Start-up method for heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system
By adopting the rotating drum control system, compressor inlet temperature and pressure control, rotation shaft speed and circulation loop flow control methods in the heat pipe stack coupled supercritical CO2 Breton cycle nuclear power system, the shortcomings in the cold start characteristics of the new nuclear power system are solved, and the safety and stability of the system are achieved.
Patent Information
- Application Number
- CN202310354525.4
- Authority / Receiving Office
- CN · China
- Patent Type
- Patents(China)
- Current Assignee / Owner
- Filing Date
- 2023-04-04
- Publication Date
- 2025-05-20
- Estimated Expiration
- 2043-04-04
AI Technical Summary
The existing heat pipe cooling reactor start-up scheme is mainly aimed at static thermoelectric converters, and it is difficult to effectively analyze and control the cold start characteristics of the new heat pipe reactor coupled supercritical CO2 Breton cycle nuclear power system. Especially under the consideration of safety and stability factors such as core lift power limit and rotating drum accuracy limit, the design is complex and difficult.
A method for starting a heat pipe stack coupled supercritical CO2 Breton cycle nuclear power system is adopted. The core heat pipe start is adjusted through the rotating drum control system to meet the core start restrictions, and the core power and temperature are achieved independently control; the compressor inlet temperature and pressure control is controlled by the compressor inlet temperature and pressure; the compressor inlet temperature and pressure are adjusted; the compressor speed step-up and circulating loop flow control are achieved through the rotation shaft speed control and the circulating loop flow control.
Effective control of the key parameters of the cold start of the heat pipe stack coupled supercritical CO2 Breton circulation system is achieved, reducing the disturbance of the key parameters in the transient process, and ensuring the safety and stability of the system.
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Figure CN116291790B_ABST
Abstract
Description
Technical Field
[0001] The present invention belongs to the technical field of nuclear reactor thermal - hydraulic experiments, and particularly relates to a startup scheme for a nuclear power system of a heat pipe reactor coupled with a supercritical CO 2 Brayton cycle. Background Technique
[0002] An unmanned underwater vehicle (UUV) has autonomy, flexibility, and versatility, and is an effective tool for underwater exploration, resource development, and utilization. A heat pipe cooled reactor (HPR) is considered to be one of the most promising choices for UUV power sources due to its good inherent safety, controllability, and concealment. Due to different application scenarios of heat pipe cooled reactors, their structures are also different. Most heat pipe cooled reactors use static thermoelectric conversion devices, but with the increasing power demand, dynamic thermoelectric conversion devices are becoming more and more popular. Using a heat pipe type reactor coupled with a supercritical CO 2 Brayton cycle system has the advantages of high efficiency, high power density, high reliability, etc., and is very suitable for a structurally compact unmanned underwater vehicle.
[0003] This new type of nuclear power system has good application prospects. Therefore, the research on the cold - start characteristics of this new type of nuclear power system is of great significance. Due to the large thermal delay linearity, strong thermal expansion resistance, and drastic changes in loop switching flow rate during the startup process of this new type of nuclear power device, and at the same time, the startup process also needs to meet certain limiting conditions, these increase the complexity and difficulty of the startup scheme design of a heat pipe reactor coupled with a supercritical CO2 Brayton cycle nuclear power system.
[0004] At present, most of the existing startup schemes for heat pipe cooled reactors are for static thermoelectric converters, which are relatively simple and do not have the ability to analyze the cold - start of this new type of coupled system. Therefore, it is of great significance to explore a reasonable startup scheme for a heat pipe reactor coupled with a supercritical CO 2 Brayton cycle nuclear power system with good safety and stability. Summary of the Invention
[0005] The technical problem to be solved by the present invention is to provide a startup control method for a nuclear power system of a heat pipe reactor coupled with a supercritical CO 2 Brayton cycle in view of the insufficient research on the startup characteristics of the new type of nuclear power device, and at the same time considering safety and stability factors such as the power - up limit of the reactor core and the accuracy limit of the rotating drum.
