Research article Special Issues

A chaotic Jaya algorithm for environmental economic dispatch incorporating wind and solar power

  • Received: 10 September 2023 Revised: 24 October 2023 Accepted: 30 October 2023 Published: 06 December 2023
  • The integration of renewable energy resources (RESs) into the existing power grid is an effective approach to reducing harmful emission content. Environmental economic dispatch is one of the complex constrained optimization problems of power systems. These problems have become more complex as a result of integrating RESs, as the availability of solar and wind power is stochastic in nature. To obtain the solution of such types of complex constrained optimization problems, a robust optimization method is required. Literature shows that chaotic maps help to boost the search capability through improvisation in the exploration and exploitation phases of an algorithm; hence, they are able to provide superior solutions during optimization. Therefore, in this study, a new optimization technique was developed based on the Jaya algorithm called the chaotic Jaya algorithm. Here the main aim was to investigate the impact of RES integration into conventional thermal systems on total power generation cost and emissions released to the environment. The proposed approach was tested for two standard cases: (i) scheduling of a committed generating unit for a specific time and (ii) scheduling of a committed generating unit for a time period of 24 hours with 24 intervals of 1 hour each. The simulation results show that a tent map is the best-performing map for a sample problem under consideration, as it provides better results. Hence, it has been considered for detailed analysis.

    Citation: Vishal Chaudhary, Hari Mohan Dubey, Manjaree Pandit, Surender Reddy Salkuti. A chaotic Jaya algorithm for environmental economic dispatch incorporating wind and solar power[J]. AIMS Energy, 2024, 12(1): 1-30. doi: 10.3934/energy.2024001

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  • The integration of renewable energy resources (RESs) into the existing power grid is an effective approach to reducing harmful emission content. Environmental economic dispatch is one of the complex constrained optimization problems of power systems. These problems have become more complex as a result of integrating RESs, as the availability of solar and wind power is stochastic in nature. To obtain the solution of such types of complex constrained optimization problems, a robust optimization method is required. Literature shows that chaotic maps help to boost the search capability through improvisation in the exploration and exploitation phases of an algorithm; hence, they are able to provide superior solutions during optimization. Therefore, in this study, a new optimization technique was developed based on the Jaya algorithm called the chaotic Jaya algorithm. Here the main aim was to investigate the impact of RES integration into conventional thermal systems on total power generation cost and emissions released to the environment. The proposed approach was tested for two standard cases: (i) scheduling of a committed generating unit for a specific time and (ii) scheduling of a committed generating unit for a time period of 24 hours with 24 intervals of 1 hour each. The simulation results show that a tent map is the best-performing map for a sample problem under consideration, as it provides better results. Hence, it has been considered for detailed analysis.



    The need for electrical energy is growing day by day with industrial growth, and it will continue to increase due to widespread industrial growth. The electricity sector is still dominated by thermal power, in particular fossil fuels such as coal, natural gas and petroleum. They are considered the main sources of harmful pollution, and they have gained much attention in the last few decades. By considering new regulations for excessively generated greenhouse gases, a combination of economic dispatch and constraints on emission has come into existence; it is called economic emission dispatch (EED). EED is a multi-objective optimization problem of power systems, where in addition to the minimization of power generation cost, the minimization of emission is also considered simultaneously. The complicated operational constraints related to the EED problem, such as the valve-point loading effects, ramp-rate limits and prohibited operating zones (POZ) make the formulation highly nonlinear, discontinuous and non-convex. The main idea of EED is to find out the best compromise solution between two objectives i.e., cost and emission. The EED problem can be solved either by considering emission as a weighted function in the objective function [1,2,3] or by considering emission as a constraint [4]. Combined EED (CEED) is another method in which the coefficient of the price penalty factor is multiplied by the emission part of the objective function [5,6,7]. Also, a multi-objective optimization problem can be solved by converting it into a single-objective optimization problem using the weighted sum approach. The best part of the weighted sum method is that sets of Pareto-optimal solutions can be obtained by varying the weight [3].

    As per the literature, deterministic approaches are not found to be suitable for dealing with large-scale integrated power systems. These methods are found to be associated with the inability to escape the local minima [8]. Therefore, researchers have turned toward nature-inspired optimization (NIO) methods due to their ability to find near-optimal solutions more efficiently. NIO methods knit together five categories of optimization approaches, i.e., evolutionary optimization, swarm intelligence-based optimization, ecology-based optimization, physical science-based optimization and optimization methods inspired by human intelligence [9].

    Particle swarm optimization (PSO) is a well-accepted algorithm that belongs to the family of swarm intelligence algorithms due to its easy implementation, simplicity, fast convergence and robustness. However, PSO is very sensitive to its control parameters. A fuzzy section mechanism has been implemented and utilized for the solution to the multi objective economic dispatch (MOED) problem in [10]. To control the inertia weight an annealing reduction technique was implemented in [11]. The gravitational search algorithm (GSA) is based on Newton's law of gravity. It is a memory-less algorithm that can accelerate the optimization process without sacrificing accuracy. Obtaining the solution to multi-dimensional CEED problems by using a GSA is discussed in [5]. The harmony search algorithm (HSA) is a derivative-free optimization method inspired by the music improvisation of the musicians. In [6], the chaotic patterns and virtual memory concepts are utilized for solving the CEED problems; this modification is found to be highly efficient. The sine cosine algorithm is a population-based optimization method. It uses a mathematical model to create multiple initial random candidate solutions and requires them to fluctuate toward the best solution by utilizing sine and cosine functions. It has been applied and tested on CEED problems and found to be fast and efficient [7].

    Literature shows that with the hybridization of two methods, proper balance between exploration and exploitation can be possible and will lead to improved performance.

    Differential evolution (DE) is a heuristic method that improves candidate solutions over several generations by using three operations, i.e., mutation, crossover and selection, to reach an optimal solution. DE is found to give better solutions while satisfying all operational constraints for multimodal non-convex EED problems [12]. However, DE is unable to map its unknown variables efficiently when the complexity and size of the system increase. In the initial phase, the solution moves toward its optima in a faster manner; however, in a later stage, it requires fine-tuning. To achieve a proper balance between exploration and exploitation, a hybrid DE/biogeography-based optimization (BBO) method [13] has been used; it utilizes the migration operator of BBO, along with the three operators of DE, to find better convergence and solution quality. Similarly, by simultaneously updating the particle velocity in PSO and the acceleration coefficient of the GSA, improved performance was achieved [14]. By applying the time-variable acceleration coefficient in PSO to explore the entire search space and a local version of DE to the exploitation phase a hybrid DE-PSO algorithm [15] was used to obtain the feasible solution in a fast and efficient manner for a multi-objective economic dispatch (MOED) constraint optimization problem.

    Rising power demand with minimum pollution constraints can be achieved through the integration of renewable energy sources (RESs) in the existing power network. However, the integration of RESs further complicates the problem due to their stochastic nature. RESs such as wind and solar power have maximum power generation limits that are variable and change with time. The uncertainty associated with RESs is a serious factor that must be considered for power generation planning for a longer time frame. The uncertainty function associated with RESs can be modeled by using the beta, log-normal, or Weibull probability distribution function (PDF). The solution to the EED problem for wind-thermal systems, as obtained by using a Weibull PDF is presented in [9,16,17]. Recently, in [18,19,20] solutions for EED were presented as a result of incorporating solar power. The binary flower pollination algorithm [18] has been applied to solve the CEED problem by incorporating solar power. Risk probability concepts were utilized to attain a better solar share of photovoltaic units and this reduced the total cost of the hybrid system. Impact analysis with a focus on the total operating cost and reduction in emission level of a solar-wind-thermal system was carried out by using a hybrid teaching-learning-based optimization (TLBO)-PSO algorithm in [19]. A new constrained multi-objective extremal optimization algorithm that has advanced constrained handling capability was proposed for the solution of the EED problem incorporating variable wind and solar power [20]. The lognormal PDF for calculating solar power, as well as the Weibull PDF for the calculation of wind power are utilized here.

