be posed on a finite dimensional space [8],[9] and it is thus easier to study. In this paper, we
adopt a framework which is similar to the one of [9]. In particular we shall study a master
equation whose derivation relies on the expression of dynamical equilibria on markets, even if
no precise MFG is introduced. This type of approach is quite natural in Economics like for
example equations which result from no-arbitrage assumptions. Indeed, in those situations, it
is not necessarily the mathematical problem of the arbitrageurs which is important but rather
the equilibrium relations that it implies.
In this paper, we analyse the long-term competition between producers who invest in re-
newable assets taking into account the cannibalisation effect. Moreover, we study the effect of
subsidies on the aggregate level of capacity of production of renewable energies. We adopt a
master equation formulation as in [9]. For a given level of subsidies, we are able to explicitly
characterise the level of capacities which would develop within the competition framework and
compare it to the level of renewable capacities achieved in a monopoly setting. The equilibrium
we obtain is explicit but also unique and our model provides a way to analyse the impact of
the level of subvention. We prove that competition strengthens the development of renewable
achieving a larger total renewable capacities and diminishes the profitability of producers com-
pared to a non-regulated monopoly setting. Numerically, we can analyse the rhythm at which
renewable develops and how fast a given renewable capacity target can be achieved. We are also
able to compute the optimal levels of subsidies for a central planner wants to achieve a target
of renewable capacity while saving the distributed subventions. In particular, we demonstrate
that from a regulator point of view, to subsidize the cost of production as a decreasing amount
of installed capacities is more efficient than keeping a fixed subvention over time. We provide
this study in two cases: one in which the renewable energies are the only adjustable capacities
of production on the market and one in which the other capacities of production, the reserve,
adjust to the production of renewable energies. When the strategic reserve adapts to the level
of renewable capacity, we show in the paper the explicit and unique equilibrium of competitive
and monopoly situation.
Mathematically, this problem can be named as the one of controlling a MFG equilibrium.
Even though this problem seems quite natural from the point of view of applications, it has
received only few attention for the moment. This may be due to the intrinsic difficulty of the
problem, that we shall not enter in in this paper. Here, we shall restrict ourselves to our par-
ticular problem and illustrate the results we obtain with numerical simulations.
A MEAN FIELD MODEL FOR THE DEVELOPMENT OF RENEWABLE CAPACITIES 3
The rest of the paper is organized as follows. In Section 2, we introduce and study a simple
model in which the capacity of electric production outside the renewable source is fixed. In
this setting, we develop the case with a constant subvention to the production and also with a
decreasing subvention with the total renewable capacity. In Section 3, we then proceed to study
the more involved case in which this capacity evolves with the installed capacity of renewable.
2. Renewable capacity development with fixed reserve
2.1. A first general model. Assume that we have a multitude of producers of a renewable
energy, that they are symmetric and non-atomic in the sense that every one of them is too small
to have an influence on the market. Assume that the total (aggregate) available capacity of
renewable energy Kt(in MW) at time t(in years) evolves according to
˙
Kt=δKt+Xt.(1)
The parameter δ > 0is given and represents the decay of old installations due to time (in
years1). The quantity Xtis the variation of capacity, at time t, induced by the behaviour of
the producers. Let Ptbe the market remuneration assimilated at the spot price in e/MWh and
assume that it depends on the total (aggregate) available capacity Ktin a decreasing way:
Pt=p
Kt+ε,(2)
where εis a fixed parameter in MW and pa constant in e/h. This model for the spot price is
directly inspired by structural approaches to model electricity prices, such as models developed
in [6] or in [3], which represent spot prices as the intersection of the production and demand
curves in a stylised way. Because, in our model, the new capacities Xare renewable technolo-
gies with very low cost of production, large introduction of this type of technology mechanically
decreases the spot price most of the time.
