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Article

Analysis of Power System Cost Evolution Characteristics Under Different Thermal Power Substitution Modes

1
School of Electrical Engineering, Northeast Electric Power University, Jilin 132012, China
2
Electric Power Research Institute, State Grid Jilin Electric Power Co., Ltd., Changchun 130021, China
*
Author to whom correspondence should be addressed.
Energies 2026, 19(9), 2174; https://doi.org/10.3390/en19092174
Submission received: 28 March 2026 / Revised: 19 April 2026 / Accepted: 29 April 2026 / Published: 30 April 2026
(This article belongs to the Section F1: Electrical Power System)

Abstract

With the continuous decline in the cost of renewable energy such as wind power and photovoltaic power generation, the economic competitiveness in the power supply structure is increasing, and traditional thermal power units are gradually being replaced, resulting in a profound adjustment of the power supply structure. However, the unclear alternative between units may lead to system redundancy configuration or power supply shortage. At the same time, the volatility of the new energy output and the flexible allocation of resources and other factors work together, resulting in the cost of the power system showing complex evolution characteristics. Therefore, it is of great significance to study the evolution of system cost in the process of thermal power substitution. This paper first analyzes the internal mechanism of the cost change of the new power system. Second, the cost accounting model of the power system is constructed to reveal the relationship between ‘thermal power substitution mode-system cost’ in the process of thermal power installed capacity substitution. Finally, the Garver-6 system is taken as an example to carry out simulation analysis, solve the optimal thermal power substitution mode under different renewable energy penetration rates, and explore the evolution law of system cost. The results of the example show that with the increase of renewable energy penetration, the total cost of the system first decreases and then increases, and the optimal substitution method is ‘unit thermal power to replace more renewable energy’.

1. Introduction

In the development stage of the traditional power system, the power structure is dominated by fossil fuel units. The power generation side exhibits strong controllability and stability, and the system operation follows the typical “generation follows load” scheduling logic, resulting in a relatively stable system cost structure [1,2]. Historically, provinces such as Shanxi, Shaanxi, Liaoning, Jilin, and Heilongjiang have had abundant coal reserves and a well-developed infrastructure, which were the primary prerequisites for the development of thermal power plants in Northeast and Central China. It is also worth noting that, historically, thermal power plants in China were developed using a condensing cycle. By the end of 2025, the installed capacity of renewable energy in China had exceeded 2.159 billion kW, accounting for 59.2% of the country’s total installed power generation capacity, surpassing thermal power for the first time to become the dominant power source in the power system [3]. The high penetration of wind and photovoltaic power has gradually shifted the power supply side from being predominantly controllable to predominantly stochastic. The volatility and uncertainty of the renewable energy output have been significantly enhanced, and the system operation logic has gradually evolved from “generation follows load” to a new paradigm of “source–load bidirectional interaction” and even “load follows generation” [4,5]. Meanwhile, the large-scale integration of new resources such as distributed generation and energy storage has progressively transformed the power system structure from a centralized network with traditional unidirectional power flow to a complex network system characterized by multi-node, multi-agent collaborative interaction [6,7]. This structural transformation of the new power system, by increasing the demand for flexibility resources and strengthening real-time balancing and coordination management, has shifted the system costs from being stable and controllable to being highly complex and heavily dependent on flexibility.
The above structural changes do not simply reduce the overall cost of the system but profoundly reshape the cost structure of the power system. On the one hand, renewable energy has a low marginal generation cost. As its installed capacity continues to expand, it has gradually become the dominant power source in the new power system. The share of fuel costs in the total cost of power generation is gradually decreasing [8], leading to a reduction in the cost of electricity production. However, the change in the system’s energy structure introduces power and energy balance issues. To cope with the power deviations caused by fluctuations in renewable energy output, the system’s demand for flexibility resources has increased significantly. This includes increased investments in energy storage power and capacity allocation, flexible retrofitting of thermal power plants, and the construction of peak-shaving and frequency-regulation resources. Reference [9] effectively alleviates the long-term supply–demand imbalance risk in the system by constructing a flexibility resource allocation mechanism for managing long-term supply–demand imbalance risks. Reference [10] constructs a source–storage–transmission joint planning model, improving the overall regulation capability of the system through energy storage participation. Reference [11] points out that when a sudden flexibility shortage occurs in the system, energy storage can achieve energy throughput and regulation compensation through emergency dispatch, thereby alleviating system operation risks. China’s national power grid currently has approximately 30 Ultra-High Voltage Direct Current (UHVDC) lines, which facilitate the integration of large-scale solar and wind power plants by enabling long-distance, low-loss transmission of renewable energy from resource-rich regions to load centers.
At the same time, the centralized development of wind and solar power, together with the need for large-scale long-distance transmission, has revealed insufficient grid strength in the existing system. Existing transmission corridors in some regions struggle to meet power transmission demands, making grid expansion and transmission capacity enhancement important supporting measures for renewable energy integration. References [12,13] avoid waste in energy storage investment and redundancy in line expansion by optimizing the coordinated planning of energy storage and transmission lines, effectively improving weak links in the grid. Based on a mixed-integer linear programming (MILP) approach, References [14,15,16] minimize transmission investment costs while ensuring line transmission capacity.
Therefore, compared with the traditional power system, the cost change in the new power system is a systematic reconstruction process driven jointly by the transformation of the power supply structure and the change in system operation mechanisms [17,18]. It is not merely a simple substitution of traditional energy sources (such as coal and natural gas) with higher marginal costs by renewable energy sources (such as wind and solar) with very low marginal costs. The shift in system operation mode caused by the change in system structure makes the calculation of system costs more complex. In this context, characterizing the evolution of system costs under different renewable energy penetration rates and revealing the impact of flexibility resource allocation on cost changes have become key issues in new power system research. However, existing research mostly focuses on the economic analysis of a single technology or static scenario comparisons, lacking a systematic characterization of the dynamic evolution path of overall system costs. Based on this, it is necessary to construct a multi-scenario, multi-agent collaborative analysis framework to systematically study the reconstruction process and evolution mechanism of the power system cost structure under high renewable energy penetration, thereby providing a decision-making basis for power structure optimization and system cost control under high renewable energy penetration.
To clarify the cost composition structure of the new power system, distinguish the cost shares of its various components (power sources and regulation resources), analyze the factors driving system cost changes, and thereby understand the evolution law of system costs during renewable energy development, this paper provides path guidance for power structure optimization and regulation resource allocation under the new power system. Specifically, this paper carries out the following:
(1)
Analyzes the factors driving system cost changes
(2)
Defines the substitution method between traditional thermal units and renewable energy
(3)
Constructs a cost accounting model for the power system
(4)
Uses the Garver-6 system as a case study to conduct simulation analysis, determine the optimal thermal power substitution mode under different renewable energy penetration rates, and explore the evolution law of system costs.

