Добавил:
Upload Опубликованный материал нарушает ваши авторские права? Сообщите нам.
Вуз: Предмет: Файл:

UnEncrypted

.pdf
Скачиваний:
11
Добавлен:
16.05.2015
Размер:
6.75 Mб
Скачать

Proceedings of the 12th International Conference on Computational and Mathematical Methods in Science and Engineering, CMMSE 2012 July, 2-5, 2012.

Taking Care of the Singularities in the

Probabilistic Evolutionary Quantum Expectation

Value Dynamics

N.A. BAYKARA

1

˙

˙

2

 

and METIN DEMIRALP

 

1 Department of Mathematics, Marmara University

2 Informatics Institute, Istanbul Technical University

emails: nabaykara@gmail.com, metin.demiralp@gmail.com

Abstract

This work is somehow the extension of the work to be presented by Metin Demiralp in this conference. Purpose is the same as before, to get an infinite set of ODEs over the expectation values of the state vector’s outer powers. Almost completely same strategy is followed here. The basic di erence requesting extension is the singularity in the commutator of the state vector with the system Hamiltonian. The analyticity in this commutator is missing and the related problems are bypassed by defining inverse outer powers of the state vector.

Key words: Probabilistic Evolution Equations, Quantum Expected Values, Singular Hamiltonians.

1Introduction

Probabilistic Evolution Equations [1] and their solution is a quite new approach to solve ODEs, and also PDEs via expectation values as long as they can be defined. This approach extends the space to an infinite one by using the integer outer powers of the state vector. Then an infinite set of ordinary di erential equations (ODEs) is constructed such that it is linear and has an infinite constant coe cient matrix. This facilitates the theory however at the expense of dealing with infinitely many items. Curious readers can refer certain new resources [2, 3] on this topic.

c CMMSE

Page 153 of 1573

ISBN:978-84-615-5392-1

Taking Care of the Singularities ...

 

start with the definition of the expected value of a given operator O as follows

We d

O (t)

 

 

 

 

i

 

 

 

"

 

#

i

 

 

 

 

$

 

 

 

 

 

V

 

 

 

 

 

 

 

 

 

 

dt

V

 

 

!

 

 

 

 

 

!

 

 

 

 

 

ψ (x, t) =

 

 

 

 

(1)

 

=

d ψ (x, t)

HO

 

OH

 

 

HO

 

OH

 

V where H and ψ (x, t) stand for the system Hamiltonian and the wave function while and

dV denote the spatial volume of the integration and the infinitesimal volume element respectively. This equality’s dependence on the operator under consideration disables universality. Hence, it better to deal with the state vector whose elements are operators like positions and momenta, instead of this operator. We define the state vector denoted by s as follows

s [ s1 ... sn ]T

 

(2)

state vector’s outer square (outer or Kro-

where n denotes the “System’s dimension. The

 

 

necekr product with itself) is given explicitly below

 

 

s 2 s s % s1sT ... snsT &T .

 

(3)

This can be extended to the following general formula

 

 

s m s s (m−1) ≡ s1s (m−1)T ... sns (m−1)T ! ,

m = 0, 1, 2, 3, ...

(4)

where the mth outer power of the state vector has nm number of elements. The zeroth outer power is defined as the universal scalar, just 1 (that is, it is a single element vector).

The state vector’s expected value satisfies the following equation

 

 

 

d s (t)

=

i

Hs sH

!$

(5)

 

 

 

 

 

We assume

 

 

dt

#

 

 

 

 

 

i

 

sH !

 

 

 

 

 

Hs

j=0 Hj s j

(6)

 

 

 

 

 

 

 

j

 

 

 

where Hj is a rectangular matrix of n × n type. (5) can be extended to the outer powers

by using certain properties of the outer product together with the matrix product to get

 

d

s j

(t)

Ej,

s (j−1+ )

(t), j = 0, 1, 2, ...

(7)

'

dt(

 

= =0

 

 

 

 

 

 

 

 

 

where

 

 

 

j−1

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Ej, I k H I (j−1−k).

(8)

k=0

c CMMSE

Page 154 of 1573

ISBN:978-84-615-5392-1

 

 

 

 

 

 

˙

 

 

 

 

 

 

 

 

 

 

 

 

 

 

N.A. BAYKARA, Metin DEMIRALP

 

 

 

 

 

 

 

 

 

 

 

If we define

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

E0,0

· · ·

E0,m

· · ·

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

.

 

.

 

.

 

'

(

 

T

'

(

 

T

 

 

!

T

 

 

.. ...

..

.

..

 

(t)

 

(t)

 

...

 

,

E

.

.

.