Let ctbe the cost of production, in e/MW, at time t. We introduce also a parameter h
(in hours/year) which accounts for the number of hours of production of the renewable energy,
per year. Indeed, renewable technologies have the particularity to depend on meteorological
conditions and as such do not run at full capacity all the time.
We want to characterize the value of a single unit of production at time t, which we denote
by ut. Note that, equivalently, it represents the value of the "game" for a producer detaining a
single unit of production at time t. From the previous assumptions, we can write utas the sum
of the expected payments given by a unit of production, before it defaults, which happens at
rate δ > 0. This yields (denoting by a+the positive part of a)
ut=E"Zτt
t
er(st)hp
Ks+εcs+
ds#.(3)
The random variable τtis an exponential random variable of parameter δ1which models the
time at which the unit of production will default.
The strategic equilibrium which takes place in our model can be seen through the link be-
tween the equations (3) and (1). Indeed to compute the value of a unit of production, we need to
have anticipation on the evolution of the future total capacity installed. But on the other hand,
the evolution of the total capacity installed should depend on the value of a unit of production:
the more profitable the production of renewable, the more capacity should be installed. To
make this link more apparent, we make the assumption that Xtis a function of only the time t,
the aggregate capacity of production Ktand the value utof a unit of production, and we write
Xt=F(t, Kt, ut). We shall come back on this assumption later on.
4 CLÉMENCE ALASSEUR, MATTEO BASEI, CHARLES BERTUCCI, AND ALEKOS CECCHIN
The previous assumption hints to seek utas a function of only tand Ktwhich we note
ut=U(t, Kt). This leads to a sort of dynamic programming formulation for utwhich takes the
form
U(t, Kt) = E"Zt+dtτt
t
er(st)hp
Ks+εcs+
+{t+dt<τt}U(t+dt, Kt+dt)#,
for dt > 0. Assuming that ct=c(t, Kt), simply computing d
dt U(t, Kt), applying the chain rule
and using (1) and the above equation, we find that Ushould solve the PDE
tU(t, k)+(F(t, k, U(t, k)) δk)kU(t, k)(r+δ)U(t, k) + hp
k+εc(t, k)+
= 0 (4)
on the domain (t, k)(0,)×[0,). Note that the previous equation is backward in time,
that no boundary condition is needed at t=because of the presence of the discount factor
rand that no boundary condition is needed at k= 0 provided that F(t, 0, U(t, 0))) 0. In the
terminology of the MFG theory, this PDE is the master equation of the problem.
Let us note that the well-posedness (existence and uniqueness) of the previous PDE yields
the existence and uniqueness of an equilibrium in our model. Indeed, if we are able to compute
Uthrough (4), then we can also compute the evolution of Ktthrough (1). We stress that (4)
is not the master equation of a mean field game, because Udoes not represent the value of
an agent in a Nash equilibrium, but the value of a unit. Instead, in our model, (4) is simply
derived by the chain rule, and we call it master equation because it has the same mathematical
structure of the mean field game master equation (in one space dimension), so that we easily
get well-posedness results. It is in fact an equation for the value of a unit in equilibrium, but
not a game, and the sole fact we use of MFG theory is the idea that producers are non-atomic
(or small), as explained above.
Equilibrium with a large number of competitive producers. We now make two
assumptions to make the precedent model more tractable and get, in particular, an explicit
expressions for the equilibrium capacity. We assume first that the model is stationary, that is
that no quantity depends explicitly on the time variable. This leads to the master equation
(r+δ)U(k)+(F(k, U(k)) δk)kU(k) + hp
k+εc(k)+
= 0 (5)
which thus reduces to a singular ODE since only one variable is remaining.
We now make the more crucial assumption that, for some constant λ > 0and function
α:R+R,
F(k, U) = λ(Uα(k)).(6)
Remark 1. This assumption has the important property that higher the value of a unit of
production, the higher is the installation of new capacity and is justified by the following model.