    Dynamic EED (DEED) is an extension of the EED problem, where the scheduling of committed generator units is carried out over the scheduled time period. Here, the ramping constraints of generators are also taken into consideration [3]. It is much more complex to solve than the classical EED problem due to the application of much more variable and operational constraints. In 2006, a PSO-based goal attainment method was used to solve the five-unit DEED problem. The multi-objective problem has been converted to single objective optimization goal attainment and then solved by using PSO [21]. PSO with avoidance of worst locations (AWL) and gradually increasing directed neighborhoods (GIDN) has been used to solve the 10-unit DEED problem. In the aforementioned study, a weighted sum approach was applied to convert the multi-objective problem into a single objective problem. The simulation results demonstrated that the performance of PSO with GIDN topology and AWL performs best [22]. The non-dominated sorting genetic algorithm II (NSGA II) was applied to solve 10 DEED problems with non-smooth cost and emission functions [23]. In their study, the NSGA simulation results were found to be better than those for the classical approach. To improve the computational efficiency of the bacterial foraging algorithm (BFA), a BFA with a crossover operation and parameter automation strategy has been used to solve the 10-unit DEED problem [24]. Finally, the fuzzy selection mechanism was adopted to find non-dominating solutions. In this previous study, the simulation results show that an improved BFA performs better than the classical BSA and NSGA-II. To avoid entrapment in local optima, TLBO phase angle-based mechanisms have been proposed and applied to solve 5-, 10- and a large-scale 120-unit DEED problem [25]. Simulation results demonstrate that ϴ-TLBO was able to provide high-quality well-distributed solutions in a single run. Variants of DE like multi-objective neural networks evolved with DE [26] to generate the Pareto front and the efficient fitness-based DE [27] which has a double mutation strategy, random mutation factor and crossover rate with learning ability have been proposed to solve DEED problem. In [28], a new enhanced harmony search algorithm was used to solve the DEED problem that utilizes (i) three arbitrary distance bandwidths to enhance global and local search capability and (ii) consideration of both the best and worst memory vectors in the second half of generation to enhance solution quality and avoid premature convergence.

    Considering the ever-increasing power demand, fossil fuel costs and environmental legislation (e.g., Kyoto protocol) have forced expansion of the use of RESs. Hence, hybrid power generating systems come into existence. For this, a collective cost function of conventional thermal power generators with RESs and emission function needs to be investigated to analyze its impact on environmental and economic factors. The power generation by RES like wind and solar both is uncertain and variable. Therefore, direct cost, overestimation and underestimation costs are considered in the modeling. However, the uncertainty of RES leads to more complications in the formulation of the DEED problem [29,30,31]. A hybrid flower pollination algorithm that combines flower pollination algorithm (FPA) and DE is used to solve the DEED problem of a six-unit wind-thermal system [29]. Here fuzzy selection was used to find better trade-off solutions. Whale optimization algorithm (WOA) which is inspired by the hunting strategy of humpback whales [30], DE with ensemble selection method [31] was used to handle the DEED problem with wind integration. Substantial saving in cost and emission is reported in [32] using electric vehicles and a multi-objective evolutionary approach known as the exchange market algorithm. The membrane optimization algorithm is employed for the solution of the combined cost-emission optimization problem and produces Pareto solutions and recommendations for the best solution which is superior to reported results [33]. In reference [34] Equilibrium optimization was used for profit maximization as well as reduction in pollution content. It was tested on a hybrid thermal-wind-PV system.

    PV systems and wind turbines both are dependent on climate change and hence neither system is capable of delivering enough electricity reliably and efficiently. However, a Battery storage system with its integration in a suitable size helps to improve power quality, suppresses power due to renewable energy resources and also helps to reduce the mean cost of energy [35,36].

    According to the no-free-lunch (NFL) theorem, no algorithm can solve all types of optimization problems and there is still a chance to get a better solution by a new algorithm [37]. Also, literature shows that chaotic sequences with heuristic optimization have been used together to get improved performance [38,39].

    Mostly the reported methods used to solve CEED/DEED problems have some limitations as trapping to local optima, slow convergence and complexity due to more control parameters. JAYA algorithm is selected due to the fewer control parameters to tune and easier implementation. Chaotic map with JAYA is used to avoid trapping to local optima. The main contribution in this work is summarized as follows:

    • An analytical objective function model is developed for a hybrid thermal-wind-solar system. It includes the collective cost function of three types of power generating units, operational constraints, uncertainty of wind, solar system and emission function due to thermal units.

    • Population-based JAYA algorithm and JAYA algorithm embedded with a chaotic map are implemented to investigate the hybrid thermal-wind-solar for CEED and DEED problems.

    • The impact of wind integration, with both solar and wind integration is investigated with a 10-thermal unit non-convex system and analyzed for single and bi-objective optimization under fixed load demand.

    • The competence and robustness of the proposed methodology are confirmed with the reported results.

    • The impact of wind integration, both solar and wind integration is investigated with 10-thermal units analyzed for single and bi-objective optimization for 24 hours with 24 intervals of 1 hour each.

    Problem formulation is presented in Section 2. A brief introduction of the JAYA algorithm, chaos maps and step-by-step implementation process of the Ch-JAYA algorithm for the solution of the EED problem are discussed in section 3. The simulation results and discussions are presented in section 4 and finally, concluding remarks are drawn in section 5.

    The objective of the DEED problem is to find out the optimal generation schedule over the period in such a manner that costs associated with power generation and emission are minimized simultaneously. The total cost (TC) of power generation can be symbolically represented by,

    TC=Hh=1{Nthk=1C(Pthk)h+Nwl=1C(Pwl)h+Npvm=1C(Ppvm)h} (1)

    The first part of Eq (1) represents the fuel cost of the thermal power generating unit, and it is given by,

    Nthk=1C(Pthk)=Nthk=1[akP2thk+bkPthk+ck+|eksin(fk(PminthkPthk))|] (2)

    The second part of Eq (1) is the cost due to wind power. The system operator has to deal with either for deficit or more than scheduled power generation by wind farms due to the stochastic nature of wind power. The deficit in wind power can be fulfilled by maintaining a sufficient amount of spinning reserve (SR) and it is considered as an overestimation and the cost corresponding to SR is added to power generation. On the other hand, the generation of more power than scheduled power by wind farm system operators has to bear the penalty called underestimation cost. Therefore, wind power generation includes three costs: direct cost, overestimation cost/reserve cost and underestimation cost/penalty cost [3,20,29,30,31].