 

 

(9)

ξ(t) s 0

 

 

s 1

 

 

 

Em,0

· · ·

Em,m

· · ·

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

..

..

..

 

..

 

 

then we obtain

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

(t)

= Eξ(t)

 

 

 

 

 

 

(10)

 

 

 

 

 

 

 

 

 

dt

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

which is an infinite set of ODEs whose coe cient matrix E is composed of constant elements. The second block element of its solution gives the sought expected value of the state vector. The solution can be formally written as

 

 

 

ξ(t) = etEξ(0)

 

 

 

(11)

where

 

ξ(0)

's 0(

(0)T 's 1(

(0)T ...

!T

 

 

 

(12)

and

's m(

(0) V dVψ0 (x) s mψ0 (x) ,

m = 0, 1, 2, ...

(13)

We find this information su cient for our purposes here. Further details can be found in Metin Demiralp’s paper[Ref] in this conference.

2Singularities in the Hamiltonian

The Probabilistic Evolution Philosophy is based on the inspiration from the analyticity and therefore Taylor series. However this inspiration remains applicable only when the system’s Hamiltonian has no singularities. Since the Hamiltonian’s dependence on the momenta are rather polynomial its position dependent part, that is, the potential gains a lot of importance for the singularities. If the potential function has singularities somewhere in the complex plane of the spatial variables then it a ects the solution of the Schr¨odinger equation and therefore the expected values. This means that (6) remains no longer valid. It must be replaced by something di erent. In the case of polar singularities Taylor series are replaced by Laurent series which has inverse powers of the independent variable or its deviation from a fixed reference point, together with the nonnegative powers. This inspires us to introduce the inverse outer powers of the state operators. We define

s (1)

1

 

... sn1 &

(14)

n % s11

 

 

 

 

 

 

c CMMSE

Page 155 of 1573

ISBN:978-84-615-5392-1

Taking Care of the Singularities ...

hence the transposition operation helps us to realize the outer inversion. We have

s (1) s j = s (j−1),

j = 0, ±1, ±2, ...

(15)

which urges us to assume

 

 

 

 

 

i

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Hs

sH

! j=−∞ Hj s j

(16)

where the coe cients are in the abstract operators mapping related outer power to a vector space where s lies.

This assumption and the abovementioned extensive definitions permits us to construct an infinite set of equations as follows

 

 

 

 

(t)

= Eξ(t)

 

 

 

 

 

 

(17)

 

 

 

 

 

dt

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

where

 

 

 

 

 

 

 

 

 

 

 

 

 

 

E(1,1)

E(1,2)

 

 

 

 

 

T

 

 

T

T

 

E /

0

, ξ(t) / s(1)

(t)

s(2)

(t)

0 .

(18)

E(2,1)

E(2,2)

 

 

3Conclusion

In the last three equalities the entities superscripted by integers between parantheses are all infinite blocks whose types are compatible to what we have said above. (17) again corresponds to an infinite set of ODEs. However, this time, the indexing of the infinite entities are not only on the nonnegative integers but over all integers. This, of course, complicates the issue a little bit more even though it is still possible to construct truncation approximant. However, this time truncation is not only downward, it is both upward and downward. More information will be given in the presentation and also in the relevant paper.

References

[1]M. Demiralp, Quantum Expected Value Dynamics in Probabilistic Evolution Perspective, CMMSE2012 Proceedings (this conference)

[2]M. Demiralp, E. Demiralp, L. Hernandez-Garcia, A probabilistic foundation for dynamical systems: theoretical background and mathematical formulation, J. Math. Chem. 58 (2012) 850-869. 2012.

[3]E. Demiralp, D. Demiralp, L. Hernandez-Garcia, A probabilistic foundation for dynamical systems: phenomenological reasoning and principal characteristics of probabilistic evolution, J. Math. Chem. 58 (2012) 870-880.

c CMMSE

Page 156 of 1573

ISBN:978-84-615-5392-1

Proceedings of the 12th International Conference on Computational and Mathematical Methods in Science and Engineering, CMMSE 2012 July, 2-5, 2012.

Real-time optimization of wind farms and fixed-head pumped-storage hydro-plants

L. Bay´on1, J.M. Grau1, M.M. Ruiz1 and P.M. Su´arez1

1 Department of Mathematics, University of Oviedo, Spain

emails: bayon@uniovi.es, grau@uniovi.es, mruiz@uniovi.es, pedrosr@uniovi.es

Abstract

In this paper we analyze whether real-time compensation of wind power plant deviation penalties is profitable by means of the coordinated optimization of the wind power plant with a pumped-storage hydro-plant. We shall make use of optimal control techniques to carry out the optimization. We shall also analyze another possible solution based on compensation carried out a posteriori, instead of in real time.

