Volume 7, Issue 5 e70185
RESEARCH ARTICLE
Open Access

Enhanced Automatic Generation Control in Multiarea Power Systems: Crow Search Optimized Cascade FOPI-TIDDN Controller With Integrated Renewable Solar Thermal Models and HVDC Lines

Naladi Ram Babu

Corresponding Author

Naladi Ram Babu

Department of Electrical and Electronics Engineering, Aditya University, Kakinada, India

Correspondence: Naladi Ram Babu ([email protected])

Wulfran Fendzi Mbasso ([email protected])

Contribution: Conceptualization, Methodology, Writing - review & editing

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Pamarthi Sunitha

Pamarthi Sunitha

Department of Electronics and Communication Engineering, Aditya University, Kakinada, India

Contribution: ​Investigation, Validation, Writing - original draft

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Ganesh Pardhu B. S. S.

Ganesh Pardhu B. S. S.

Department of Electrical and Electronics Engineering, Aditya University, Kakinada, India

Contribution: ​Investigation, Validation, Formal analysis

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Sanjeev Kumar Bhagat

Sanjeev Kumar Bhagat

Department of Electrical Engineering, Sandip University, Madhubani, India

Contribution: Methodology, Visualization, Formal analysis

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Adireddy Ramesh

Adireddy Ramesh

Department of Electrical and Electronics Engineering, Aditya University, Kakinada, India

Contribution: Validation, Data curation, Resources

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Arindita Saha

Arindita Saha

Department of Electrical Engineering, Regent Education and Research Foundation Group of Institutions, Kolkata, India

Contribution: Visualization, Formal analysis, Resources

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Wulfran Fendzi Mbasso

Corresponding Author

Wulfran Fendzi Mbasso

Technology and Applied Sciences Laboratory, U.I.T. of Douala, University of Douala, Douala, Cameroon

Department of Biosciences, Saveetha School of Engineering, Saveetha Institute of Medical and Technical Sciences, Chennai, India

Applied Science Research Center, Applied Science Private University, Amman, Jordan

Correspondence: Naladi Ram Babu ([email protected])

Wulfran Fendzi Mbasso ([email protected])

Contribution: Writing - review & editing, Project administration, Supervision

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Pradeep Jangir

Pradeep Jangir

University Centre for Research and Development, Chandigarh University, Gharuan Mohali, India

Department of CSE, Graphic Era Hill University, Dehradun, India

Department of CSE, Graphic Era Deemed to be University, Dehradun, India

Centre for Research Impact & Outcome, Chitkara University Institute of Engineering and Technology, Chitkara University, Rajpura, Punjab, India

Department of Electrical and Electronics Engineering, J.J. Technology, Tiruchirappalli, Tamilnadu, India

Contribution: Supervision, Validation, Visualization

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Ahmed Hossam-Eldin

Ahmed Hossam-Eldin

Department of Electrical Power and Machines, Faculty of Engineering, Alexandria University, Alexandria, Egypt

Contribution: Writing - review & editing, Project administration, Supervision

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First published: 16 May 2025

ABSTRACT

As renewable energy sources (RES) are increasingly unified into multiarea power systems, automatic generation control (AGC) faces challenges such as frequency instability, longer settling times, and higher overshoot. While existing optimization techniques like Firefly (FF) and gray wolf (GW) suffer from slow convergence and local optima trapping, conventional controllers like FOPI, PIDN, TIDN, and TIDDN struggle to maintain stability under fluctuating load conditions. Fractional-Order Proportional-Integral with Tilt Integral Double Derivative and Filter (FOPI-TIDDN), a novel cascade controller optimized using the crow search (CS) algorithm, is proposed in this paper to overcome these issues. Furthermore, a two-area AGC framework incorporates realistic dish-Stirling solar thermal systems (RDSTS) and parabolic trough solar thermal plants (PTSTP), and the effects of these systems are examined under different patterns of solar insolation. Additionally, the study assesses how high voltage direct current (HVDC) tie-lines contribute to increased system stability. According to simulation data, the FOPI-TIDDN controller works noticeably better than others in terms of improved frequency regulation, faster settling time, and less overshoot. Compared to FF and GW approaches, the CS algorithm guarantees faster convergence. An ideal fixed-random solar insolation method and HVDC integration also improve system performance. The suggested method enhances renewable-integrated power systems' resilience, efficiency, and stability.