    Nwl=1C(Pw,l)=Nwl=1(bw,l×Pws,l)+Nwl=1kp(Pwav,lPws,l)+Nwl=1kr(Pws,lPwav,l) (3)

    Reserve cost/overestimation cost of wind power is given by,

    kr(Pws,lPwav,l)=kr×Pws,l0(Pws,lPw,l)fw(Pw)dPw (4)

    The penalty cost/underestimation cost of wind power is given by,

    kp(Pwav,lPws,l)=kP×Pw𝓇lPws,l(Pw,lPws,l)fw(Pw)dPw (5)

    In this work, the Weibull PDF is used for wind speed distribution as the wind speed is uncertain and irregular. The Weibull PDF is represented by,

    f(v)=(kc)×(vc)k1×exp[(vc)k] (6)

    The corresponding cumulative distribution function (CDF) can be represented by,

    F(v)=1exp[(vc)k] (7)

    For each wind power generating unit, the power output at a given wing speed can be expressed by using [29,30,37],

    Pw(v)={0v<vinandv>voutPw𝓇(vvinvrvin);vin<v<vrPw𝓇;vr<v<vout (8)

    The probability of wind power is 0 to Pw𝓇, and it can be calculated by using,

    fw(Pw){Pw=0}=1exp((vinc)k)+exp((voutc)k) (9)

    Wind power in the range vin<v<vr is given by [37],

    P=Pw𝓇(vvinvrvin)=(Pw𝓇vrvin)×v(vinvrvin) (10)
    fw(Pw)=k×𝒽×vinPwr×c((1+𝒽×PPw𝓇)vinc)k1×exp{((1+𝒽×PPw𝓇)vinc)k} (11)

    where

    𝒽=(vrvin)1 (12)
    fw(Pw){Pw=Pw𝓇}=exp((vrc)k)exp((voutc)k) (13)

    A typical Weibull PDF with a shape factor of 2 and scale factors of 5 and 10 is shown in Figure 1. The third part of Eq (1) represents the cost associated with solar power. It also has three cost components including direct cost, reserve cost and penalty cost [40].

    Npvm=1C(Ppv,m)=Npvm=1(bpv,m×Ppvs,m)+Npvm=1kp(Ppvav,mPpvs,m)+Npvm=1kr(Ppvs,mPpvav,m) (14)
    Figure 1.  Weibull probability density function (PDF) for k = 2 and C = 5, 10.

    Reserve cost associated with solar power generation that is derived from the overestimation of solar power and it can be represented by using [40],

    kr(Ppvs,mPpvav,m)=kr×Ppvs,m0(Ppvs,mPpv,m)fpv(Ppv)dPpv (15)

    Penalty cost associated with solar power generation is derived from the underestimation of solar power and it can be represented by using [40],

    kp(Ppvav,mPpvs,m)=kp×Ppv𝓇,mPpvs,m(Ppv,mPpvs,m)fpv(Ppv)dPpv (16)

    The solar irradiation (Gpv) to energy conversion function of solar PV generators can be represented as [40],

    Ppv(Gpv)={Ppv𝓇×(Gpv2Gstd×Rc),for0<Gpv<RcPpv𝓇×(GpvGstd),forGpv>Rc (17)

    The output of a solar power plant depends on irradiation at a particular location which can be modeled by Beta, Weibull, or Lognormal distribution. Here, Weibull PDF is used and it is represented by using [40],

    f(Gpv)=ω×(k1c1)×(Gpvc1)k11×exp[(Gpvc1)k1]+(1ω)×(k2c2)×(Gpvc2)k21×exp[(Gpvc2)k2] (18)

    The cumulative distribution function (CDF) of Eq (18) can be represented by using,

    F(Gpv)=ω×[1exp{(Gpvc1)k1}]+(1ω)×[1exp{(Gpvc2)k2}] (19)

    As per the transformation of the random variable, linear transformation is carried out with solar irradiation (Gpv) random variable, and it can be represented by using [40],

    Ppv=𝒶Gpv+𝒷=Γ(Gpv) (20)
    fpv(Ppv)=f[Γ1(Ppv)]|dΓ1(Ppv)dPpv|=f(Gpv)×|1𝒶|=f(Gpv)×|Ppv𝒷𝒶|×|1𝒶| (21)

    Solar power probability for the piecewise function can be represented by using,

    Ppv=Gpv×(Ppv𝓇Gstd)=𝒶Gpv for Gpv>Rc (22)

    where

    𝒶=Ppv𝓇Gstd (23)
    fpv(Ppv)=fpv(Ppv𝒶)×1𝒶=fpv(Ppv.GstdPpv𝓇)×GstdPpv𝓇 (24)

    The second-order transformation is accomplished with solar irradiation (Gs), and it can be represented by using,

    Ppv=Gpv2×(Ppv𝓇Gr×Rc)=𝒶2Gpv;for0<Gpv<Rc (25)
    fpv(Ppv)=12𝒶Ppv[f(Ppv𝒶)+f(Ppv𝒶)] (26)
    f(Ppv)=12Ppv𝓇PpvGstdRc×[f(PpvGstdRcPpv𝓇)+f(PpvGstdRcPpv𝓇)] (27)

    The total emission (TE) from various pollutants can be symbolically represented as follows:

    minimize

    TE=Nthi=1Ei(Pi) (28)

    where

    Ei(Pi)=αiP2i+βiPi+γi+ηiexp(δi.Pi) (29)

    The multi-objective optimization problem was converted into a single-objective optimization problem using the weighted sum approach [3]. The objective of the DEED problem can be written as,

    minimize

    [w×TC+(1w)×TE];where  w(0,1) (30)

    Subjected to the following operational constraints.

    These constraints are expressed as,

    Nthk=1Pth,k+Nwl=1Pw,l+Npvm=1Ppv,m=PD+PL (31)
    Pminth,kPthPmaxth,k (32)
    Pminw,lPw,lPmaxw,l (33)
    Pminpv,mPpv,mPmaxpv,m (34)
    RRLdownth,kPth,kP(th1)kRRLupth,k (35)

    To aggregate two conflicting objectives (cost and emission), the fuzzy-min ranking method is used. Linear membership function μi,r(ith solution of rth objective function) is described for each objective function Fi in Eq (36) and also in Figure 2.

    μi,r={1ifFi,rFminrFmaxrFi,rFmaxrFminrifFminrFi,rFmaxr0ifFi,rFmaxr (36)
    Figure 2.  Membership function.

    For ith solution, the rank is defined as [24],

    fuzzy_mini=min(μi,r)forr=1,2.m (37)

    The solution with maximum membership value (μr) is considered as the best compromise solution (BCS).

    The Jaya algorithm is one of the simple and powerful optimization methods proposed by Rao [41]. The basic idea behind the Jaya algorithm is to obtain a solution for a specified optimization problem that avoids the worst solution and moves toward the best one. It is a population-based evolutionary algorithm and does not require any algorithm-specific parameter to tune for its convergence.

    Let us consider an objective function f(X), where X is a d-dimensional variable and the population size is p. Let the best and worst values of the objective function produced by the candidate solution be f(Xbest) and f(Xworst), respectively [39]. Then, the jth element of the ith solution is updated by using,

    Xn+1ij=Xnij+𝓇1,ij×(Xbest,ij|Xij|)𝓇2,i,j×(Xworst,ij|Xij|) (38)

    where 𝓇1,ij and 𝓇2,i,j are the two random numbers in the range [0, 1].

    The second term of Eq (38) helps to move solutions towards the best solution and the third term helps to escape away from the worst solution. All the improved objective function values at the end of every iteration are transferred to successive iterations. Hence, the algorithm can achieve victory by attending to the global best solution. This process carries forward the victorious members of the population through the iterations. Therefore, the algorithm has been named as Jaya which means victory in the Sanskrit and Hindi languages.