[0006] The present invention is achieved by adopting the following technical solutions:
[0007] A method for 2Starting method for a Brayton cycle nuclear power system, said heat pipe reactor coupled with supercritical CO 2 The cycle process of the Brayton cycle nuclear power system is as follows: the core transfers heat to the CO flowing through the condensation section of the heat pipe through the heat pipe 2 gas, and the CO 2 gas absorbs heat in the condensation section and then enters the turbine to expand and do work, driving the rotating shaft to rotate, and then driving the compressor to rotate to provide driving force for the entire heat pipe reactor coupled supercritical CO 2 Brayton cycle nuclear power system's cycle loop, driving the generator to output power outward. After the exhausted steam after the turbine does work outputs part of the thermal energy again in the recuperator, it enters the pre-cooler to exchange heat with the cooling water, enters the compressor for pressurization after the gas reaches the target temperature at the compressor inlet, and then enters the recuperator to absorb the thermal energy released by the exhausted steam to complete the cycle process; heat pipe reactor coupled supercritical CO 2 The cold start of the Brayton cycle nuclear power system includes the start of the core heat pipe, the start of the compressor, and the switching of the cycle loop; when the system is started for the first time, the active start method is adopted, and the neutron source is placed at the lower end of the control rod absorber in the core center; the rotation drum control system is used to adjust the start of the core heat pipe to meet the core start limit conditions and achieve the autonomous control of the core power and temperature; the compressor inlet temperature is adjusted during the start-up process by controlling the compressor inlet temperature; the compressor inlet pressure is adjusted during the start-up process by controlling the compressor inlet pressure; the compressor speed is stepped up by controlling the rotating shaft speed; the system cycle loop flow rate is controlled by the compressor inlet throttle valve to adjust the system cycle loop flow rate during the start-up process; the system cycle loop switching control is achieved by controlling the opening degrees of the turbine bypass valve and the turbine inlet throttle valve, so that the working medium is gradually switched from the bypass branch to the turbine branch during the start-up process.
[0008] The rotation drum control system adjusts the start of the core heat pipe to meet the core start limit conditions, and changes the core power rise rate by adjusting the rotation angle of the control drum and the observation time.
[0009] Control the single rotation angle of the rotation drum. After each control of the rotation of the rotation drum, if the maximum rise rate is less than 0.5% FP (full power) within the observation time, the next rotation is carried out, otherwise enter the next observation time.
[0010] When the compressor inlet temperature changes, the difference between the actual compressor inlet temperature and the set compressor inlet temperature is used as the input signal and input into the PI controller. According to the signal output by the PI controller, the opening degree of the cooling water inlet valve is changed, and then the cooling water mass flow rate is changed to maintain the stability of the compressor inlet temperature.
[0011] The opening degree O(t) of the cooling water inlet valve is:
[0012] O(t) = O(0) + u(t)
[0013] Where O(0) is the initial opening of the cooling water inlet valve, and u(t) is the compressor inlet temperature control output signal.
[0014] The compressor inlet pressure control is achieved by connecting an air extraction and replenishment box at the compressor inlet to timely extract air during the system circulation loop heating process to prevent the system circulation loop from overpressure.
[0015] In the early stage of the system circulation loop startup, the generator drives the compressor to work and maintain the speed step-by-step increase. By controlling the power of the motor coaxially connected to the compressor, the torque on the rotating shaft is changed, so that the compressor runs at the set speed.
[0016] The system circulation loop flow control is regulated by the compressor inlet throttle valve control. During the startup process, the control signal is triggered when the flow exceeds the set value. The calibrated flow of the system circulation loop under rated speed operation is used as the reference value. The difference between the real-time flow and the reference value is the input signal. The PI controller is used to adjust the compressor inlet throttle valve opening to stabilize the flow.
[0017] The opening of the turbine bypass valve and the opening of the turbine inlet throttle valve change over time.
[0018] A method for coupling supercritical CO with a heat pipe stack 2 Start-up method of Brayton cycle nuclear power system, the heat pipe stack coupled with supercritical CO 2 The Brayton cycle nuclear power system is composed of: the core 1 and the heat pipe 2 are connected with the regenerator 3, the compressor 6, the precooler 4, the regenerator 3 and the gas turbine 8 in sequence to form a circulation loop; the low-pressure side outlet of the regenerator 3 is connected to the precooler inlet 4, the outlet pipeline of the precooler 4 is connected to the compressor inlet throttle valve 10, the compressor inlet throttle valve 10 is connected to the compressor inlet, the compressor 6, the generator 7 and the gas turbine 8 are on the same rotating shaft 14; the outlet of the compressor 6 is connected to the high-pressure side inlet of the regenerator 3, the high-pressure side of the regenerator 3 preheats the fluid and then enters the heat pipe heat exchanger 2, the outlet of the heat pipe heat exchanger 2 is divided into two paths, one path is connected to the gas turbine inlet throttle valve 11 and then connected to the gas turbine 8 inlet, and the other path is connected to the low-pressure side inlet of the regenerator 3 through the gas turbine bypass valve 12.