1 Introduction

Power systems (PS) experience abrupt fluctuations in demand that cause a disparity between generation and load, leading to frequency and power value variations. This can be mitigated by AGC [1]. The main goal of AGC is to establish a reliable control system that ensures a consistent frequency profile, and that can be achieved by effectively distributing power among generation and load sides. AGC aims to maintain stability by carefully managing the power flow [2, 3]. The single-area thermal works are foundation works and later expanded to multiarea systems [4]. Physical constraints like generation rate constraints (GRC) and time delays are considered [4, 5]. An AGC analysis on a multiarea thermal system encompassing hydro and gas units is studied by Parmar et al. [6].

The gradual decline in fossil fuel use and increased CO2 emissions have led to the use of renewable sources (RS). The idea of RS inclusion in AGC studies was first introduced in [7]. The most advanced methods can boost energy conversion efficiency while lowering their adverse environmental effects [8]. The RS is dominated by solar-wind energies [9]. The AGC study incorporating solar PV was presented by Bervani et al. [7]. The solar grid connection with thermal was demonstrated by Wang et al. [8]. The frequency parameter of a fusion inaccessible system with a parabolic trough collector-based solar thermal plant (PTSTP) was investigated by Das et al. [9], and its control strategy was demonstrated by Sharma et al. [10]. The concept of a dish-stirling solar thermal system (DSTS) with various solar insolations was presented by Rahman et al. [11]. Li et al. [12-14] suggested the narrow-speed operation of SCIG with energy devices for frequency regulation. Nonetheless, the PTSTP and RDSTS are not considered with conventional generation considering various types of solar insolation.

A rise in population causes a sharp increase in systems demand and can be overcome by interarea PS [15]. Also, an enhancement in interarea power transfer capability is necessary to accommodate the systems growing demand and this can be compensated by HVDC [16]. HVDCs offer effective power transfer capabilities and can be placed with existing systems [17, 18]. The AGC focus has historically been on two areas and further facilitates multiarea PS control. Moreover, the multiarea AGC studies with RDSTS and PSTSP integration, considering HVDC, have not been carried out.

There has been a significant emphasis on the secondary controller design in AGC. This focus led to the advance of secondary controllers. Classical IO controllers like I, PI, PID [19]; fractional such as FOPI and FOPID [20]; cascade such as FOPI − (1 + TD) [21], FOPID − (1 + TD) [22], fuzzy-IDD [23]; fuzzy-PID [24]; tilt controllers [25, 26]; adaptive fuzzy [27]; deep neural networks [28]; degree of freedom (DOF) controllers [29]; sliding mode [30] and so on, have been successfully implemented for the AGC study. A new cascade controller named FOPI-TIDDN has not been studied under AGC; thus, providing scope for further investigations.

To improve the AGC performance, various optimization techniques have been implemented. Conventional and heuristic algorithms optimize controller gains. Traditional techniques like gradient search and random search stick at local optima, and heuristic techniques like bacterial foraging [4, 23], genetic [5, 9], gray wolf [10], biogeography [11], sine-cosine [31], firefly [19, 32], flow direction [21], teaching learning [25], cuckoo search [29], flower pollination [33], barnacle optimizer [34], adopting jaya optimizer [35], global neighborhood algorithm [36], particle swarm [37, 38], salp swarm [39, 40], stochastic fractal search [41], Aquila [42], dragon fly [43] and learner behavior [44] provide global optima. A recent technique named crow search (CS) [45] works with the brainy behavior of crows, such as face recognition, tool usage, food search, effective communication, and so on. However, the CS technique is not utilized for the FOPI-TIDDN controller optimization.

The objectives are:
  • To demonstrate the effect of PTSTP and RDSTS with thermal systems.
  • To apply the CS algorithm to optimize controller parameters in PIDN, TIDN, and FOPI-TIDDN controllers.
  • To study the effect of various solar insolations.
  • Convergence comparison with gray wolf, firefly, and proposed CS technique.
  • To validate the impact of the HVDC.