    The search process of the Jaya algorithm is governed by the two uniformly distributed random numbers 𝓇1,ij and 𝓇2,i,j. The Jaya algorithm was found to saturate prematurely for practical real-life problems where the objective functions have non-convex and discontinuous nature and there are probabilistic variables. From the literature, it was found that the random numbers generated using chaotic sequences enhance the population diversity and the global search capability of evolutionary algorithms [6,24,36,37] thus avoiding convergence to the local optimum solution. Different chaotic maps were used to generate a sequence of chaotic random numbers introduced to replace two random numbers. The jth element of the ith modified solution vector in the (n+1)th iteration will be computed by using

    Xn+1ij=Xnij+Chn+1×{𝓇1,ij×(Xbest,ij|Xij|)𝓇2,i,j×(Xworst,ij|Xij|)} (39)

    where Chn+1 is the random number generated by using a chaotic map as explained in the next section. The solution strategy used for the optimization process using the Chaotic Jaya algorithm is presented using the flowchart in Figure 3.

    Figure 3.  Flow chart for Ch-Jaya algorithm.

    Chaos theory is a branch of mathematics that deals with nonlinear dynamic systems and chaos systems are found to be highly sensitive to the initial condition. Chaos helps to improve the performance of population-based metaheuristic algorithms. The ten chaos maps [36,37] which are embedded with the Jaya algorithm are listed below. For n = 1, Xn=rand.

    Xn+1=Cos(nCos1(Xn)) (40)
    Xn+1=mod{Xn+𝒷(𝒶2π)×sin(2πXn),1),𝒶=0.5,𝒷=0.2 (41)
    Xn+1={1,Xn=01mod(Xn,1),otherwise (42)
    Xn+1=Sin(𝒶πXn),𝒶(0,1) (43)

    here, the range of the map is (-1, 1).

    Xn+1=𝒶Xn(1Xn),𝒶=4 (44)
    Xn+1={XnP0Xn<PXnP0.5PPXn<121PXn0.5P12Xn<(1P)1XnP(1P)Xn<1 (45)

    here P is the control parameter considered as 0.4.

    Xn+1=(𝒶4)×Sin(πXn),where0<𝒶4 (46)
    Xn+1=μ(7.86Xn23.31X2n+28.75X3n13.1302875X4n),μ=1.7 (47)
    Xn+1=𝒶X2n×Sin(πXn),where𝒶=2.3 (48)
    Xn+1={Xn0.7Xn<0.7(103)×(1Xn)Xn0.7 (49)

    To verify the effectiveness of the Ch-JAYA algorithm for the solution of the EED problem, first define the experimental data like the number of power generating units as the dimension of the problem, cost coefficients, emission cost coefficients, min-max limit of power generating units, operational constriction, population size and maximum iteration as stopping criteria.

    Step 1: Initialize the population randomly within upper and lower power generation limits as below:

    Pi=Pmini+𝓇×(PmaxiPmini)wherei=1,2,,N (50)

    where 𝓇[0,1] is a random number and N is the number of power-generating units.

    Step 2: Calculate the total cost for each candidate solution using Eq (1), check for all associated operational constraints by using the Eqs (31−35), identify the best and worst solutions and preserve them.

    Step 3: This process indicates the modification process of the algorithm. Modification of each power generating unit has been carried out as per Eq (39).

    Pnewi=Pi+Ch×[rand1×(Pbest,i|Pi|)rand2×(Pworst,i|Pi|)] (51)

    This step helps to move a solution towards the best solution and away from the worst one. The chaotic term Ch, acts as a scaling factor to ensure good diversification during the optimization process. The new best solution Pnewbest and the new worst solution Pnewworst are preserved for use in the next iteration.

    Step 4: Calculate the total cost for a modified solution after each iteration. All operational constraints given by Eqs (31−35) are checked for violations if any. The violations are used to convert the constrained optimization problem into an unconstraint problem by using the penalty function approach. Thus, a feasible solution gets a better fitness as compared to an infeasible solution.

    Step 5: If the updated solution is found to be better, then replace the modified solutions with previous solutions otherwise retain the previous one. The best solutions are stored when the stopping criterion is reached.

    Step 6: Similarly, compute all Pareto optimal solutions and rank them based on fuzzy_min to get the best possible solution by using Eqs (36) and (37).

    The proposed approach for the solution of the EED problem with the integration of RESs has been implemented using an improved version of the Jaya algorithm. The proposed Ch-Jaya algorithm is tested on two standard power system test cases, representing static/dynamic cases respectively, with different complexity levels as shown in Table 1. Both the test cases have a non-convex, multimodal and stochastic objective function, where RESs uncertainty is modeled by using the random variables. In addition to these, Test Case II has a discontinuous objective function and the optimization variables are dynamically coupled in successive intervals through the ramp rate limits.

    Table 1.  Test cases and their complexity.
    Complexity level of test cases I. 10-unit EED system [6] II. 10-unit DEED system [42]
    Non-convex multimodal
    Ramp rate limit X
    Wind (Probabilistic model)
    Solar (Probabilistic model)
    Losses included (more complex equality constraints) X

     | Show Table
    DownLoad: CSV

    Test Case I: Four test example cases are created from the 10-thermal unit non-convex system with a load of 2000 MW [6]. The data is appended in Table A1 and Table A2. In Test Case I(A), the transmission losses are included in the model, which creates additional complexity in the equality constraint. Test Case I(B) is selected for result validation; it is similar to Test Case I(A) but the losses have been neglected here. In Test Case I(C), the second and third thermal generators in I(B) are replaced by wind power units. Test Case I(D) is constructed by adding one additional solar PV system to Test Case I(C); the data for the wind and solar units is listed in Table A.3 and Figure 4.

    Figure 4.  Solar radiation for a sample day.

    System I(A) is included in the study for benchmarking the proposed Ch-Jaya algorithm with previously reported results.

    Test Case II: Test Case II(A) has all the complexities described earlier in this section and presented in Table 1. The limits, coefficients and ramp rates are given in Table A.4, and hourly demand variation is listed in Table A.5. Case II(B) is created to study the impact of RESs; hence thermal units eight and nine are replaced by wind power units and rest of the data is similar to Case IIA. Test Case II(C) has one additional solar system. The data for wind and solar units is the same as listed in Table A3 and Figure 4.

    The physical representation of the problem is shown in Figure 5. The programs have been written in MATLAB R2013a and executed on an Intel Core i7 processor with a 3.40 GHz computer with 2 GB RAM.

    Figure 5.  Schematic of Hybrid Thermal-wind-PV system.

    In metaheuristic optimization methods, the population size must be set such that the best solution can be obtained within the least possible computational time. Studies were conducted on Test Case I by varying the population size from 10 to 100 with stopping criteria of 100 iterations. Based on the statistical analysis of results presented in Table 2, using 30 trials it is observed that a population size of 50 is optimal for this problem. Similarly, for Test Case II, the best population size is found to be 100.

    Table 2.  Selection of population size for test case IA.
    NP Min cost ($/h) Ave cost ($/h) Max cost ($/h) S. D** Comp. Time/iter. (Second)
    10 111498.6776 111510.3160 111637.0302 13.1548 0.0009
    20 111497.9356 111500.8442 111515.6150 2.8109 0.0016
    50 111497.6480 111498.7725 111500.6211 0.2237 0.0039
    100 111497.9698 111498.7453 111499.6834 0.1756 0.0075
    ** Standard deviation.

     | Show Table
    DownLoad: CSV

    All chaotic maps described in Section 3.3 are embedded one by one with the Jaya algorithm and their effects were investigated on Test case IA. The statistical results of trials conducted with different chaotic maps are presented in Table 3. It is observed that the results for all the chaotic maps were almost similar, but with the lowest standard deviation, the tent map was found to be the most consistent as compared to the other maps. Therefore, for further analysis 'tent map' is used in the Ch-Jaya algorithm. However, the computational time gets increased as compared to the analysis carried out using the JAYA algorithm alone. The characteristics of the tent map along with other maps are presented in Figure 6. The convergence behavior of the Ch-Jaya algorithm is found to be superior to the Jaya algorithm as shown in Figure 7.