2. Analysis of System Cost Change Motivation

To clarify the evolution of system costs during increasing renewable energy penetration, it is first necessary to identify the factors influencing system costs. This section examines four key aspects: power system transformation, flexibility requirements under different renewable penetration scenarios, the impact of transmission lines on system flexibility and costs, and the determination of thermal power substitution modes. The objective is to clarify what factors affect system costs and how they evolve. A detailed point-by-point analysis is provided below.

2.1. Energy Structure Transformation

In the new power system, the “source” side, i.e., the electricity production stage, undertakes the core function of converting primary energy into electrical energy and connecting it to the power grid. As shown in Figure 1 (drawn by the authors), the profound transformation of the energy structure from traditional fossil fuels to high-proportion renewable energy is becoming one of the key driving factors behind system cost changes.
With the acceleration of the energy transition, the energy structure of the new power system is undergoing profound changes. The installed capacity of clean energy sources such as wind and solar power is increasing rapidly, gradually replacing traditional thermal power generation. However, wind and solar power are characterized by intermittency, volatility, and randomness, and cannot generate power on demand like traditional sources. Consequently, the power supply has shifted from being deterministic to uncertain. When renewable energy generation is high, it cannot be fully absorbed by the power grid, resulting in curtailment of wind and solar power. Conversely, during periods with no wind or sunlight, or during peak demand, power shortages occur. Thus, curtailment and shortage coexist.
To address these issues, the new power system requires more flexible resources, such as battery energy storage and pumped storage hydropower. The investment and operational costs of these resources are very high. As the share of renewable energy increases, the demand for such resources also grows, which significantly increases the overall system cost. The transformation from the traditional power system to the new power system is fundamentally a shift from a centralized dispatch mode dominated by controllable power sources to a multi-energy complementary mode with large-scale renewable energy integration. This transformation also changes the system’s operation mode and cost structure.

2.2. Flexibility Analysis of New Power System

Under different renewable energy penetration rates, the net load curve exhibits significant variation, which in turn imposes differentiated requirements on the regulation capability of flexible resources. Taking a typical 24 h operating day of the new power system as an example, this study reveals the factors influencing system cost changes by comparing net load and curtailment characteristics across various penetration rates.
As shown in Figure 2, in the low penetration rate stage illustrated in Figure 2a, as the renewable energy penetration rate increases, thermal power remains the absolute main body, undertaking the base load and most of the flexibility tasks. At this stage, system flexibility is abundant, generation costs decrease, and the system cost shows a declining trend.
When the renewable energy penetration rate reaches 50%, as shown in Figure 2b, the net load becomes negative and falls below the thermal power output lower bound. At this point, relying solely on thermal power peak regulation can no longer meet system flexibility requirements, and curtailment occurs. Additional flexibility resources are needed to regulate the power balance, leading to an increase in system cost.
As the renewable energy penetration rate rises to 70% or even higher, as shown in Figure 2c,d, thermal power gradually transforms from a base load power source to a regulating power source, with some units being retired. During specific periods, such as hours 2–4, even when the thermal power output has been reduced to its minimum, the wind and solar output still exceed the load, resulting in mandatory curtailment. During hours 22–24, insufficient upward flexibility occurs, and part of the load cannot be supplied. The source–load temporal mismatch intensifies, and curtailment and shortage occur simultaneously within a single day. More flexibility resources need to be added to shift the power and reduce the occurrence of imbalance events, leading to a significant increase in system cost.
Through the analysis of the above four daily penetration rate scenarios, it can be seen that with the increase in renewable energy penetration, although clean, low-cost wind and solar power have replaced relatively expensive thermal power, the decline in thermal power installed capacity has led to a serious shortage of system flexibility. Flexibility resources must be allocated to address curtailment and shortage in the system. The resulting increase in regulation cost leads to a change in the total system cost.

2.3. Analysis of Line Expansion of New Power System

In the process of the transformation of the new power system, more and more new power sources such as distributed photovoltaic and distributed wind power are beginning to be connected to the transmission grid. This results in the traditional ‘centralized power generation, long-distance transmission’ model changing. The new model should not only achieve local balance but also achieve wide-area mutual assistance.
This change has also led to a strategic shift in the expansion of the transmission network. The focus of grid investment is changing. In the traditional power system, the investment is mainly focused on large thermal power and hydropower bases. However, the focus of investment in the new power system has shifted to areas with rich scenery resources but they may be far away from the power center. These areas are also known as new energy hubs. The extension and strengthening direction of transmission lines are densely directed to the collection stations of large-scale wind power and photovoltaic clusters. At the same time, in order to integrate the distributed power supply, it is also very important to strengthen the transmission channel and regional networking lines of the original distribution network.
As shown in Figure 3, unlike thermal power with stable and controllable output, wind and solar power are characterized by intermittency and strong randomness. To ensure that all electricity can be transmitted and utilized during concentrated output periods, and to avoid curtailment caused by network congestion, line planning cannot be based solely on average transmission power. Instead, it is necessary to increase the number of line circuits and coordinate them with energy storage to ensure transmission capacity while reducing imbalances on both the source side and the load side. Consequently, system costs will change; increasing the number of transmission line circuits raises grid investment, while reducing imbalances caused by insufficient transmission capacity lowers system penalty costs.

2.4. Determination of the Thermal Power Substitution Mode

The replacement ratio of thermal power installed capacity is also a factor affecting system cost. If thermal power replaces less new energy, the phenomenon of power abandonment may occur; if more new energy is replaced, the load may not be supplied. In this paper, alternative mode 2 is set up: with the increase of the renewable energy penetration rate by 10%, the thermal power will reduce the load supply by 10%, so as to calculate the power generation capacity of the thermal power and calculate the installed capacity of the thermal power under different penetration rates with equivalent utilization hours of 4500 h. By analogy, the installed capacity of thermal power units under different alternative modes is obtained, as shown in Table 1.

3. Power System Cost Accounting Model and Cost Evolution

To characterize the evolution of power system costs under increasing renewable energy penetration, this chapter develops a comprehensive optimization model for power system cost accounting. The model is formulated within a Mixed Integer Linear Programming (MILP) framework to ensure computational tractability while accurately capturing the operational characteristics of thermal power units, renewable generation, and energy storage systems. This paper uses a DC power flow model. Therefore, the model considers only active power and voltage phase angles. All calculations are performed with a mandatory active power balance. Reactive power and voltage magnitude variations at nodes are not considered. This is a common simplification in power system expansion planning studies. This study adopts a deterministic modeling framework. Hourly wind and solar generation profiles, as well as load profiles, are treated as known exogenous inputs.