1.1 Novelty and Contributions

From the above, the novelties are:
  • Evaluation performance of RDSTS and PTSTP in a two-area thermal system (TATS).
  • Designing a new FOPI-TIDDN controller for AGC studies of TATS.
  • Performance of thermal-RES system with a combination of various solar insulations.
  • Utilization of CS algorithm for synchronized enhancement of RDSTS parameter and FOPI-TIDDN controller.
The main contributions are:
  • A study was conducted in a TATS considering RDSTS and PTSTP.
  • A new controller termed FOPI-TIDDN was proposed by integrating RDSTS and PTSTP.
  • RDSTS and controller parameters are successfully optimized by the CS technique for the first time.
  • Efforts are made to analyze the impact of RDSTS and PTSTP at various solar insolations.

2 System Description

Investigations were carried out on a system with a capacity of 1:4 comprising thermal-RES units with HVDC integration. Area-1 comprises the PTSTP unit, and area-2 comprises RDSTS units with fixed and random solar insolations. The nominal values of the RDSTS, thermal, PTSTP, and HVDC tie-line models are from [4, 12, 23], respectively. The study and transfer function models of the investigated two-area systems comprising thermal, RDSTS, PTSTP, and HVDC units are in Figure 1a,b, respectively.

Details are in the caption following the image
(a) Study system model. (b) Study system's transfer function model.

3 The Proposed FOPI-TIDDN Controller

The FOPI-TIDDN controller aims to overcome the challenges associated with traditional fractional order and tilt controllers in handling complex power systemPS dynamics. Also, this controller is of cascade type with two loops that enhance dynamics over single loop control systems. The transfer functions of FOPI and TIDDN considering the real order of the integrator (λ), differentiator (μ), and a real number (n) are from [6, 7] and represented in Equations (1) and (2), respectively. The transfer function block diagrams are in Figure 2.
G FOPI ( s ) = K Pj + K Ij s λ j $$ {G}_{FOPI}(s)\kern0.5em =\kern0.5em {K}_{Pj}+\frac{K_{Ij}}{s^{\lambda j}} $$ (1)
G TIDDN ( s ) = K Tj ( s ) 1 / n j + K Ij s + K DDj s 2 N j s 2 + N j $$ {G}_{TIDDN}(s)\kern0.5em =\kern0.5em \frac{K_{Tj}}{(s)^{1/{n}_j}}+\frac{K_{Ij}}{s}+{K}_{DDj}{s}^2\left(\frac{N_j}{s^2+{N}_j}\right) $$ (2)
Details are in the caption following the image
The FOPI-TIDDN transfer function diagram.
CS algorithm optimizes the FOPI-TIDDN controller gains–RDSTS parameters. The Simulink model is developed in a MATLAB environment considering integral squared error (ISE) with constraints in Equations (3) and (4), respectively.
η ISE = 0 T Δ F j 2 + Δ P j - k 2 . dt $$ {\upeta}_{\mathrm{ISE}}=\int_0^{\mathrm{T}}\left\{{\left({\Delta F}_{\mathrm{j}}\right)}^2+{\left({\Delta P}_{\mathrm{j}\hbox{-} \mathrm{k}}\right)}^2\right\}.\mathrm{dt} $$ (3)
K Pj 1 , 0 K Ij 1 , 0 λ j 1 , 0 K Tj 1 , 0 n j 7 , 0 K TIj 1 , 0 K DDj 1 , and 0 N j 100 $$ {\displaystyle \begin{array}{cc}& \le {\mathrm{K}}_{\mathrm{Pj}}\le 1,0\le {\mathrm{K}}_{\mathrm{Ij}}\le 1,0\le {\lambda}_{\mathrm{j}}\le 1,\\ {}0& \le {\mathrm{K}}_{\mathrm{Tj}}\le 1,0\le {\mathrm{n}}_{\mathrm{j}}\le 7,0\le {\mathrm{K}}_{\mathrm{TIj}}\le 1,0\le {\mathrm{K}}_{\mathrm{DDj}}\le 1,\mathrm{and}\kern0.5em 0\le {\mathrm{N}}_{\mathrm{j}}\le 100\end{array}} $$ (4)

4 Crow Search (CS) Algorithm

A Askarzadeh [45] proposed CS grounded on the intelligence of crow's behavior, and its flow diagram is in Figure 3. It can recognize face tools usage and is greedy. They also steal, store food, and recall their hiding place. The hiding location (m) in position (p), size (n), and iteration (iter) are given by Equation (5).
X p , iter = X 1 p , iter , X 2 p , iter , . . , X d p , iter $$ \left[{\mathrm{X}}^{\mathrm{p},\mathrm{iter}}={\mathrm{X}}_1^{\mathrm{p},\mathrm{iter}},{\mathrm{X}}_2^{\mathrm{p},\mathrm{iter}},..\dots, {\mathrm{X}}_{\mathrm{d}}^{\mathrm{p},\mathrm{iter}}\right] $$ (5)
Details are in the caption following the image
Flowchart of CS.