Key words: Optimal Control, Pumped-Storage Plant, Wind Farm

MSC 2000: 49J52, 49M05

1Introduction

The new regulations allow wind farms to go to the market to sell the energy generated by their facilities. If wind farms o er in the pool, they will prepare their o ers and schedule their power production. However, a major problem exists: the unpredictability of wind farm production. Forecasting errors lead to the wind farm incurring financial losses, known as deviation penalties. Diverse methods have also been proposed to store this energy [1]. In this paper we focus on combined use of a wind farm with pumped-storage plants.

Some authors ([2], [3]) have researched the operation of a wind farm cooperating with a micro-hydroelectric power plant and a pumped-storage hydro-plant. Previous studies exclusively employ the storage ability to compensate for wind power imbalances. However, this approach is not representative for large pumped-storage plants in power systems. One of the techniques used for large pumped-storage plants ([4], [5]) is to calculate the optimal amount of spinning reserve that the system operator should provide so as to be able to

c CMMSE

Page 157 of 1573

ISBN:978-84-615-5392-1

Real-time optimization of a wind-hydro power plant

respond to errors in forecasts. The combined operation of wind farms and a pumped-storage hydro-plant is also analyzed in [6].

The present paper aims to calculate the optimal operation of the pumped-storage plant, simultaneously pursuing two goals: to maximize revenue in conventional operations in the day-ahead market and to coordinate with the wind power producer with the aim of partially compensating for wind power imbalances. In this paper we shall consider a large capacity pumped-storage working jointly with a wind farm adjacent to its facilities. We shall consider them to be a single unit (a wind-hydro power plant). Two di erent joint configurations for the resulting joint-unit formed by the pumped-storage plant and the wind farm are considered. In the first (uncoordinated operation), the pumped-storage plant does not compensate for the errors due to forecasting wind power. In the second (coordinated operation), we shall attempt to compensate for these errors in real time. We shall see in this paper that the fact that the pumped-storage plant is a fixed-head plant will mean that the optimal solution is of a very special type: bang-singular-bang. This will have crucial consequences in coordinated operation and we shall present a qualitative study of the realtime compensation of forecasting errors. In view of the result obtained in this study, we shall propose a second solution: to employ the over-generation deviations of the wind power plant a posteriori to pump water into the upper reservoir of the pumped-storage plant, thus increasing profits. Finally, we present a realistic example.

2Problem description and model overview

The day-ahead market in the Spanish wholesale electricity market is organized as a set of twenty-four simultaneous hourly auctions. The simple bid format consists of a pair of (hourly) values: quantity q (MW h) and price p (euro/MW h). The problem we shall solve is the one faced by a wind-hydro power plant when preparing its o ers for the day-ahead market. This basic scheduling, with plants working independently, is based on the volume of water b m3 that must be used and on the best forecast of wind power generation available each hour W f (t)(MW ). Unfortunately, wind power forecasts within a 14 38 hour time horizon are usually highly inaccurate and hence incur deviation penalties.

As regards the pumped-storage plant, we shall model it in great detail without any additional simplifications. For a large capacity reservoir, the e ective head is constant over the optimization interval and here the fixed-head hydro-plant model is defined. In plants of this type, the active power generated, P (MW ), is represented by the linear equation: P (z (t)) = Az (t), where A represents the e ciency and diverse parameters related to the geometry of the hydro-plant (see [7]) and z (m3/s) is the rate of water discharge. Taking into account the conversion losses of the pumping process, we must therefore introduce the e ciency, η, in the model.

We consider z (t) to be bounded by technical constraints: qmin ≤ z (t) ≤ qmax, t [0, T ]

c CMMSE

Page 158 of 1573

ISBN:978-84-615-5392-1

L. Bayon,´ J.M. Grau, M.M. Ruiz, P.M. Suarez´

and we assume that b is the volume of water that must be discharged over the entire optimization interval [0, T ], so: z(0) = 0, z(T ) = b. The function P is thus defined piecewise

as:

A · z

 

z ≥ 0

 

P (z ) := (

if

(1)

η · A · z

if

z < 0

3Optimization of a fixed-head pumped-storage plant

In a previous paper [8] by the authors, we presented an algorithm that allows the optimal solution of a fixed-head pumped-storage plant to be obtained. The objective function is given by hydraulic profit over the optimization interval, [0, T ]. Profit is obtained by multiplying the hydraulic production of the pumped-storage hydro-plant by the clearing price, π(t), at each hour, t. An Optimal Control problem can thus be mathematically formulated as follows:

 

T

 

 

T

max

#0

L(t, z(t), u(t))dt = max

#0

π(t)P (u)dt

(u,z)

(u,z)

(2)

z = u;

z(0) = 0, z(T ) = b; umin ≤ u(t) ≤ umax

For the Optimal Control problem (2), we define the Hamiltonian in normal form:

H(t, z, u, λ) := L(t, z, u) + λu = π(t)P (u) + λu

(3)

and the resulting Hamiltonian, H, is linear in the control variable, u. It is well known [9] that when the Hamiltonian is linear in u, the optimality condition leads to the optimal u being undetermined if the switching function Φ(x, λ) ≡ Hu = 0. An added complication arises in our problem: the Hamiltonian is defined piecewisely and the derivative of H with respect to u (Hu) presents discontinuity at u = 0. When non-di erentiable objective functions arise in optimization problems, the generalized (or Clarke’s) gradient (see [9]) must be considered. Based on the above theoretical results, in [8] we determined the bang-singular-bang (b-s-b) optimal solution:

 

umax

if A · π(t) > −λ0

 

 

u (t) =

using = 0

if

−λ0 [A · π(t), η · A · π(t)]

(4)

 

 

if

η

·

A

·

π(t) <

λ0

 

 

umin

 

 

 

 

The previous algorithm interpolates π(t) and works with a continuous function. Thus, by adjusting the switching times, it is capable of achieving the final volume b to discharge with the desired precision. However, generating companies must in fact present o ers in the day-ahead market for each of the 24 hours of the following day. That is, we need to convert a continuous variable into a discrete variable. We shall lose an essential feature in this conversion: we shall no longer be able to achieve any final volume of water precisely.

c CMMSE

Page 159 of 1573

ISBN:978-84-615-5392-1

Real-time optimization of a wind-hydro power plant

In fact, the volume discharged in the b-s-b solution must belong to the set of M possible values: Ω = {b1, b2, ..., bM }. The plant operator therefore only needs choose in Ω = {bi}Mi=1 the nearest value, without exceeding the available volume, b (bsol < b < bsol+1). In this case, bsol is the discharged volume corresponding to the optimal b-s-b solution.

4Qualitative analysis of real-time optimization

In view of the above results, we shall conduct a qualitative study on the b-s-b solution. Let us assume we have obtained the solution for a certain λsol (calculated by aiming at a certain final volume, bsol). We can know the price, πturb, above which it is of interest to discharge water, and we can know the price, πpump, below which it is of interest to pump water. It is shown that, between the instants of pumping (tpump), stoppage (tstop) and discharging water (tturb), the following relations exist between the prices:

π(tpump) < π(tstop); π(tstop) < π(tturb);

π(tturb) > η · π(tpump)

Furthermore, between two instants of stoppage, it is verified that:

 

 

 

λsol

λsol

π(tstop1

), π(tstop2

)

 

,

 

 

η · A

A

(5)

(6)

When the plant operator prepares its o er for the day-ahead market for day D, this solution obtained for the pumped-storage plant, assuming the market prices and available water to be known, is the one that it will o er, seeing as it maximizes profits. The wind power plant will o er according to the best forecast for wind power production available at 10 hours the day before, D − 1. However, when day D arrives, deviations will almost certainly be produced between the actual wind power production, W r(t), and the forecasted production, W f (t). In this context, we shall pose the following question: when faced with a deviation in wind power generation at the instant t, might it be of interest to the pumped-storage plant to modify its behavior in real time (i.e. at t) so as to compensate for the deviation penalties of the wind farm and thus achieve a greater joint profit?

Let us call d(t) = W r(t) − W f (t) the deviation of the wind farm at the instant t, p+(t) the price the market pays the over-generation deviation (which will be a certain fraction s of the market price) and p(t) the price we must pay for the under-generation penalty (which will be a certain fraction l of the market price). Let us assume in all cases that the deviations are against the system. We shall analyze in detail the two possibilities for the deviations, d(t), of the wind power plant: 1) the over-generation deviation, and 2) the under-generation deviation.