3.1. Power System Cost Accounting Model Framework

The framework of the power system cost accounting model established in this paper is illustrated in Figure 4. As shown, the formulation comprises three core cost components—investment cost, operation cost, and penalty cost—subject to a set of technical and operational constraints.
The model established in this chapter serves as the theoretical foundation for the Garver-6 system case study presented in Section 4. Detailed specifications of variables, parameters, and equations are provided in the subsequent subsections.

3.2. Objective Function

The proposed model aims to minimize the total annualized system cost under varying renewable energy penetration rates. The total cost comprises three components: annualized investment cost for generation and storage capacity, system operation cost including fuel and maintenance expenditures, and penalty cost incurred from load shedding and renewable energy curtailment. The objective function is formulated as follows:
min C plan = C plan inv + C plan oper + C plan punish
where C plan inv , C plan oper , and C plan punish denote the annualized investment cost, system operation cost, and penalty cost, respectively. The detailed formulations of these three components are provided in Equations (2)–(4).

3.2.1. Annualized Investment Cost

The annualized investment cost C plan inv converts the upfront capital expenditure of generation and storage capacity into an equivalent annual cost over the planning horizon, which is expressed as follows:
C plan inv = η ( 1 + η ) N s ( 1 + η ) N s 1 ( c gen inv P gen + c wind inv P wind + c sun inv P sun + c pess inv P e + c ess inv E e )
where c gen inv , c wind inv , c sun inv , c pess inv and c ess inv are the unit investment cost coefficients of thermal power, wind, photovoltaic, energy storage power and energy storage capacity, respectively (yuan/kW or yuan/kWh); Pgen, Pwind, Psun, and Pe denote the installed capacity of each technology (kW); Ee is the energy storage capacity (kWh); η is the discount rate (5%); Ns is the planning horizon (15 years).

3.2.2. System Operation Cost

The system operation cost C plan oper accounts for the annual expenditures on fuel consumption, environmental treatment, and operation and maintenance, which is given by the following:
C plan oper = ( α g + β g ) P g , t + P gen R g + P wind R w + P sun R s + ( c pess inv P e + c ess inv E e ) R e
where αg and βg are the fuel and environmental cost coefficients of thermal units (yuan/kWh); Pg,t is the output of the thermal power unit at time t; Rg, Rw, Rs, and Re are the operation and maintenance cost coefficients (yuan/kW).

3.2.3. Penalty Cost

The penalty cost C plan punish captures the economic penalties associated with power shortage and renewable energy curtailment, which is formulated as follows:
C plan punish = δ d D n , t cut + δ w P w , t cut + δ pv P p v , t cut     t T
where δd, δw, δpv are the penalty coefficients for power shortage, wind curtailment, and photovoltaic curtailment, respectively (yuan/kWh); D n , t cut is the power shortage at time t (kW); P w , t cut , P p v , t cut are the curtailed wind and photovoltaic power at time t (kW).

3.3. Constraints

The minimization of the objective function is subject to a set of technical and operational constraints that ensure the feasibility and reliability of the system operation. These constraints govern power balance, generation limits, ramping capabilities, transmission capacity, energy storage dynamics, and network expansion limits. The detailed formulations are presented in the following subsections.

3.3.1. Power Balance Constraint

The power balance constraint ensures that generation and storage discharge equal load and storage charging at every time step, accounting for power shortage and renewable curtailment:
P g , t + P w , t + P p v , t + P e , t dis P e , t c h a = D n , t D n , t cut P w , t cut P p v , t cut     t T
where Pg,t is the output of the thermal power unit at time t; Pw,t and Ppv,t are the wind and photovoltaic power outputs at time t; P e , t dis and P e , t c h a are the discharging and charging power of energy storage at time t; Dn,t is the system load at time t; T is the set of time periods.

3.3.2. Generation Limits of Thermal Power Units

The output of each thermal power unit is constrained within its technical minimum and maximum limits:
P g min P g , t P g max     t T
where P g min and P g , t max are the minimum and maximum output limits of the thermal power unit.

3.3.3. Ramping Constraints of the Thermal Power Unit

The ramping constraints limit the rate at which thermal units can increase or decrease their output between consecutive time periods:
μ P gen P g , t + 1 P g , t μ P gen     t T
where μ is the ramping rate coefficient of the thermal power unit (50%).

3.3.4. Energy Storage Constraints

Lithium-ion battery energy storage is considered as the primary flexibility resource. Lithium-ion batteries offer advantages including fast response, high energy density, and high cycle efficiency, making them the most widely deployed electrochemical storage technology in modern power systems. The operation of energy storage is governed by power limits, state-of-charge dynamics, and daily energy balance requirements:
0 P e , t dis P e   ,   0 P e , t cha P e     t T
S O C t = S O C t 1 + η e P e , t cha P e , t dis / η e     t T
S O C min S O C t S O C max     t T
S O C ( 24 ) = S O C i n i
where P e , t dis and P e , t cha represent the discharging power and charging power of the energy storage; ηe represents the charging/discharging efficiency of the energy storage (taken as 0.95); SOCt and SOCt−1 represent the state of charge of the energy storage at time t and time t − 1; SOCmin and SOCmax represent the minimum and maximum state of charge limits of the energy storage (taken as 10% and 90%); SOCini represents the initial state of charge of the energy storage (taken as 50%).

3.3.5. Available Transfer Capability Limitation of Lines (DC Power Flow)

The power flow on each transmission line is governed by the DC power flow model and must respect the line’s thermal capacity limits (The supplementary content is shown in Appendix A):
B θ t = P g , t + P w , t + P p v , t + P e , t dis P e , t c h a D n , t     t T
where B is the node admittance matrix (susceptance matrix); θt is the vector of nodal voltage phase angles at time t.

3.3.6. New Line Construction Constraints

The number of new transmission lines that can be constructed is subject to corridor capacity limits:
0 x i j new N i , j max     ( i , j ) Ω line
where x i j new is the number of new transmission lines constructed in corridor (i, j); N i , j max is the maximum allowable number of new lines in that corridor; Ωline is the set of candidate transmission corridors.

3.3.7. Transmission Line Power Flow Constraints

The power flow on each transmission corridor is limited by the total capacity of existing and newly constructed lines:
P i j , t ( x i j 0 + x i j new ) P i j max     ( i , j ) Ω line t T
where Pij,t is the actual power flow on corridor (i, j) at time t; P i j max is the maximum capacity of a single transmission line in that corridor, x i j 0 is the number of existing lines; x i j new is the number of newly constructed lines.