    Table 3.  Statistical comparison using different maps in Chaotic-Jaya (Test Case IA).
    Sr. No. Chaotic map Best cost ($/hr) Mean cost ($/hr) Max cost ($/hr) SD Ave time/iter.(seconds)
    1 Chebyshev 111497.6590 111498.1261 111500.6339 0.0978 0.0180
    2 Circle 111497.6419 111497.7775 111498.2863 0.0301 0.0179
    3 Gauss/mouse 111497.6354 111497.6646 111497.7993 0.0055 0.0182
    4 Iterative 111497.6553 111497.7350 111497.9460 0.0131 0.0183
    5 Logistic 111497.6419 111497.7897 111499.2180 0.0513 0.0183
    6 Piecewise 111497.6416 111497.72205 111498.1050 0.0176 0.0181
    7 Sine 111497.6343 111497.7277 111498.3407 0.02411 0.0183
    8 Singer 111497.6518 111497.9670 111498.8708 0.0573 0.0185
    9 Sinusoidal 111497.6596 111498.3263 111504.9584 0.24890 0.0183
    10 Tent 111497.6312 111497.6403 111497.6545 0.0007 0.0177

     | Show Table
    DownLoad: CSV
    Figure 6.  Variation of random parameters in Ch-Jaya through chaotic maps.
    Figure 7.  Cost convergence curve obtained by Jaya and C-Jaya for Test Case I.

    The results of cost and emission optimization, for single objective cases, are compared and validated with previously published results of parallel hurricane optimization algorithm (PHOA) [43], DE [12] and chaotic improved harmony search CIHSA [6] in Table 4. The least cost solution obtained by the Ch-Jaya algorithm is $ 111497.6312/hr which is better than the other methods while all operational constraints are also satisfied. Table 4, also shows that the best emission 3932.2426 lb/hr is also obtained by using Ch-JAYA. These values are shown in bold.

    Table 4.  Validation of Ch-JAYA algorithm with published results (single objective (SO): Test Case IA).
    Quantity Best cost solution Best emission solution
    PHOA[43] DE [12] CIHSA [6] JAYA Ch-JAYA DE [12] CIHSA [6] JAYA Ch-JAYA
    P1(MW) 34.2892 55 55.0000 54.9996 55.0000 55 55.000000 55 55
    P2(MW) 79.5228 79.8063 80.0000 79.9997 80.0000 80 80.000000 79.9978 79.9998
    P3(MW) 116.4348 106.8253 106.934727 107.0043 106.9381 80.5924 81.149904 81.1711 81.1362
    P4(MW) 105.4548 102.8307 100.6003177 100.5125 100.5886 81.0233 81.359769 81.3775 81.3696
    P5(MW) 110.0841 82.2418 81.476793 81.5588 81.4959 160 160.000000 159.9999 160.000
    P6(MW) 108.3113 80.4352 83.026871 82.9670 83.0162 240 240.000000 239.9996 240.000
    P7(MW) 285.1402 300 300.0000 299.9988 300.0000 292.7434 294.507931 294.5300 294.5035
    P8(MW) 319.0626 340 340.0000 339.9998 340.0000 299.1214 297.268922 297.1563 297.2800
    P9(MW) 457.6793 470 470.0000 469.9996 470.0000 394.5147 396.720288 396.8830 396.7832
    P10(MW) 470.0000 469.8975 470.0000 469.9993 470.0000 398.6383 395.587840 395.4790 395.5220
    PL(MW) 85.9792 NR 87.038709 87.0392 87.0388 NR 81.594656 81.5942 81.5943
    TC ($/h) 112130 111500 111497.6310 111497.6480 111497.6312 116400 116412.5655 116412.5699 116412.60
    TE(lb/h) 4520 4581.00 4572.27630 4572.1918 4572.2407 3923.40 3932.2433 3932.2443 3932.2426
    NR: Not reported, PL: Power loss.

     | Show Table
    DownLoad: CSV

    The results of optimization of the bi-objective model given in Eq (30) are compared in Table 5 with GSA [5], MODE [12], NSGAII [12], enhanced multi-objective cultural algorithm (EMOCA) [44], flower pollination algorithm (FPA) [45] and CIHSA [6]. The results are comparable; the best cost $ 113246.5991/hr is found by Ch-JAYA while the lowest emission 3932.44734 lb/hr is reported by CIHSA [6].

    Table 5.  Validation of best compromise solution of the Ch-JAYA algorithm (bi-objective: Test case I(A)).
    Unit EMOCA [44] NSGAII [12] MODE [12] GSA [5] FPA [45] CIHSA [6] JAYA Ch-JAYA
    P1(MW) 55 51.9515 54.9487 54.9992 53.188 55.000000 54.9879 55.0000
    P2(MW) 80 67.2584 74.5821 79.9586 79.975 80.000000 79.8351 80.0000
    P3(MW) 83.5594 73.6879 79.4294 79.4341 78.105 81.081501 86.4770 83.8795
    P4(MW) 84.6031 91.3554 80.6875 85.0000 97.119 80.930292 85.2756 83.8340
    P5(MW) 146.5632 134.0522 136.8551 142.1063 152.74 160.000000 139.9055 138.4066
    P6(MW) 169.2481 174.9504 172.6393 166.5670 163.08 240.000000 157.4987 159.5070
    P7(MW) 300 289.4350 283.8233 292.8749 258.61 290.800949 297.4614 298.0548
    P8(MW) 317.3496 314.0556 316.3407 313.2387 302.22 296.689692 316.5739 314.9958
    P9(MW) 412.9183 455.6978 448.5923 441.1775 433.21 398.842744 432.6969 433.0782
    P10(MW) 434.3133 431.8054 436.4287 428.6306 466.07 398.331226 433.3181 437.4092
    PL(MW) 83.56 84.25 84.33 83.9869 84.3 81.676404 84.0304 84.1653
    TC ($/hr) 113445 113539 113484 113490 113370 116390.278321 113249.3676 113246.5991
    TE (lb/hr) 4113.98 4130.2 4124.9 4111.4 3997.7 3932.4473 4133.2117 4133.3853

     | Show Table
    DownLoad: CSV

    The optimal generation schedule for Test Case I(B), I(C) and I(D) is presented in Table 6 separately for cost and emission minimization. Furthermore, the statistical comparison for cost and emission obtained by Ch-JAYA and JAYA alone are compared in Table 6 (A) for Test Case I and in Table 7(A) for Test Case II. Here, it is observed that the performance of Ch-JAYA is better than JAYA in terms of either cost or emission minimization for all different cases considered for the analysis.