Two possibilities occur in food search:

Crow-q does not recognize that crow-p is subsequent, and its walloping place is given by Equation (6).

Crow-q knows that crow-p is subsequent and flies to a random position, as in Equation (7).
X p , iter + 1 = X p , iter + r p × FL p , iter × m q , iter - X p , iter r q AP q , iter $$ {\mathrm{X}}^{\mathrm{p},\mathrm{iter}+1}=\left.\begin{array}{l}{\mathrm{X}}^{\mathrm{p},\mathrm{iter}}+{\mathrm{r}}_{\mathrm{p}}\times {\mathrm{FL}}^{\mathrm{p},\mathrm{iter}}\times \left({\mathrm{m}}^{\mathrm{q},\mathrm{iter}}\hbox{-} {\mathrm{X}}^{\mathrm{p},\mathrm{iter}}\right)\\ {}\kern3.4em {\mathrm{r}}_{\mathrm{q}}\ge {\mathrm{AP}}^{\mathrm{q},\mathrm{iter}}\end{array}\right\} $$ (6)
X p , iter + 1 = random position $$ {\mathrm{X}}^{\mathrm{p},\mathrm{iter}+1}=\mathrm{random}\ \mathrm{position} $$ (7)
where flight length (FL), random (r), and awareness probability (AP). The tuned CS technique parameters are noted in the Appendix A. The FOPI-TIDDN controller gains and RDSTS parameters are optimized by the CS technique considering ISE as the performance index and are in Equations (4) and (8).
0 T 1 1 , 1 T 2 4 , 0 T ds 1 1 , and 1 T ds 2 10 $$ 0\le {\mathrm{T}}_1\le 1,1\le {\mathrm{T}}_2\le 4,0\le {T}_{\mathrm{ds}1}\le 1,\mathrm{and}\ 1\le {T}_{\mathrm{ds}2}\le 10 $$ (8)

5 Simulation Results

The two-area thermal system with RDSTS, PTSTP, and HVDC lines considering CS optimized FOPI-TIDDN controller is regarded for the investigations and is in Figure 1b.

5.1 System Dynamics With PIDN, TIDN, and FOPI-TIDDN Controllers

Figure 1a (i) with thermal units are considered and are provided with secondary controllers like FOPI [8], PIDN [19], TIDN [25], TIDDN [41], and FOPI-TIDDN. Their values are simultaneously augmented using CS and are in Table 1a. The system dynamics corresponding to every controller are illustrated in Figure 4. The performance indices are listed in Table 1b. With the keen observation of the numerical values in Table 1b, and from Figure 4, it is apparent that the responses with the proposed FOPI-TIDDN controller outperform other controllers.