3.4. Solving Procedure

The solution methodology employs a two-level framework that couples scenario-based parameter analysis at the outer level with Mixed Integer Linear Programming (MILP) optimization at the inner level. The outer level systematically varies the renewable energy penetration rate to characterize cost evolution trajectories. For each penetration scenario, the inner level solves a full MILP problem to optimality using the Gurobi solver 10.0, determining the optimal thermal capacity, energy storage configuration, and hourly dispatch decisions. The overall solution framework is illustrated in Figure 5.
The solving steps are as follows.
  • Step 1: Data Input and Preprocessing
Input 8760 h system data of wind power, photovoltaic generation, and load. Normalize the wind power output, photovoltaic output, and load profiles. Perturb (or adjust) the renewable energy penetration rate to the initial stage r k (e.g., 0%). Complete data preprocessing to obtain time-series wind/PV output curves and time-series load profiles.
  • Step 2: Optimization Model Formulation
Formulate an optimization model aimed at minimizing total system cost. The objective function comprises three components: annualized investment cost, system operation cost, and penalty cost. Constraints include power balance constraints, thermal power unit constraints, energy storage constraints, and transmission expansion constraints. The model is solved using the Gurobi optimizer via Mixed Integer Linear Programming (MILP).
  • Step 3: Time-Series Production Simulation
Perform time-series production simulation to evaluate the system operating state under the current penetration scenario.
  • Step 4: Scenario Iteration Check
Check whether all predefined penetration rate scenarios have been evaluated. If No, update to the next penetration scenario r k + 1 and return to Step 3. If Yes, proceed to Step 5.
  • Step 5: Output Results
Output the optimal planning scheme for each penetration scenario, including the following: optimal thermal power substitution modes (optimal thermal installed capacity), optimal energy storage configuration, total system cost, curtailment and shortage metrics, and time-series power output of all generation units.
  • Step 6: Results Analysis
Compile the results across all scenarios and analyze the evolution characteristics of the system costs with increasing renewable energy penetration. Complete the results analysis.

4. Case Study

To validate the effectiveness of the proposed cost evolution framework and to investigate the mechanism by which renewable energy penetration influences system costs, this section presents a comprehensive case study based on the modified Garver-6 test system. The analysis encompasses multiple renewable energy penetration rate scenarios, progressively transitioning from a thermal-dominated baseline configuration to a high-renewable future scenario. The calculation parameters are first provided, followed by a comparison of different thermal power substitution modes and the determination of the optimal thermal substitution strategy. Finally, the system cost evolution characteristics are derived and analyzed.

4.1. Base Data

In order to analyze the influence of the change of the renewable energy penetration rate on the total cost of the power system and obtain the evolution path of the system cost, this paper uses the measured wind and solar load data of a province in Northeast China in recent years to analyze as an example.
Perturb the renewable energy penetration rate with 10% as the step size, simulate the system cost, and analyze its change trend under the condition of penetration rate from 0% to 100% through time series production simulation. The planning period of this paper is 15 years, and the discount rate is 5%. The calculation parameters used are shown in Table 2.

4.2. Analysis of Cost Evolution Trend Under a 1:1 Replacement Scenario

Through the above steps, the production simulation is solved under different renewable energy penetration rates, and the cost composition and changes in the system are obtained as shown in Figure 6.
From Figure 6, it can be seen that with the increase of penetration rate, the total cost of the system shows a trend of decreasing first and then increasing. At 30%, the total cost is the lowest at 334.86 billion yuan. The main reason is that renewable energy sources with relatively low costs such as wind power and photovoltaics are connected to the power system, resulting in the compression of the output space of the thermal power units and the continuous decline of the thermal power costs. It decreased from yuan 37.23 billion at the initial 0% penetration rate to yuan 0 billion at the 100% penetration rate. Due to the 100% penetration rate, the installed capacity of thermal power is 0, thermal power no longer provides electricity, so the cost is 0 billion yuan.
When the penetration rate is low, it is not necessary to configure short-term energy storage or configure a small amount of short-term energy storage to maintain the stability of the system, and there are fewer violations such as load shedding; that is, the increase in the adjustment cost of wind, light, and power connected to the system is less than the reduction in the cost of the thermal power output. Therefore, the total cost of the system decreases from 374.85 billion yuan at 0% to 334.86 billion yuan at 30%, a total decrease of 3.999 billion yuan; with the gradual increase of penetration rate, the output of wind power and photovoltaic power in the system increases. It is necessary to configure more short-term energy storage and expand more lines to increase the flexibility of the system, ensure the smooth transmission of power, and reduce the lack of peak shaving and the blocking of transmission lines. With the increase of the penetration rate, the energy storage cost increases monotonously, reaching a maximum of 9.49 billion yuan when the penetration rate is 100%. The number of line expansions increases, and the expansion center of gravity shifts to wind power and photovoltaic nodes. At the same time, the adjustment cost and the cost of scenery construction have risen sharply, and there are also more load shedding phenomena, so the total cost of the system has increased by up to 230.696 billion yuan.
Based on the above analysis, under this thermal power substitution mode, the total cost of the system and the cost of electricity are first decreased and then increased, and the minimum value is obtained at 30% penetration rate. On the one hand, wind power and photovoltaic renewable energy, as a ‘double-edged sword’, reduce the system cost while causing the system adjustment cost to rise. As the penetration rate increases, the difference between the two increases, and the total system cost increases; on the other hand, renewable energy is gradually replacing thermal power, the installed capacity of thermal power is declining, the system has no power supply, and there is no flexible resource to solve the problem of long-term abandonment and shortage of electricity. Therefore, a large number of abandonments and shortages of electricity have a great impact on the system cost.