    Table 6.  Validation and comparison of optimal schedule with/without renewable integration.
    Unit
    (MW)
    Best cost solution Best emission solution
    PHOA[43]
    (Case IB)
    Ch-JAYA PHOA[43]
    (Case IB)
    Ch-JAYA
    Thermal
    (Case IB)
    Thermal + wind
    (Case IC)
    Thermal + wind + PV
    (Case ID)
    Thermal
    (Case IB)
    Thermal + wind
    (Case IC)
    Thermal + wind + PV
    (Case ID)
    P1 55 14.6927 10.0432 10.3934 55 11.5922 39.3307 45.5559
    P2 80 79.9999 100.0000 100.0000 68.0479 78.0220 100.0000 100.0000
    P3 98.2792 89.0902 100.0000 100.0000 73.4161 77.5040 100.0000 100.0000
    P4 73.2943 80.2415 76.7470 62.9940 70.4446 77.5203 75.7202 70.7676
    P5 70.2278 66.3405 63.6932 53.0084 160 160.0000 160.0000 159.9999
    P6 72.7025 70.0003 70.0000 70.0000 240 240.0000 239.9941 240.0000
    P7 270.4959 290.6202 279.1228 241.4460 275.2700 275.7460 265.8428 233.0241
    P8 340 328.7074 315.4370 268.7833 289.1154 277.4743 267.5844 234.0780
    P9 470 470.0000 470.0000 434.1333 371.9836 379.1481 367.8421 328.5067
    P10 470 470.0000 470.0000 464.8209 396.7219 379.5854 368.0165 328.6240
    PV1 -- --- --- 75 -- -- --- 75
    PV2 -- --- --- 75 -- -- --- 75
    PV_C($/hr) -- --- --- 6704.9000 -- -- --- 6704.9000
    W_C($/hr) -- -- 899.5334 899.5332 -- -- 899.5334 899.5334
    Th_C($/hr) 106210 106170.3974 102348.7811 93899.5937 111820 111866.7977 108222.7974 100334.0048
    TC($/hr) 106170.3974 103248.3145 101504.0269 111820 109122.3309 107938.4382
    TE(lb/hr) 4285.4729 4278.7877 3487.4606 2975.8779 3661.8815 3650.7423 2873.4340 2434.4654

     | Show Table
    DownLoad: CSV
    Table 6(A).  Statistical comparison of results for test Case-I.
    Cost Method TCmin TCmean TCmax TCSD
    Thermal (I B)
    Ch-JAYA 106170.3974 106170.3974 106170.3974 0.000
    JAYA 106170.5855 106170.8291 106171.3163 0.3597
    Thermal +Wind (I C) Ch-JAYA 103248.3145 103248.3145 103248.3145 0.000
    JAYA 103248.3185 103248.84764 103249.8093 0.55689
    Thermal +Wind +PV (I D) Ch-JAYA 101504.0269 101504.0269 101504.0269 0.000
    JAYA 101504.5935 101505.118375 101506.6807 0.9642
    Emission Method Emin Emin Emin Emin
    Thermal (I B)
    Ch-JAYA 3650.7423 3650.7423 3650.7423 0.000
    JAYA 3650.7455 3664.9977 3680.1238 13.8663
    Thermal +Wind (I C) Ch-JAYA 2873.4340 2873.4340 2873.4340 0.000
    JAYA 2873.4744 2878.1352 2890.4320 6.4882
    Thermal +Wind +PV (I D) Ch-JAYA 2434.4654 2434.4654 2434.4654 0.000
    JAYA 2437.4654 2463.2701 2512.8796 37.2171

     | Show Table
    DownLoad: CSV
    Table 7.  Optimal dynamic scheduling results with/without renewable energy integration (Test Case-II).
    Description Method Cost minimization Emission minimization Cost and emission minimization
    Cost ($) Emission (lb) Cost ($) Emission (lb) Cost ($) Emission (lb)
    Test Case IIA:
    (Thermal system)
    Ch-JAYA 2357135.0653 297005.3021 2539639.2507 270810.7558 2394132.0810 278171.8319
    MBDE [27] 2482843.7918 ----- ---- 297235.4254 2475942.8.000 280507.6674
    Test Case II B: (Thermal+wind) Ch-JAYA 2275684.9410 286249.2552 2447015.6637 256591.0774 2361299.2651 263475.4069
    Test Case II C: (Thermal+ wind +PV) Ch-JAYA 2200281.3668 258709.1654 2384872.7478 230769.1362 2240688.9885 240771.7490

     | Show Table
    DownLoad: CSV
    Table 7(A).  Statistical comparison of results for Test Case-II.
    Cost Method TCmin TCmean TCmax TCSD
    Thermal (II A)
    Ch-JAYA 2357135.0653 2357185.2055 2357228.1341 39.1856
    JAYA 2357143.2012 2357238.8978 2357305.9396 65.7636
    MBDE [27] 2482843.7918 2536958.9047 2595664.8001 ---
    Thermal + Wind (II B) Ch-JAYA 2275684.941 2275794.2866 2275968.7051 90.1342
    JAYA 2275866.2582 2276399.9979 2276864.7177 180.1079
    Thermal + Wind + PV
    (II C)
    Ch-JAYA 2200281.3668 2200292.1569 2200329.9201 18.7739
    JAYA 2200286.855 2200387.7602 2201001.2758 104.6502
    Emission Method Emin Emin Emin Emin
    Thermal (II A)
    Ch-JAYA 270810.7558 270849.22645 270886.9112 45.3023
    JAYA 270819.3222 270862.3130 270955.822 55.0001
    MBDE [27] 297235.425431 3006001.8728 316941.7067 ---
    Thermal +Wind (II B) Ch-JAYA 256591.0774 256678.8098 256782.2145 80.0806
    JAYA 256600.597268 256769.4573 256895.0774 136.5168
    Thermal +Wind +PV
    (II C)
    Ch-JAYA 230769.1362 230791.84022 230881.3668 47.1869
    JAYA 230771.9084 230842.99605 230975.3772 81.6702

     | Show Table
    DownLoad: CSV

    For case I(B), the cost $ 106170.3974/hr and emission 3650.7423 lb/hr, both computed by Ch-JAYA are superior to PHOA [43]. The minimum cost obtained by the Ch-JAYA algorithm for Test Case IIA using dynamic scheduling $ 2357135.0653, is shown to be better than the MBDE [27] algorithm $ 2482843.7918 in Table 7. Thus, the superior global search capability of Ch-Jaya is shown for the more complex Test Case II. Further analysis of Tables 6 and 7 for the impact of RESs is presented in the next section.

    From Table 6, it can be observed that as compared to the thermal system (Test Case IB), the reduction in cost with wind integration is found to be $ 2922.0829/hr (2.75% per hour) and with wind-solar integration is $ 4666.3705/hr (4.39% per hour). When two wind farms were replaced with thermal units in Test Case I(C), the greenhouse emission was reduced to 2873.4340 lb/hr (21.29%) and by integrating wind and solar PV systems (Test Case I(D)) the emission is reduced to 2434.4654 lb/hr (33.31%) as compared to emission released by the thermal system alone. So, it is concluded that optimization of "emission only" results in a greater reduction in emission as compared to reduction in cost for "cost only" optimization cases.

    Similarly, the best cost solutions from Table 7 can be compared for Test Case II(A), II(B) and II(C) respectively. It is observed that the optimal cost of generation in a day for the three test cases is found to be $ 2357135.0653, $ 2275684.9410 and $ 2200281.3668 respectively. Comparing the results, it is observed that there is a reduction of $ 81450.1243 (3.45% per day) in total cost due to the integration of two wind power units in Case II(B). For the hybrid wind-solar PV-thermal system, IIC, the cost saving is $ 156853.6985 (6.65% per day).

    From Table 7 it is also observed that greenhouse emission is reduced from 270810.7558 to 256591.0774 lb in Test Case II(B) and to 230769.1362 lb for Test Case II(C), which amounts to a reduction of approximately 5.25% (due to replacement of thermal units by wind units) and 14.78% per day (when one solar unit is added) respectively.