TABLE 1a. CS augmented PIDN, TIDN, and FOPI-TIDDN controller values considering SLP.
With FOPI controller KP1 = 0.8547 KI1 = 0.4758 λ1 = 0.9978 KP2 = 0.4751 KI2 = 0.8757 λ2 = 0.9785
With PIDN controller KP1 = 0.5161 KI1 = 0.6383 KD1 = 0.7868 N1 = 10.6597 KP2 = 0.3299 KI2 = 0.0936
KD2 = 0.1096 N2 = 21.9706
With TIDN controller KT1 = 0.6514 n1 = 3.5842 KI1 = 0.5812 KD1 = 0.9150 N1 = 19.5652 KT2 = 0.1096
n2 = 6.3435 KI1 = 0.2622 KD2 = 0.3299 N2 = 45.8975
With TIDDN controller KT1 = 0.5674 n1 = 4.7824 KI1 = 0.7584 KDD1 = 0.7584 N1 = 99.1425 KT1 = 0.4157
n1 = 7.5416 KI1 = 0.8324 KDD1 = 0.9745 N1 = 65.7412
With FOPI-TIDDN controller KP1 = 0.6661 KI1 = 0.7542 λ1 = 0.9856 KT1 = 0.3567 n1 = 3.5647 KI1 = 0.9652
KDD1 = 0.9364 N1 = 36.4585 KP2 = 0.4578 KI2 = 0.7745 λ2 = 0.9981 KT2 = 0.7714
n2 = 6.0125 KI2 = 0.5378 KDD2 = 0.4463 N2 = 57.2450
Details are in the caption following the image
System dynamics versus time of two-area thermal unit for FOPI, PIDN, TIDN, TIDDN, and FOPI-TIDN controllers. (a) ΔF1, (b) ΔF2, and (c) ΔPtie1-2.
TABLE 1b. Performance indices of responses in Figure 4.
Response Controller Settling time (s) Peak overshoot Peak undershoot (−ve)
ΔF1 FOPI [8] 45 0.042 0.099
PIDN [19] 42 0.040 0.0965
TIDN [25] 38 0.027 0.0965
TIDDN [41] 36 0.026 0.0800
FOPI-TIDDN 34 0.025 0.0794
ΔF2 FOPI [8] 44 0.024 0.090
PIDN [19] 42 0.022 0.085
TIDN [25] 40 0.016 0.072
TIDDN [41] 36 0.0154 0.070
FOPI-TIDDN 32 0.010 0.068
ΔPtie1-2 FOPI [8] 47 0.002 0.0130
PIDN [19] 45 0.002 0.0128
TIDN [25] 42 0.001 0.0127
TIDDN [41] 40 0.001 0.0125
FOPI-TIDDN 38 0.001 0.0124

5.2 System Dynamics With Random Load Pattern (RLP) Considering PIDN, TIDN, and FOPI-TIDDN Controllers

The controllers in Section 5.1 are utilized for the study with RLP in Figure 5a CS technique optimizes the gains and is in Table 2. Responses with RLP are plotted in Figure 5b–d. Upon thorough examination of system dynamics in Figure 5b–d, it is evident that dynamics with FOPI-TIDDN controller exhibit superior performance compared to those of other controllers.

Details are in the caption following the image
Dynamic of two-area thermal unit at RLP considering FOPI, PIDN, TIDN, TIDDN, and FOPI-TIDN controllers. (a) RLP, (b) ΔF1, (c) ΔF2 and (d) ΔPtie1-2.
TABLE 2. CS augmented PIDN, TIDN, and FOPI-TIDDN controller values considering RLP.
With FOPI controller KP1 = 0.5538 KI1 = 0. 4596 λ1 = 0. 9217 KP2 = 0. 9234 KI2 = 0. 2781 λ2 = 0. 2623
With PIDN controller KP1 = 0. 1942 KI1 = 0. 6356 KD1 = 0. 2471 N1 = 34.5782 KP2 = 0. 8327 KI2 = 0. 2927
KD2 = 0. 3896 N2 = 21.9706
With TIDN controller KT1 = 0.6514 n1 = 5.7245 KI1 = 0. 9516 KD1 = 0. 6341 N1 = 98.9601 KT2 = 0. 2172
n2 = 4.4097 KI1 = 0. 6767 KD2 = 0.9004 N2 = 64.5482
With TIDDN controller KT1 = 0. 4446 n1 = 6.0502 KI1 = 0. 2908 KDD1 = 0. 1325 N1 = 83.2482 KT1 = 0. 9261
n1 = 3.7603 KI1 = 0. 0381 KDD1 = 0. 1804 N1 = 32.4983
With FOPI-TIDDN controller KP1 = 0. 8324 KI1 = 0. 3016 λ1 = 0. 9613 KT1 = 0. 6624 n1 = 5. 3426 KI1 = 0. 7410
KDD1 = 0. 979 N1 = 68.5478 KP2 = 0. 5863 KI2 = 0. 8082 λ2 = 0. 9504 KT2 = 0. 4864
n2 = 5. 9058 KI2 = 0. 2331 KDD2 = 0. 8948 N2 = 29.6547

5.3 Comparisons of Convergence Characteristics Among Algorithms Like Firefly, Gray Wolf, and CS

The unequal thermal system is considered to examine the convergence characteristics of CS, firefly [29] and gray wolf [4] techniques. The FOPI-TIDDN values are augmented by the algorithms mentioned above and are in Table 3, and their respective convergence features are in Figure 6. In Figure 6, the convergence curves of firefly [29] and gray wolf [4] are produced and analyzed with CS. The ηISE values of every algorithm are examined, and it is witnessed that CS has a lower ηISE value. Critical observations expose the system with the CS technique converging over firefly and gray wolf algorithms.