4.3. Comparative Analysis of Cost Evolution Law Under Different Alternative Methods

According to the comparison between mode 1 and mode 3 as shown in Table 1, the influence of different thermal power substitution modes on system cost is analyzed.
From Figure 7, it can be seen that under the two different thermal power substitution modes, the change of the system cost composition is quite different, but the overall change trend is first to decrease and then increase, and both reach the lowest value at 30% penetration rate, which is 362.26 billion yuan and 339.21 billion yuan respectively.
(1)
Analysis of system cost change in mode 1
First, in mode 1, because the installed capacity of the thermal power units is sufficient and does not change with the increase of the renewable energy penetration rate, the system is flexible enough at this time. As the main provider of flexibility, the thermal power can increase or decrease the output as the system needs, and the cost of thermal power is still an important part of the total cost of the system, accounting for a high proportion. However, due to its limitation of minimum output, the downward flexibility of the system is low, and problems such as inability to absorb wind power and photovoltaics occur at a high penetration rate, resulting in a continuous increase in the system’s abandonment rate and a monotonous increase in the abandonment penalty. At 100% penetration rate, it is up to 25.32 billion yuan; however, the system has sufficient upward flexibility, and no power shortage occurs. The specific energy storage configuration and line expansion are shown in Table 3 and Table 4. Although the installed capacity of thermal power is sufficient and the system flexibility is high, the configuration of energy storage is still an effective means to solve the unbalanced power, and it is also of least cost. The focus of line expansion is still shifting to renewable energy nodes.
(2)
Analysis of system cost change in mode 3
In mode 3, it can be seen from Figure 7b that in the process of gradually reducing the installed capacity of thermal power, the power shortage in the system is aggravated. When the penetration rate is 70% and above, the power shortage penalty has a huge impact on the total cost of the system, accounting for the most cost. As the penetration rate increases, the upward and downward flexibility in the system decreases, and the penalty for power abandonment also increases. As a flexible resource, short-term energy storage still cannot solve the uneven distribution of renewable energy power in the season and can only solve the flexibility shortage on some days, resulting in a sharp rise in cost after the penetration rate is 30%. The specific energy storage configuration and line expansion are shown in Table 5 and Table 6.
In summary, under different thermal power installed capacity substitution methods, the cost evolution law of the system is similar, showing a trend of decreasing first and then increasing. At a low penetration rate, the total system cost of different thermal power installed capacity substitution methods is less different. The main reason is that the thermal power installed capacity is high and basically meets the load. At the same time, the wind power photovoltaic output is low, and the system just needs to pay less adjustment cost to ensure the system power balance and to reduce the occurrence of unbalanced events. With the further increase of the penetration rate, the different alternatives begin to appear, which is embodied in the contradiction between the installed capacity of thermal power and the punishment of power abandonment and power shortage. When the installed capacity of the thermal power is redundant, the system abandonment penalty is high due to the influence of the minimum output constraint. When the installed capacity of the thermal power is insufficient, the load cannot be supplied, and the penalty of system power shortage is high.

4.4. Cost Evolution Trend Under Optimal Thermal Power Substitution Mode

Considering the relationship between the replacement ratio of thermal power installed capacity and the system cost under different penetration rates, the optimal replacement ratio of thermal power installed capacity and the total cost are obtained as shown in Table 7 and Figure 8 by solving all the above methods.
Through Table 7 and Figure 8, it can be seen that the trend of the total cost of the system under the optimal replacement ratio of thermal power installed capacity is still first decreasing and then increasing, and the lowest is 334.9 billion yuan when the penetration rate is 30%. However, in the process of rising system costs, it can be seen that the installed capacity of thermal power is almost maintained between 10–12 million kW. Although having a large number of wind power and photovoltaic access sources, the thermal power installed capacity to maintain a high level to increase the flexibility of the system is still a good choice; the thermal power installed capacity alternative to the unit capacity of thermal power to replace more renewable energy change also shows the importance of thermal power when the flexibility of resources is limited under a high penetration rate. The specific energy storage configuration is shown in Table 8. As a flexible resource, energy storage can solve some unbalanced events, but the cost of energy storage is increasing steadily.

4.5. Sensitivity Analysis of Key Parameters

To assess the robustness of the identified cost evolution characteristics and optimal thermal power substitution modes, a sensitivity analysis was conducted with respect to the investment costs of wind and photovoltaic generation. Two additional scenarios were considered.
Scenario S1: Wind and PV investment costs are reduced by 10% relative to the reference case.
Scenario S2: Wind and PV investment costs are reduced by 20% relative to the reference case.
The reference case uses the original cost assumptions as presented in Table 2.
Figure 9 presents the evolution of the total annualized system cost across the three scenarios as renewable penetration increases from 0% to 100%. The following observations can be made.
In all three scenarios, the system cost exhibits the same characteristic “U-shaped” trajectory—initially decreasing as low-cost renewable energy displaces thermal generation, reaching a minimum, and subsequently increasing as flexibility resource requirements (energy storage and transmission expansion) become dominant. The overall shape of the cost curve remains unchanged, confirming that the underlying cost structure is driven primarily by the physical constraints of the system rather than the absolute level of the renewable investment costs. As expected, reducing wind and PV investment costs lowers the total system cost across all penetration levels. The magnitude of the reduction is approximately proportional to the share of renewable investment in the total cost. Delay of the optimal penetration point: The penetration rate at which the minimum system cost occurs shifts to the right as the renewable costs decrease. Specifically, the optimal penetration rate increases from 30% in the reference case to 40% in S1 and S2. This indicates that lower renewable costs make higher penetration levels economically attractive before flexibility constraints begin to dominate.
Table 9 compares the optimal thermal power substitution mode selected under each renewable penetration level for the three cost scenarios.
The optimal substitution mode remains largely consistent across the three scenarios, particularly at low and high penetration extremes. This suggests that the choice of substitution strategy is governed more by system flexibility constraints than by renewable cost assumptions.
Minor differences are observed in the intermediate penetration range (50–60%), where the cost differential between adjacent substitution modes is relatively small. In this region, Scenarios S1 and S2 exhibit increased optimal energy storage deployment compared to the reference case. The additional storage capacity enhances system flexibility, enabling lower renewable energy costs to support a more aggressive thermal substitution strategy—that is, accommodating greater renewable generation with less thermal capacity. Consequently, lower renewable costs tend to favor lower modes over a wider range of penetration levels.
Overall, the sensitivity analysis confirms that the main findings of this study are robust to the reasonable variations in the renewable energy investment cost assumptions. The U-shaped cost evolution trajectory remains qualitatively unchanged; The optimal substitution modes are stable at the extremes and exhibit only localized, explainable variations in the intermediate penetration range.
These results reinforce the validity of the proposed cost accounting framework and the identified optimal thermal power substitution strategies.