We now present a simple model with Nsmall competitive producers to justify the equations
(6) and (5) when Nis large. Consider a producer whose capacity of production in (MW) at
time tis given by St. Let
α(k)be the cost of installation, in e/MW, given the installed (aggregate) capacity k
βNbe an adjustment cost, in eyear/MW2which represents a friction to large volume
of installation.
We shall come back later on why it is natural that βdepends on the number Nof producers.
These costs depend on the type of the production technology. Later, we will consider the
possibility for a central planner of subsidizing the cost of production cand the cost of installation
α.
We assume that the producer controls its (new) installed capacity Stthrough
˙
St=δSt+yt
A MEAN FIELD MODEL FOR THE DEVELOPMENT OF RENEWABLE CAPACITIES 5
where (yt)t0is its control, which represents the intensity of installation, in MW/year. Its
reward is then Z
0ertSthp
Kt+εc(Kt)+
α(Kt)ytβNy2
tdt. (7)
which is in infinite horizon with a discount factor rand, at every time t(in years) given by the
spot price minus the cost of production, multiplied by the capacity Stand the hours per year
of production h, while it pays the installation cost, multiplied by the intensity of installation,
and an adjustment cost.
We assume, as above, that the producer neglects the impacts its production has on the
aggregate production Kt, meaning that is is small compared to the total multitude of producers
(as in mean field models). This implies, in particular, that Ktis treated as a function of time
only in the maximization of the above reward. The maximization problem, in infinite horizon,
is easily solved by means of Pontryagin’s maximum principle: the Hamiltonian is
H(S, y, v)=(δ+S)v+Sh p
Kt+εc(Kt)+
α(Kt)yβNy2,
where vis the adjoint variable, which solves the ODE ˙v=H
S +rv and the optimal control
maximized the Hamiltonian. Thus the adjoint equation associated to this problem is given by
˙vt=δvthp
Kt+εc(Kt)+
+rvt(8)
and the maximization leads to
yt=vtα(Kt)
2βN
,(9)
which does not depend on St. From (8), expressing vt=V(Kt)as a function of Kt, we then
deduce (using the chain rule) that
(r+δ)V(Kt)+( ˙
Kt)kV(Kt) + hp
Kt+εc(Kt)+
= 0.
On the other hand, we can compute the evolution of the aggregate capacity Ktas the sum of
the evolution of the capacity of all players. Let Stbe the new aggregate available capacity of the
total multitude of producers, i.e. St=PN
i=1 Si
t, with S0= 0, thus the total available capacity
is
Kt=St+k0eδt,(10)
so that K0=k0is the initial capacity. This leads to
˙
Kt=Nytδ
N
X
i=1
Si
tδk0eδt
=NV(Kt)α(Kt)
2βN
δKt.
Assuming that, in the limit N→ ∞,βNscales as Nβ for some β > 0, we finally obtain that
˙
Kt=V(Kt)α(Kt)
2βδKt.
Hence, setting λ= (2β)1, we recover the required form F(k, U) = λ(Uα(k)).
Remark 2. Recall that in this Nplayers framework, βNis an adjustment cost. Hence it is
natural that this cost grows with the number of producers (or at least of active producers) in the
model. Indeed if βNis small, then the adjustment cost is also small and we can expect that a
few big producers can adapt their production optimally quite easily. However, as βNgrows, this
adjustment becomes more and more important and the slowness of the producers to adjust allow
rooms for smaller producers to install some small, non zero, capacity of production. Somehow
this is what the relation (9) yields.
摘要:

AMEANFIELDMODELFORTHEDEVELOPMENTOFRENEWABLECAPACITIESCLÉMENCEALASSEUR,MATTEOBASEI,CHARLESBERTUCCI,ANDALEKOSCECCHINAbstract.Weproposeamodelbasedonalargenumberofsmallcompetitiveproducersofrenewableenergies,tostudytheeffectofsubsidiesontheaggregatelevelofcapacity,takingintoaccountacannibalizationeffect...

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