TABLE 3. Optimized FOPI-TIDDN controller values considering firely, gray wolf, and CS algorithms.
With firefly [29] KP1 = 0.5686 KI1 = 0.5648 λ1 = 0.8956 KT1 = 0.4500 n1 = 4.2150 KI1 = 0.2180
KDD1 = 0.5018 N1 = 65.1245 KP2 = 0.7789 KI2 = 0.6485 λ2 = 0.9978 KT2 = 0.9601
n2 = 5.1245 KI1 = 0.3345 KDD2 = 0.9013 N2 = 21.0356
ISE = 0.006
Simulation Time = 284 s
With gray wolf [4] KP1 = 0.4856 KI1 = 0.8945 λ1 = 0.8555 KT1 = 0.7580 n1 = 4.2105 KI1 = 0.5241
KDD1 = 0.6645 N1 = 84.0125 KP2 = 0.8820 KI2 = 0.7456 λ2 = 0.8585 KT1 = 0.5463
n2 = 5.8231 KI1 = 0.7814 KDD2 = 0.8798 N2 = 66.1470
ISE = 0.004
Simulation Time = 255 s
With CS KP1 = 0.8521 KI1 = 0.7845 λ1 = 0.7425 KT1 = 0.3567 n1 = 3.5647 KI1 = 0.9652
KDD1 = 0.9364 N1 = 36.4585 KP2 = 0.7845 KI2 = 0.5485 λ2 = 0.9142 KT1 = 0.0.7714
n2 = 6.0125 KI1 = 0.5378 KDD2 = 0.4463 N2 = 57.2450
ISE = 0.0028
Simulation Time = 240 s
Details are in the caption following the image
Convergence characteristics comparison with firefly, gray wolf, and CS algorithms.

5.4 Selection of Performance Indices

System in Section 5.2 is considered and is provided with the best controller from Section 5.1 (FOPI-TIDDN) and the best algorithm from Section 5.2 (CS). CS optimizes the controller gains with ISE, ITSE, IAE, and ITAE as performance indices, considering one at a time, and responses are plotted in Figure 7. Results suggest that ISE exhibits better convergence with fewer error values over other indices.

Details are in the caption following the image
Comparison of various performance indices.

5.5 Integration of HVDC

Figure 1a (ii) considers the unequal thermal system unified with the HVDC and FOPI-TIDDN controller. The CS technique augments its gains. Table 4 lists optimum values and their responses are related to the AC system in Figure 8. From Figure 8, the dynamics with AC-HVDC clearly show their prominence over the AC tie-lines. Further, an interconnected HVDC system enhances system dynamics significantly. This improvement is because HVDC tie-lines are less susceptible.

TABLE 4. CS-optimized FOPI-TIDDN values with parallel AC-HVDC.
With AC-HVDC tie-lines KP1 = 0.7584 KI1 = 0.3213 λ1 = 0.9875 KT1 = 0.4723 n1 = 7.0251 KI1 = 0.6211
KDD1 = 0.7347 N1 = 20.1521 KP2 = 0.9952 KI2 = 0.4252 λ2 = 0.9685 KT1 = 0.2116
n2 = 6.4990 KI1 = 0.8469 KDD2 = 0.4351 N2 = 64.1150
Details are in the caption following the image
System dynamics with AC and AC-HVDC systems. (a) ΔF1, (b) ΔF2, and (c) ΔPtie1-2.

5.6 System Dynamics Under Various Patterns of Solar Insolation Considering RES

The unequal thermal-HVDC system is unified with RS like PTSTP and in area-1, 2, which are taken for investigation and are in Figure 1a (iii). The area participation factors (apf)s of RES-thermal systems are chosen as 0.45 and 0.55, respectively. The input for PTSTP and RDSTS is intermittent solar insolation in Figure 9.

Details are in the caption following the image
Various insolation of RS units.

The thermal-RES system is exposed to various groupings of insolations:

Case (a): Random and random.

Case (b): Random and fixed.

Case (c): Fixed and fixed.

Case (d): Fixed and random.