Let us now consider the first case. 1) If the wind farm presents an over-generation deviation, the hydro-plant will be able to act at t in only two cases: 1a) If it was stopped, it will use the over-generation from the wind power plant to pump water; 1b) If it was

c CMMSE

Page 160 of 1573

ISBN:978-84-615-5392-1

L. Bayon,´ J.M. Grau, M.M. Ruiz, P.M. Suarez´

discharging water, it will produce less power to compensate for the over-generation of the wind farm. If it was already pumping, as the solution is of the b-s-b type, it will not be able to act. Let us analyze sub-case 1a). At instant t, the hydro-plant was stopped and pumped d(t)(MW ) at zero cost. The amount of water pumped at t which will then be used is: d(t)/η.A. With this modification, the deviation in wind power generation does not produce any profit at t, and we must find an instant t at which it is of interest to the pumped-storage plant to discharge this water. At t , the hydro-plant may be stopped (sub-case 1a1) or pumping (sub-case 1a2), seeing that, as the solution is of the b-s-b type, if it was discharging water, the turbines cannot be put to greater use. It should be borne in mind that this action will mean a change in its scheduling and will hence result in a penalty; in this case, for over-generation.

We shall analyze all the other cases in a similar way to this case and shall see in a detailed manner that the conditions that must be fulfilled for the real-time modification to be of interest can never be given by the conditions (5) and (6). Conclusion: no real-time modification is of interest.

5A posteriori optimization of a wind-hydro power plant

Subsequent to the above study, we posed the question as to whether it is possible to model the functioning of the wind-hydro power plant so as to operate in a coordinated manner a posteriori and thus improve profits. We shall not make real-time compensations for undergeneration deviations in wind power. We shall however compensate for over-generation deviations in wind power. We shall attempt to use the surplus wind power generated on day D to pump water, thereby avoiding penalties for over-generation on day D and subsequently use this water in the hydro-plant by discharging it on the following day D +1. Furthermore, as we are working for the day-ahead market, we shall eliminate all the uncertainty associated with the process.

B = # T πD+1(t)P D+1(t) + πD(t)W D(t) − CD(t) dt (7)

0

The total profit over the optimization interval [0, T ] is revenue minus cost. Revenue is obtained by multiplying the hydraulic production, P (t), and the wind power production, W (t), by the clearing price, π(t), at each hour, t. The unique cost in our system is the cost of deviation penalties, C(t). Accordingly, and in order for the comparison to be rigorous, the wind power production is considered to be sold to the market on day D and that of the hydroplant on day D + 1. We shall use superscripts to denote the day under consideration. In uncoordinated operation, we shall have that z(T ) = bsol. In the coordinated configuration, the profit obtained shall have to take into account the reduction in deviation penalties, C(t), and the increase in the volume of water available: z(T ) = bsol + b . To illustrate

c CMMSE

Page 161 of 1573

ISBN:978-84-615-5392-1

Real-time optimization of a wind-hydro power plant

the behavior of this solution, we shall consider an example of a wind-hydro power plant and compare the uncoordinated and the coordinated configurations. We shall see that it is possible to obtain profit in the latter case.

Acknowledgements

This work was supported by the Spanish Government (MEYC, project: MTM2012-32961).

References

[1]E. Spahic, G. Balzer, B. Hellmich, W. Munch, Wind Energy Storages - Possibilities, Proc. Power Tech. 2007 IEEE Lausanne (2007), 615–620.

[2]E. D. Castronuovo, J. A. P. Lopes, On the optimization of the daily operation of a wind-hydro power plant, IEEE Trans. Power Syst. 19 (2004), 1599–1606.

[3]J. S. Anagnostopoulos, D. E. Papantonis, Pumping station design for a pumpedstorage wind-hydro power plant, Energy Conversion and Management, 48 (2007), 3009– 3017.

[4]M.A. Ortega-Vazquez, D.S. Kirschen, Estimating the spinning reserve requirements in systems with significant wind power generation penetration, IEEE Trans. Power Syst. 24 (2009), 114–124.

[5]A. Jaramillo, E. D. Castronuovo, I. Sanchez, J. Usaola, Optimal operation of a pumped-storage hydro plant that compensates the imbalances of a wind power producer, Electr. Pow. Syst. Res. 81 (2011), 1767– 1777.

[6]J. Garcia-Gonzalez, R. de la Muela, L. Santos, A. Gonzalez, Stochastic joint optimization of wind generation and Pumped-Storage units in an electricity market, IEEE Trans. Power Syst. 23 (2008), 460–468.

[7]M. E. El-Hawary, G. S. Christensen, Optimal Economic Operation of Electrical Power Systems, Academic Press, New York, 1979.

[8]L. Bayon, J. M. Grau, M. M Ruiz, P. M. Suarez, Optimization of a pumpedstorage fixed-head hydro-plant: the bang-singular-bang solution, Math. Prob. Eng. (2011), 1-11.

[9]F.H. Clarke, Optimization and Nonsmooth Analysis, Wiley, New York, 1983.

c CMMSE

Page 162 of 1573

ISBN:978-84-615-5392-1

Соседние файлы в предмете [НЕСОРТИРОВАННОЕ]