5. Conclusions

With the increasing proportion of renewable energy grid-connected, the source–load operation mode in the traditional power system is difficult to sustain, and the flexibility demand increases sharply. Based on the actual development and future trend of China’s new power system, this paper analyzes the changes of system flexibility and the factors affecting system cost and proposes a cost evolution model considering the development of the new power system in the future. Through the analysis of examples, the differences and problems of system cost evolution under different thermal power installed capacity substitution ratios are compared, and the optimal thermal power installed capacity substitution ratio under different penetration rates is obtained. The following conclusions are obtained:
  • From the perspective of the daily penetration rate, in the process of increasing wind power and photovoltaic penetration rate, the installed capacity of thermal power is being gradually reduced, and the flexibility of the system is becoming sharply reduced. At the same time, there is a problem of insufficient flexibility in up-regulation and down-regulation, which needs to be solved by configuring energy storage.
  • The main factors affecting the system cost are the cost of reducing the output of compressed thermal power after the integration of wind power and photovoltaic power and the cost of increasing the allocation of flexible resources when the system flexibility is in short supply during the change of the renewable energy penetration rate. At the same time, the replacement ratio of the installed capacity of different thermal power units also has a great impact on the system cost.
  • The example analysis shows that with the increase of the penetration rate, the system cost shows a trend of first decreasing and then increasing. When the installed capacity of the thermal power is balanced with the flexible resource allocation, the system cost is the lowest. The substitution method of thermal power installed capacity is also changing to replace more renewable energy with less thermal power, indicating that the system still needs a certain thermal power to ensure the stability of the system at a high penetration rate.
  • Finally, while renewable energy penetration continues to increase, thermal power plants still play an indispensable role as the main backbone of the system, providing essential flexibility and reliability services that cannot yet be fully replaced by renewable generation or energy storage.
The Garver-6 system used in this study is suitable for methodological validation but is too small to capture the geographic diversity of wind and solar power, realistic congestion models, or the variety of flexibility products in large-scale power systems. Future research will focus on the following two directions:
  • The proposed model will be tested on larger, more realistic test systems (e.g., IEEE 118-bus system or a provincial-level power system in China) with multi-region modeling to capture the spatial and temporal variability of wind and solar resources.
  • The current deterministic framework will be extended to incorporate stochastic or robust optimization techniques to account for the variability and uncertainty of renewable energy generation and load demand, which is critical for real-world applications.
  • We note that incorporating shiftable loads, price-responsive demand, and electric vehicle charging flexibility would enable a more comprehensive assessment of the system cost evolution under high renewable penetration.

Author Contributions

Conceptualization, X.Y. and Y.W.; Methodology, X.Y. and Y.W.; Software, Y.W.; Validation, X.Y. and Y.W.; Formal analysis, X.Y. and Y.W.; Investigation, Y.W., G.Y. and C.L.; Resources, X.Y., Y.W., G.Y. and C.L.; Data curation, Y.W., H.D. and C.L.; Writing—original draft, X.Y. and Y.W.; Writing—review & editing, X.Y., Y.W. and H.D.; Visualization, G.Y.; Supervision, X.Y., Y.W. and H.D.; Project administration, X.Y.; Funding acquisition, X.Y. and G.Y. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the State Grid Corporation of China Headquarters Science and Technology Project (Grant No. 4000-202399368A-2-2-ZB).

Data Availability Statement

Due to privacy and ethical restrictions, the data supporting the findings of this study are not publicly available. They may be requested from the corresponding author upon reasonable justification and with the permission of all the involved participants.

Acknowledgments

We thank the support from the Science and Technology Project of the State Grid Corporation of China.

Conflicts of Interest

Authors H.G. and C.L. were employed by State Grid Jilin Electric Power Co., Ltd. during the conduction of this study. The research received funding from State Grid Corporation of China Headquarters Science and Technology Project. All authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as potential conflicts of interest. The funder was not involved in the study design, collection, analysis, interpretation of data, the writing of this article, or the decision to submit it for publication.

Appendix A

In the DC power flow model adopted in this paper, the following simplifying assumptions are made.
Line resistance is neglected (rij ≈ 0), and the branch impedance is approximated as purely reactive: zijjxij.
Nodal voltage magnitudes are approximated as 1.0 p.u.
Under these assumptions, the imaginary part of the nodal admittance matrix becomes the susceptance matrix B, whose elements are calculated as follows.
Diagonal elements:
B i i = j i 1 x i j
Off-diagonal elements:
B i j = 1 x i j   ( i j )
If there is no direct transmission line between node i and node j, then Bij = 0.
The transmission expansion in this study follows the rules enumerated below.
  • Candidate corridors: New transmission lines may only be constructed in the nine corridors listed in Table A1 and Table A2.
  • Maximum new lines per corridor: Each corridor can accommodate at most seven new lines, as specified in Table A2.
  • Co-optimization: Transmission expansion decisions are optimized simultaneously with generation capacity investments and energy storage configuration to minimize the total system cost, as defined in the objective function (Equation (1)).
Table A1. Transmission line parameters of the Garver-6 system.
Table A1. Transmission line parameters of the Garver-6 system.
Line No.From Node iTo Node jReactance xij (p.u.)
1120.40
2140.60
3150.20
4230.20
5240.40
6350.20
7260.31
8360.48
9460.30
For the initial network topology of the Garver-6 system, the 6 × 6 susceptance matrix B (in p.u.) is as follows:
B = 9.17 2.5 0 1.67 5 0 2.5   13.23 5 2.5 0 3.23 0 5 12.08 0 5 2.08 1.67 2.5 0 7.5 0 3.33 5 0 5 0 10 0 0 3.23 2.08 3.33 0 8.64
Table A2. Maximum allowable number of new transmission lines for each corridor in the Garver-6 system.
Table A2. Maximum allowable number of new transmission lines for each corridor in the Garver-6 system.
Line No.From Node iTo Node jExisting Lines x i j 0 Max New Lines N i , j max Total Max Lines
112178
214178
315178
423178
524178
635178
726178
836178
946178
These rules ensure that transmission expansion is modeled realistically while maintaining computational tractability within the MILP framework.
Table A3. Table of notation.
Table A3. Table of notation.
SymbolDescriptionUnit
Cplantotal cost108 yuan
C plan inv annualized investment cost108 yuan
C plan oper system operation cost108 yuan
C plan punish penalty cost108 yuan
c gen inv , c wind inv , c sun inv , c pess inv , c ess inv the unit investment cost coefficients of thermal power, wind, photovoltaic, energy storage power and energy storage capacityyuan/kW
Pgen, Pwind, Psun, Pe, Eethe installed capacity of each technology104 kW
ηdiscount rate%
Nsplanning horizonyear
αg, βgthe fuel and environmental cost coefficients of thermal unitsyuan/kW
Rg, Rw, Rs, Rethe operation and maintenance cost coefficientsyuan/kW
δd, δw, δpvthe penalty coefficients for power shortage, wind curtailment, and photovoltaic curtailmentyuan/kW
D n , t cut the power shortage at time tyuan/kW
P w , t cut , P p v , t cut the curtailed wind and photovoltaic power at time tyuan/kW
Pg,tthe output of the thermal power unit at time t104 kW
Pw,t, Ppv,tthe wind and photovoltaic power outputs at time t104 kW
P e , t dis , P e , t c h a the discharging and charging power of energy storage at time t104 kW
Dn,tthe system load at time t104 kW
Tthe set of time periodshour
P g min , P g max the minimum and maximum output limits of thermal power unit104 kW
μthe ramping rate coefficient of thermal power unit%
ηethe charging/discharging efficiency of the energy storage%
SOCt, SOCt−1the state of charge of the energy storage at time t and time t − 1%
SOCmin, SOCmaxthe minimum and maximum state of charge limits of the energy storage%
SOCinithe initial state of charge of the energy storage%
Bthe node admittance matrix (susceptance matrix)-
θtthe vector of nodal voltage phase angles at time tangle
x i j new the number of new transmission lines constructed in corridor-
N i , j max the maximum allowable number of new lines in that corridor-
Ωlinethe set of candidate transmission corridors-
Pij,tthe actual power flow on corridor at time t104 kW
P i j max the maximum capacity of a single transmission line in that corridor104 kW
x i j 0 the number of existing lines-
x i j new the number of newly constructed lines-