    The impact of RES integration is shown in Table 8 by comparing the results of Test Case I(B), I(C) and I(D) considering the bi-objective model. It is observed that a reduction of $ 2989.2133/hr (2.77% per hour) in cost and $ 5141.307/hr (4.76% per hour) in emission is achieved by wind integration. When both wind and solar PV systems are integrated with the thermal system the reduction in cost and emission content was found to be $ 5141.307/hr (4.77%) and 1229.4157 lb/hr (31.71%) respectively as compared to the original thermal system.

    Table 8.  Effect of renewable integration on best compromise solution for test case I.
    Unit (MW) Thermal Thermal + Wind Thermal + Wind + PV
    P1 20.9275 23.7312 26.3369
    P2 79.9996 100.0000 99.9999
    P3 81.1851 99.9981 100.0000
    P4 79.0380 77.8904 73.0557
    P5 127.0308 123.2389 109.4966
    P6 141.9648 137.0887 118.7713
    P7 285.8607 280.0773 257.0533
    P8 302.5896 294.1344 267.1088
    P9 421.2271 412.9401 382.6090
    P10 426.1043 418.7427 386.9054
    PV1 --- --- 75.0000
    PV2 --- --- 75.0000
    PV_C --- --- 6704.9000
    W_C --- 899.4238 899.5328
    Th_C 107836.9544 103947.2172 95091.2145
    TC 107836.9544 104847.7411 102695.6474
    TE 3876.1238 3098.4094 2646.7081

     | Show Table
    DownLoad: CSV

    For Test Case II, it is observed that the total cost is reduced by $ 32832.8159 (1.37% per day) in Test Case II(B) and $ 153443.0925 (6.40% per day) in Test Case IIC due to wind and wind-solar PV integration respectively. The emission content is reduced by 14696.425 lb (5.28%) for Test Case II(B) and 37400.0829 lb (13.44%) for Test Case II(C).

    The percentage reduction in total cost and emission due to RES integration for single and bi-objective goals for static/dynamic test cases—Test Cases I and II, respectively—has been summarized and shown as a stacked bar chart in Figure 8. The results in Figure 8 clearly show that after the integration of RES, the percentage reduction in emission for both test cases is higher as compared to the percentage reduction in total cost. This is because the uncertainty cost of RES, in terms of reserve and penalty costs, is included in the model. The reduction in emission in Test Case II is found to be lesser as compared to Test Case I for the same conditions/goals. This is due to the dynamic ramp-rate constraints in the DEED problem in Test Case II. These constraints limit the ramping down of the thermal generation leading to reduced scheduling of RES. Hence, emission reduction is lesser as compared to the static conditions in Test Case I. The bi-objective optimization succeeds in reducing both, cost and emission and presents a reasonably good percentage reduction in both objectives for all the tested cases.

    Figure 8.  Percentage reduction in total cost and emission due to RES integration with different goals for static/dynamic test cases.

    The full optimal generation schedule obtained by Ch-JAYA under the three different optimization goals is available for test case I(A) in Tables 4 and 5, respectively. Tables 6 and 8 give the same for test cases I(B), I(C) and I(D). Similarly, Table 9 presents the optimal schedules for hybrid Test Case-II under the dynamic condition. From all these tables it can be seen that all operational constraints are fully satisfied by the proposed Ch-JAYA.

    Table 9.  Best compromise solution for the hybrid system: Test case II(C).
    Hr P1
    (MW)
    P2
    (MW)
    P3
    (MW)
    P4
    (MW)
    P5
    (MW)
    P6
    (MW)
    P7
    (MW)
    W8
    (MW)
    W9
    (MW)
    P10
    (MW)
    PV Share
    (MW)
    1 150.0014 135.0001 191.8234 151.5584 118.5281 89.9424 129.6950 0.6593 18.4462 50.3457 0
    2 150.2594 135.0005 116.1969 169.8757 115.1308 134.9533 129.4157 95.2536 8.4065 55.5076 0
    3 150.0018 144.3037 170.9945 119.9176 164.2224 148.1099 117.5870 99.9997 92.7767 50.0867 0
    4 150.0061 214.2780 250.8108 113.6353 204.4053 111.2748 129.7704 100.0000 81.8171 50.0022 0
    5 156.4759 214.9372 241.5891 163.3822 204.6265 140.3210 129.9154 99.9999 78.3711 50.3428 0.03888
    6 151.4708 248.3874 215.6170 213.3768 243.0000 159.9998 129.9999 99.9986 100.0000 52.5487 13.601
    7 151.4197 268.7914 178.7951 263.2757 243.0000 159.9985 129.9808 99.9999 99.9999 55.9990 50.74
    8 150.0001 190.6894 252.5426 299.9989 242.5281 159.5676 129.9999 94.6370 97.7932 50.0032 108.24
    9 169.9263 242.0545 317.1218 299.9997 242.9191 159.9994 129.9955 99.9996 99.9985 55.9056 106.08
    10 184.4012 307.1239 339.9998 282.3602 242.6156 159.9994 129.6074 63.7359 99.9999 53.3767 158.78
    11 264.1419 269.8161 293.8628 299.9984 242.9990 159.9962 129.9541 99.7928 99.7843 55.6544 190
    12 259.3396 266.3450 339.9984 299.9999 242.9998 159.9268 129.7458 99.9215 99.9999 53.7233 198
    13 197.0151 264.3825 339.9999 299.9998 243.0000 159.8219 130.0000 99.9993 99.9910 55.7905 182
    14 155.8151 291.6280 282.1309 258.1326 242.9966 160.0000 129.5412 82.5117 99.9997 51.6042 169.64
    15 196.7869 213.6477 208.4307 261.2499 242.9997 142.6472 129.9959 81.3642 99.9988 53.5390 145.34
    16 178.3078 228.8341 210.8882 226.5601 204.8421 92.6599 115.3215 15.8511 99.7621 50.1731 130.8
    17 150.0027 158.7912 260.0941 225.1065 183.0817 140.2208 129.7157 68.6940 32.8061 52.9072 78.58
    18 150.2003 149.0089 266.3200 270.1136 209.5865 159.9966 129.9989 99.9958 99.7562 50.0032 43.02
    19 175.5597 228.8108 339.9994 253.3853 231.0325 159.9911 129.6348 99.9178 99.9992 55.6931 1.9763
    20 254.3194 290.4072 339.9998 299.9939 243.0000 159.9928 129.9995 99.9998 99.9996 54.2880 0
    21 252.9620 243.0624 339.9998 299.9997 242.9997 159.6172 129.8155 99.9991 99.9999 55.5447 0
    22 201.9526 179.6179 269.9255 256.2532 242.3204 121.1640 100.9190 99.9989 100.0000 55.8485 0
    23 150.0083 135.0017 189.9457 206.3243 192.3238 151.9635 70.9248 88.3861 97.1195 50.0023 0
    24 150.0012 135.0005 210.9407 237.2007 156.4406 149.3306 56.4945 38.2114 0.2879 50.0919 0
    Total cost: $ 2240688.9885, Emission: 240771.7490 (lb), Thermal cost: $ 2171546.8197, PV_cost: $ 68930, Wind cost: $ 212.1688

     | Show Table
    DownLoad: CSV

    The optimal dynamic power sharing between solar, wind and thermal systems obtained by Ch-JAYA for best cost and best emission model for Test Case II(C) is shown in Figure 9(a, b). Similarly, the optimal power sharing under the bi-objective optimization of contradictory objectives is presented in Table 9. Here, all operational constraints are also fully satisfied.

    Figure 9.  Optimal dynamic generation schedule for the hybrid system, case II(C).