The FOPI-TIDDN controller is used, and CS augments its gains and RDSTS parameters in the above combinations and its values in Table 5. The corresponding dynamics with various combinations of solar insolations are compared in Figure 10 and show that the solar insolation combination of fixed and random in area 1–2 exhibits a better response than others.

TABLE 5. CS optimized FOPI-TIDDN values of the thermal-RS systems considering various solar insolation.
Case (a) KP1 = 0.6585 KI1 = 0.1245 λ1 = 0.9978 KT1 = 0.5945 n1 = 5.1205
KI1 = 0.8140 KDD1 = 0.7015 N1 = 85.1240 KP2 = 0.8852 KI2 = 0.4578
λ1 = 0.9978 KT2 = 0.5012 n2 = 3.2451 KI2 = 0.4385 KDD2 = 0.3104
N2 = 60.4503
Case (b) KP1 = 0.6645 KI1 = 0.4512 λ1 = 0.8879 KT1 = 0.5680 n1 = 5.4102
KI1 = 0.2478 KDD1 = 0.7820 N1 = 64.0528 KP2 = 0.7845 KI2 = 0.4532
λ2 = 0.8952 KT1 = 0.4780 n2 = 2.5478 KI2 = 0.4196 KDD2 = 0.4578
N2 = 22.4587
Case (c) KP2 = 0.6598 KI2 = 0.4561 λ2 = 0.4532 KT1 = 0.2300 n1 = 1.2450
KI1 = 0.8174 KDD1 = 0.8174 N1 = 25.4710 KP2 = 0.4578 KI2 = 0.3212
λ2 = 0.9978 KT2 = 0.3201 n2 = 4.1250 KI1 = 0.5410 KDD2 = 0.1208
N2 = 34.7809
Case (d) KP2 = 0.7832 KI2 = 0.5821 λ2 = 0.9965 KT1 = 0.6478 n1 = 5.1240
KI1 = 0.1820 KDD1 = 0.1047 N1 = 88.4510 KP2 = 0.6585 KI2 = 0.4856
λ2 = 0.9899 KT2 = 0.1780 n2 = 4.1205 KI1 = 0.4580 KDD2 = 0.3019
N2 = 18.2045
Details are in the caption following the image
Dynamic responses versus time of thermal-RES units considering various types of solar insolation.(a) ΔF1, (b) ΔF2, and (c) ΔPtie1-2.

5.7 Impact of Renewables

The effect of RES, such as a PTSTP and RDSTS in area-1, 2, on the system dynamics is examined. The finest solar insolation combinations (fixed and random) are delivered to the RS units. The thermal-RS system with an FOPI-TIDDN controller and the CS technique optimizes its gain parameters. The attained values with CS are noted in case (d) and its dynamics are shown in Figure 11.

Details are in the caption following the image
Dynamics of two-area thermal-RES units with AC-HVDC tie lines considering the best combination of solar insolation with and without PTSTP. (a) ΔF1, (b) ΔF2, and (c) ΔPtie1-2.

The effect of RES, like PTSTP and RDSTS integration, is highly noticeable when contrasted in a thermal system. Figure 11 shows that integrating the system with RES indicates a significant oscillation reduction.

5.8 Sensitivity Analysis

The thermal-RES system with FOPI-TIDDN with CS optimization is considered. Investigations are performed at ± 20% varied inertia and loading conditions and plotted in Figure 12. It is pragmatic that the FOPI-TIDDN controller exhibits almost the same responses.

Details are in the caption following the image
Dynamics of ∆F1 at varied (a) inertia and (b) loading conditions.

5.9 Stability Analysis

The thermal-RES-HVDC system with FOPI-TIDDN controller in Figure 1b is investigated for stability analysis by considering eigenvalue analysis. The input and output of each significant block in Figure 1b are under consideration and represented as state variables. Investigations are performed by considering “linmod” function in MATLAB. The obtained eigenvalues are noted in Table 6. It is apparent that eigenvalues are located on the left half of the s-plane. Also, the proposed system is supported by the negative values of the imaginary and real eigenvalues.