References

  1. Ding, X.; Shi, S.; Yu, J.; Chen, Z.; Shang, Y.; Zeng, X.; Zhang, Y.; Dong, X. Exploration of New Power System Protection Architecture. In Proceedings of the 2024 IEEE 8th Conference on Energy Internet and Energy System Integration (EI2), Shenyang, China, 29 November–2 December 2024; pp. 3553–3559. [Google Scholar] [CrossRef] [Scilit]
  2. Zhang, Z.; Kang, C. Challenges and prospects for building a new power system under the goal of carbon neutrality. Chin. J. Electr. Eng. 2022, 42, 2806–2819. [Google Scholar] [CrossRef]
  3. Zhou, D. China has the world‘s leading renewable energy installed capacity. Sino-Foreign Energy 2026, 31, 65. [Google Scholar]
  4. Lu, Z.; Li, H.; Qiao, Y. Flexibility Evaluation and Supply/Demand Balance Principle of Power System with High-Penetration Renewable Electricity. Proc. CSEE 2017, 37, 9–20. [Google Scholar]
  5. Chai, G.; Yang, X.; Xu, T.; Xu, M.; Chai, R. Flexibility Planning Method for Electric Power System Based on Bi-Level Scene Reduction. J. Northeast. Electr. Power Univ. 2020, 40, 11–20. [Google Scholar]
  6. Denisov, V. Integrated Power System Multi-Node Model, Taking into Account the Nondispatchable of Renewable Energy Sources. In Proceedings of the 2022 IEEE 8th International Conference on Energy Smart Systems (ESS), Kyiv, Ukraine, 12–14 October 2022; pp. 175–179. [Google Scholar] [CrossRef] [Scilit]
  7. Zhang, X.; Conejo, A.J. Robust Transmission Expansion Planning Representing Long- and Short-Term Uncertainty. IEEE Trans. Power Syst. 2018, 33, 1329–1338. [Google Scholar] [CrossRef] [Scilit]
  8. Sun, T.; Ding, W.; Zhou, N.; Yang, X. Analysis of Renewable Energy Electricity Prices Based on System Costs. In Proceedings of the 2024 5th International Conference on Smart Grid and Energy Engineering (SGEE), Nanchang, China, 22–24 November 2024; pp. 447–450. [Google Scholar] [CrossRef] [Scilit]
  9. Yin, B.; Liu, T.; Zhang, Y.; Hu, J.; Ma, W.; Zhang, L.; Han, J. Coordinated Planning Method for Energy Storage and Thermal Power Flexibility Retrofit Considering Ancillary Service Revenue. Power Syst. Technol. 2023, 47, 1350–1362. [Google Scholar] [CrossRef]
  10. Sun, Z.; Tian, H.; Wang, W.; Pan, M.Y.; Zhang, L. Economic Study of Cascade-Utilized Battery Energy Storage System Participating in User-Side Peak Shaving and Valley Filling. Acta Energiae Solaris Sin. 2021, 42, 95–100. [Google Scholar]
  11. Yang, X.; Guo, Q.; Liu, X.; Zhou, Z.; Yan, G.; Zhang, H. Source-Storage-Grid Joint Planning Method Considering Coupling Relationship of Wind Curtailment Events. Autom. Electr. Power Syst. 2023, 47, 53–60. [Google Scholar]
  12. Yang, X.; Fan, Z.; Yan, G.; Yang, C. Joint Planning Method of Energy Storage and Transmission Considering Identification of Weak Links in Regulation Capability. Trans. China Electrotech. Soc. 2026; Advance Online Publication. [CrossRef]
  13. Yang, X.; Zang, Y.; Zhang, Y.; Xiong, X.; Fu, Y.; Bian, X. Hierarchical optimal scheduling method for power system considering line-source-storage flexibility. Electr. Power Autom. Equip. 2024, 44, 185–192+209. [Google Scholar] [CrossRef]
  14. Sainju, D.; Sinha, R.; Pokhrel, B.R. Static Expansion Planning of Transmission Line Using Mixed Integer Linear Programming Method. In Proceedings of the 2016 IEEE 6th International Conference on Power Systems (ICPS), New Delhi, India, 4–6 March 2016; pp. 1–6. [Google Scholar] [CrossRef] [Scilit]
  15. Yang, X.Y.; Liu, P.Y.; Sun, Y.; Li, H.Y.; Yan, G.G. Dynamic Planning Method of Flexible Resources Considering the Evolution Law of Flexibility Demand. Electr. Power Constr. 2023, 44, 3–12. [Google Scholar]
  16. Yang, D.; Ni, J.; Yang, Y.; Jiao, Y.; Qi, Y.; Xu, X.; Liu, J. Review of Transmission Line Planning Methods and Life Cycle Cost. Sichuan Electr. Power Technol. 2024, 47, 65–71. [Google Scholar] [CrossRef]
  17. Tan, J.; Liu, E.; Li, H.; Zhang, Y.; Yang, X.; Shi, J.; Xie, Z.; Yin, C. Exploration on the Practice of Improvement Measures for the Power Supply Reliability in Distribution Network in New Type Power System. In Proceedings of the 2024 7th International Conference on Renewable Energy and Power Engineering (REPE), Beijing, China, 25–27 September 2024; pp. 215–219. [Google Scholar] [CrossRef] [Scilit]
  18. Lu, Z.; Huang, H.; Shan, B.; Wang, Y. Morphological evolution and power forecasting prospects of high-proportion renewable energy power system structure. Autom. Electr. Power Syst. 2017, 41, 12–18. [Google Scholar]
Figure 1. Comparison of the traditional power system and new power system.
Figure 1. Comparison of the traditional power system and new power system.
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Figure 2. System flexibility under different daily penetration rates.
Figure 2. System flexibility under different daily penetration rates.
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Figure 3. Comparison of source-side and load-side line expansion before and after.
Figure 3. Comparison of source-side and load-side line expansion before and after.
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Figure 4. Model frame diagram.
Figure 4. Model frame diagram.
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Figure 5. Resolving flow chart.
Figure 5. Resolving flow chart.
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Figure 6. Cost evolution trend under a 1:1 replacement scenario.
Figure 6. Cost evolution trend under a 1:1 replacement scenario.
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Figure 7. Changes in system cost composition in two ways.
Figure 7. Changes in system cost composition in two ways.
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Figure 8. Cost evolution diagram under the optimal alternative mode.