    In bi-objective optimization of contradictory objectives, there are many competing solutions and the decision maker selects the best suitable solution based on case-specific constraints set by economic or environmental limitations and guidelines. Figures 10 and 11 present the multiple trade-off solutions for Case I and Case II obtained by Ch-Jaya. It can be seen that Ch-Jaya has produced solutions that cover the full spread of cost-emission solution space, between the two extreme points marked by the best cost and best emission solutions.

    Figure 10.  Comparison of Pareto-fronts for Test Case I(B), I(C) and I(D).
    Figure 11.  Comparison of Pareto-fronts for Test Case II(A), II(B) and II(C).

    A modified JAYA algorithm is developed with different chaos maps for solving a non-convex, mixed integer, multimodal and stochastic problem with practical constraints. The effect of the integration of the uncertain nature of wind and solar PV systems on the optimal scheduling of two complex test systems is modeled using a probabilistic cost function, employing single/multi-objective models. The performance of the proposed method is validated with published results for static/dynamic operating conditions, non-linear, discontinuous objective functions with multi-period, time-coupled constraints. The major findings are summarised as:

    • The Jaya algorithm is an efficient population-based evolutionary algorithm that is free from convexity assumptions and any user-controlled program-specific tuning parameters.

    • The results show that due to the integration of chaotic maps, the proposed Ch-JAYA has a superior convergence. The proposed Ch-JAYA algorithm is capable of producing feasible and credible results while handling complex and practical constraints.

    • The bi-objective optimization succeeds in reducing both, cost and emission and presents a reasonably good percentage reduction in both objectives for all the tested cases.

    • The effect of RES integration was investigated with single and bi-objective optimization goals and it was observed that the percentage reduction in emission for both the test cases is higher as compared to the percentage reduction in total cost.

    • Results show that RES integration reduces the cost by about 2-4% but results in emission curtailment in the range of 20-33%.

    • Considering simulation results under different test conditions it is observed that the Ch-JAYAalgorithm can provide credible and superior quality results and handle associated complex constraints as well as probabilistic functions in an efficient manner while satisfying all operational constraints.

    • The fuzzy-min ranking approach is utilized to get the best solution for satisfying cost and emission.

    • Pareto optimal solutions obtained under different test conditions provide various power scheduling options to GENCOs and the ISO can select scheduling options for minimizing either (i) total power generation cost, (ii) emissions or (iii) both simultaneously, to gain profit while protecting the environment.

    • Power generation from wind turbine and solar PV systems is highly.

    • This work may be extended with battery storage to improve power quality, suppress power fluctuation due to renewable energy resources and also to enhance supply security.

    This research work was supported by "WOOSONG UNIVERSITY's (Daejeon, Republic of Korea) Academic Research Funding-2023".

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    Surender Reddy Salkuti is an editorial board member for AIMS Energy and was not involved in the editorial review or the decision to publish this article. All authors declare that there are no competing interests.

    Table A1.  Unit data for Test Case I (ten unit system) [6].
    Unit Pmin
    (MW)
    Pmax
    (MW)
    a
    ($/(MW)2h)
    b
    ($/MWh)
    c
    ($/h)
    e
    ($/h)
    f
    ((rad/MW)
    α
    (lb/(MW)2h)
    β
    (lb/MWh)
    γ
    (lb/h)
    η
    (lb/h)
    δ
    (1/MW)
    1 10 55 0.12951 40.5407 1000.403 33 0.0174 4.702 -398.64 36000.12 0.25475 0.01234
    2 20 80 0.10908 39.5804 950.606 25 0.0178 4.652 -395.24 35000.56 0.25475 0.01234
    3 47 120 0.12511 36.5104 900.705 32 0.0162 4.652 -390.23 33000.56 0.25163 0.01215
    4 20 130 0.12111 39.5104 800.705 30 0.0168 4.652 -390.23 33000.56 0.25163 0.01215
    5 50 160 0.15247 38.539 756.799 30 0.0148 0.420 32.77 1385.93 0.2497 0.012
    6 70 240 0.10587 46.1592 451.325 20 0.0163 0.420 32.77 1385.93 0.2497 0.012
    7 60 300 0.03546 38.3055 1243.531 20 0.0152 0.680 -54.55 4026.69 0.248 0.0129
    8 70 340 0.02803 40.3965 1049.998 30 0.0128 0.680 -54.55 4026.69 0.2499 0.01203
    9 135 470 0.02111 36.3278 1658.569 60 0.0136 0.460 -51.12 4289.55 0.2547 0.01234
    10 150 470 0.01799 38.2704 1356.659 40 0.0141 0.460 -51.12 4289.55 0.2547 0.01234

     | Show Table
    DownLoad: CSV
    Table A2.  B-Loss coefficients (ten unit system).

     | Show Table
    DownLoad: CSV
    Table A3.  Data for solar PV unit and wind farm.
    Type of system No. of units Rated power (MW/Unit) bw, or bpv, ($/MWh) kp kr k c Vci
    (m/s2)
    Vr
    (m/s2)
    Vco
    (m/s2)
    Solar PV 2 100 40 5 5 1.5 5 - - -
    Wind 2 100 40 2 10 5 15 45

     | Show Table
    DownLoad: CSV
    Table A4.  Unit data for Test Case II (ten unit system) [42].
    Unit Pmin
    (MW)
    Pmax
    (MW)
    UR
    (MW)
    DR
    (MW)
    a
    ($/(MW)2h)
    b
    ($/MWh)
    c
    ($/h)
    e
    ($/h)
    f
    ((rad/MW)
    α
    (lb/(MW)2h)
    β
    (lb/MWh)
    γ
    (lb/h)
    η
    (lb/h)
    δ
    (1/MW)
    1 150 470 80 80 0.1524 38.5397 786.7988 450 0.041 0.0312 −2.4444 103.3908 0.5035 0.0207
    2 135 470 80 80 0.1058 46.1591 451.3251 600 0.036 0.0312 −2.4444 103.3908 0.5035 0.0207
    3 73 340 80 80 0.0280 40.3965 1049.9977 320 0.028 0.0509 −4.0695 300.3910 0.4968 0.0202
    4 60 300 50 50 0.0354 38.3055 1243.5311 260 0.052 0.0509 −4.0695 300.3910 0.4968 0.0202
    5 73 243 50 50 0.0211 36.3278 1658.5696 280 0.063 0.0344 −3.8132 320.0006 0.4972 0.0200
    6 57 160 50 50 0.0179 38.2704 1356.6592 310 0.048 0.0344 −3.8132 320.0006 0.4972 0.0200
    7 20 130 30 30 0.0121 36.5104 1450.7045 300 0.086 0.0465 −3.9023 330.0056 0.5163 0.0214
    8 47 120 30 30 0.0121 36.5104 1450.7045 340 0.082 0.0465 −3.9023 330.0056 0.5163 0.0214
    9 20 80 30 30 0.1090 39.5804 1455.6056 270 0.098 0.0465 −3.9524 350.0056 0.5475 0.0234
    10 50 56 30 30 0.1295 40.5407 1469.4026 380 0.094 0.0470 −3.9864 360.0012 0.5475 0.0234

     | Show Table
    DownLoad: CSV
    Table A5.  Load data for Test Case II (ten unit system) [42].
    Hour Load (MW) Hour Load (MW) Hour Load (MW) Hour Load (MW)
    1 1036 7 1702 13 2072 19 1776
    2 1110 8 1776 14 1924 20 1972
    3 1258 9 1924 15 1776 21 1924
    4 1406 10 2022 16 1554 22 1628
    5 1480 11 2106 17 1480 23 1332
    6 1628 12 2150 18 1628 24 1184

     | Show Table
    DownLoad: CSV


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