TABLE 6. Eigen values of thermal-RES-HVDC system with proposed FOPI-TIDDN controller.
−0.00137 + 0.000i −1.5100 + 0.000i −50.000 + 0.000i −46.100 − 2.2700i
−0.00169 + 0.000i −2.5700 + 0.000i −56.400 + 0.000i −47.700 + 4.060i
−0.00481 + 0.000i −3.3300 + 0.000i −100.00 + 0.000i −47.700  4.060i
−0.00500 + 0.000i −3.8800 + 0.000i −111.00 + 0.000i −50.100 + 4.880i
−0.00593 + 0.000i −9.0100 + 0.000i −390.00 + 0.000i −50.100  4.880i
−0.3330 + 0.000i −12.500 + 0.000i −1000.0 + 0.000i −52.800 + 4.350i
−0.5560 + 0.000i −28.000 + 0.000i −0.2080 + 0.0001i −52.800  4.350i
−0.7310 + 0.000i −31.600 + 0.000i −0.2080 + 0.0001i −55.100 + 2.400i
−1.0000 + 0.000i −45.500 + 0.000i −46.100 + 2.2700i −55.100  2.400i

6 Conclusion

A novel method has been obtained using the grouping of fixed-random insolation in a thermal-renewable system. The cascade FOPI-TIDDN controller is used for the first time, and its gain RDSTS parameters are optimized using a novel CS algorithm. System dynamics with the FOPI-TIDDN controller outperform FOPI, PIDN, TIDN, and TIDDN in performance indices. CS optimizes controller gains with a better convergence rate over cuckoo search and particle swarm techniques. Also, studies reveal that the FOPI-TIDDN controller with ISE shows better dynamics over other performance indices. Investigations reveal that insolations of fixed random in area-1 and 2 are the best over other combinations for renewable systems. Moreover, the effect of renewable in combination with AC-HVDC has been evaluated and assessed for two-area thermal systems. Sensitivity analysis suggests that the proposed FOPI-TIDDN controller is robust. Further, stability analysis suggests that the considered system is stable. Furthermore, this work can be extended to realistic scenarios.

Nomenclature

  • AGC
  • automatic generation control
  • CS
  • crow search
  • FF
  • firefly
  • FOPI-TIDDN
  • Fractional-Order Proportional-Integral With Tilt Integral Double Derivative and Filter
  • GRC
  • generation rate constraints
  • GW
  • gray wolf
  • HVDC
  • high voltage direct current
  • PS
  • power systems
  • PTSTP
  • parabolic trough solar thermal plants
  • RDSTS
  • realistic dish-stirling solar thermal systems
  • RES
  • renewable energy sources
  • Author Contributions

    Naladi Ram Babu: conceptualization, methodology, writing – review and editing. Pamarthi Sunitha: investigation, validation, writing – original draft. Ganesh Pardhu B. S. S.: investigation, validation, formal analysis. Sanjeev Kumar Bhagat: methodology, visualization, formal analysis. Adireddy Ramesh: validation, data curation, resources. Arindita Saha: visualization, formal analysis, resources. Wulfran Fendzi Mbasso: writing – review and editing, project administration, supervision. Pradeep Jangir: supervision, validation, visualization. Ahmed Hossam-Eldin: writing – review and editing, project administration, supervision.

    Conflicts of Interest

    The authors declare no conflicts of interest.

    Appendix A: System Nominal Parameters

    System Model: F = 60 Hz; Kpj = 120 Hz/pu MW; loading = 50%, Tjk, AC = 0.086 pu MW/rad; Dj = 8.33 × 10-3 pu MW/Hz; Hj = 5 s; Rj = 2.4 pu MW/Hz; Bi = βj = 0.425 pu MW/Hz; Tpj = 20 s; apf11 = apf21 = apf31 = 0.45; apf12 = apf22 = apf32 = 0.55; SLP = 1%; a12 = −Pr1/Pr2 = −1000/4000 = −1/4; a23 = −Pr2/Pr3 = 4000/8000 = −1/4; a31 = −Pr3/Pr1 = 8000/1000 = −8/1.

    Thermal System: Tgj = 0.08 s; Ttj = 0.3 s; Trj = 10s; Krj = 0.5 s.

    Parabolic Trough Collector Base Solar Thermal Plant: Ks = 1.8; Ts = 1.8 s; Tgsj = 1.0 s; Ttsj = 3.0 s.

    High-Voltage Direct Current: KDC = 0.5; TDC = 0.03 s.

    Crow Search Technique: Flight length = 0.2, Awareness Probability = 0.1, flock size = 50, iteration size = 100.

    Data Availability Statement

    The data that support the findings of this study are available from the corresponding author upon reasonable request.

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