Figure 8. Cost evolution diagram under the optimal alternative mode.
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Figure 9. Sensitivity analysis: Impact of wind and PV cost reduction on system cost evolution.
Figure 9. Sensitivity analysis: Impact of wind and PV cost reduction on system cost evolution.
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Table 1. Thermal power installed capacity under different penetration rates (Unit: 10,000 kW).
Table 1. Thermal power installed capacity under different penetration rates (Unit: 10,000 kW).
RE Penetration Rate0%10%20%30%40%50%60%70%80%90%100%
Mode 121112111211121112111211121112111211121112111
Mode 221112090206920482027200619851964194219211900
Mode 321112069202719851942190018581816177417311689
Mode 421112048198519211858179517311668160515411478
Mode 521112027194218581774168916051520143613511267
Mode 621112006190017951689158414781372126711611056
Mode 7211119851858173116051478135112251098971845
Mode 821111964181616681520137212251077929781633
Mode 92111194217741605143612671098929760591422
Mode 10211119211731154113511161971781591401211
Table 2. Design conditions.
Table 2. Design conditions.
ParameterNumerical ValueParameterNumerical Value
Thermal power construction cost 50,000 yuan/kWThermal power operation and maintenance cost3000 yuan/kW
Wind power construction cost54,000 yuan/kWFuel cost2.8 yuan/kW
Photovoltaic construction cost33,000 yuan/kWThermal power environmental protection cost3000 yuan/kW
Energy storage power cost1000 yuan/kWWind power operation and maintenance cost1500 yuan/kW
Energy storage capacity cost6000 yuan/kWhPhotovoltaic operation and maintenance cost2000 yuan/kW
Curtailment penalty830 yuan/kWhEnergy storage operation and maintenance cost coefficient1.05
Power shortage penalty100 yuan/kWhTransmission line construction cost1000 yuan/kW/km
Table 3. Mode 1. Energy storage configuration.
Table 3. Mode 1. Energy storage configuration.
RE Penetration RateEnergy Storage Power/10,000 kWEnergy Storage Capacity/10,000 kWhEnergy Storage Cost/100 Million Yuan
0%000
10%000
20%000
30%174.8342.51.9
40%482.61670.48.9
50%766.92685.614.2
60%1009.04081.521.5
70%1211.45022.626.4
80%1445.35944.531.3
90%1627.06792.835.7
100%1644.67361.938.6
Table 4. Mode 1. Line expansion.
Table 4. Mode 1. Line expansion.
RE Penetration RateLine 1–2Line 1–4Line 1–5Line 2–3Line 2–4Line 3–5Line 2–6Line 3–6Line 4–6
0%111100000
10%111100000
20%111101101
30%111101101
40%111101212
50%111101312
60%111101312
70%111101313
80%111111314
90%111111314
100%111111325
Table 5. Mode 3. Energy storage configuration.
Table 5. Mode 3. Energy storage configuration.
RE Penetration RateEnergy Storage Power/10,000 kWEnergy Storage Capacity/10,000 kWhEnergy Storage Cost/100 Million Yuan
0%000
10%000
20%000
30%189.92561.5
40%390.71235.46.6
50%761.22840.215
60%1034.55692.829.7
70%1286.38078.441.9
80%1534.59814.150.9
90%162312,086.262.5
100%1795.813,356.369
Table 6. Mode 3. Line expansion.
Table 6. Mode 3. Line expansion.
RE Penetration RateLine 1–2Line 1–4Line 1–5Line 2–3Line 2–4Line 3–5Line 2–6Line 3–6Line 4–6
0%111100000
10%111100000
20%111100101
30%111101212
40%111101212
50%111101312
60%011111312
70%011111313
80%011201314
90%011202314
100%010202315
Table 7. Optimal thermal power installed capacity substitution ratio and total cost under different penetration rates.
Table 7. Optimal thermal power installed capacity substitution ratio and total cost under different penetration rates.
RE Penetration RateReplacement ModeThermal Power Installed Capacity/10,000 kWTotal Cost/100 Million Yuan
0%/2111374.9
10%1:11900359.7
20%1:11689345.6
30%1:11478334.9
40%1:11267335.0
50%0.9:11161351.9
60%0.7:11225380.9
70%0.7:11077419.7
80%0.6:11098464.3
90%0.5:11161518.5
100%0.5:11056573.6
Table 8. Energy storage configuration of the optimal alternative method.
Table 8. Energy storage configuration of the optimal alternative method.
RE Penetration RateEnergy Storage Power/10,000 kWEnergy Storage Capacity/10,000 kWhEnergy Storage Cost/100 Million Yuan
0%000
10%000
20%16.822.10.1
30%250596.13.2
40%513.22248.511.8
50%832.24364.822.8
60%957.93658.219.3
70%1271.96111.632
80%14585803.630.6
90%14516718.935.2
100%16767603.939.9
Table 9. Impact of wind and PV cost reduction on optimal thermal power substitution mode.
Table 9. Impact of wind and PV cost reduction on optimal thermal power substitution mode.
RE Penetration RateReference (Original Cost)Scenario S1 (Cost −10%)Scenario S2 (Cost −20%)
0%///
10%1:11:11:1
20%1:11:11:1
30%1:11:11:1
40%1:11:11:1
50%0.9:11:11:1
60%0.7:10.7:10.8:1
70%0.7:10.7:10.7:1
80%0.6:10.6:10.6:1
90%0.5:10.5:10.5:1
100%0.5:10.5:10.5:1
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Yang, X.; Wang, Y.; Yan, G.; Dong, H.; Li, C. Analysis of Power System Cost Evolution Characteristics Under Different Thermal Power Substitution Modes. Energies 2026, 19, 2174. https://doi.org/10.3390/en19092174

AMA Style

Yang X, Wang Y, Yan G, Dong H, Li C. Analysis of Power System Cost Evolution Characteristics Under Different Thermal Power Substitution Modes. Energies. 2026; 19(9):2174. https://doi.org/10.3390/en19092174

Chicago/Turabian Style

Yang, Xiuyu, Yi Wang, Gangui Yan, Hongda Dong, and Chenggang Li. 2026. "Analysis of Power System Cost Evolution Characteristics Under Different Thermal Power Substitution Modes" Energies 19, no. 9: 2174. https://doi.org/10.3390/en19092174

APA Style

Yang, X., Wang, Y., Yan, G., Dong, H., & Li, C. (2026). Analysis of Power System Cost Evolution Characteristics Under Different Thermal Power Substitution Modes. Energies, 19(9), 2174. https://doi.org/10.3390/en19092174

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