[0019] Compared with the prior art, the present invention has at least the following beneficial effects:
[0020] The present invention provides a startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system, which realizes the ability to control the key parameters of the cold startup of the heat pipe reactor coupled supercritical CO2 Brayton system and reduces the disturbance of key parameters in the transient process coupling system.
[0021] The rotating drum control system can effectively control the rising rate of the core startup power and ensure the influence on the single - rotation accuracy of the rotating drum. The compressor inlet temperature control can effectively control the stability of the compressor inlet temperature and avoid large - scale density changes caused by temperature changes. Connect a gas extraction and makeup tank at the compressor inlet to extract gas in a timely manner during the startup and heating process to prevent loop overpressure. The motor drives the compressor to do work and maintain a stepped increase in speed, which is beneficial to maintaining the stability of the circulation loop flow, overcoming the influence caused by the thermal expansion of the working fluid, and ensuring the warm - up of the turbine. The loop flow control can achieve the protection of the compressor equipment and eliminate the risk of blockage caused by an increase in the compressor flow due to a small loop resistance during the speed increase at startup. The opening degrees of the turbine bypass valve and the turbine inlet throttle valve change in stages over time, which is beneficial to reducing the flow fluctuations caused by the change in the loop resistance when the opening degrees change and maintaining the stability of the key system parameters. 2 due to large - scale density changes caused by temperature changes. Connect a gas extraction and makeup tank at the compressor inlet to extract gas in a timely manner during the startup and heating process to prevent loop overpressure. The motor drives the compressor to do work and maintain a stepped increase in speed, which is beneficial to maintaining the stability of the circulation loop flow, overcoming the influence caused by the thermal expansion of the working fluid, and ensuring the warm - up of the turbine. The loop flow control can achieve the protection of the compressor equipment and eliminate the risk of blockage caused by an increase in the compressor flow due to a small loop resistance during the speed increase at startup. The opening degrees of the turbine bypass valve and the turbine inlet throttle valve change in stages over time, which is beneficial to reducing the flow fluctuations caused by the change in the loop resistance when the opening degrees change and maintaining the stability of the key system parameters.
[0022] In summary, the present invention can effectively control the changes in the key parameters of the cold - state startup of the heat - pipe - coupled supercritical CO2 Brayton system and has reasonable safety and stability. Brief Description of the Drawings
[0023] Figure 1 is a control schematic diagram of the heat - pipe reactor - coupled supercritical CO2 Brayton system;
[0024] Figure 2 is a flowchart of the startup scheme;
[0025] Figure 3 is a control logic diagram of the control drum;
[0026] Figure 4 is a control logic diagram of the compressor inlet temperature;
[0027] Figure 5 is a control logic diagram of the loop flow;
[0028] Figure 6 is a cold - state startup core power curve;
[0029] Figure 7 is a schematic diagram of the cold - state startup response of the coupled system. Among them, a is the change in the inlet mass flow rate of each key component of the loop and the change in speed during startup, b is the change in the opening degrees of the turbine bypass valve and the throttle valve over time, and c is the change in the temperature of each key component of the loop.
[0030] Among them: 1. Core; 2. Heat pipe; 3. Regenerator; 4. Pre - cooler; 5. Liquid storage tank; 6. Compressor; 7. Generator; 8. Turbine; 9. Seawater throttle valve; 10. Compressor inlet throttle valve; 11. Turbine inlet throttle valve; 12. Turbine bypass valve; 13. Turbine outlet check valve; 14. Rotating shaft. Detailed Embodiment
[0031] To make the objectives, technical solutions and features of the embodiments of the present invention clearer, the exemplary embodiments of the present disclosure will be described in more detail below with reference to the accompanying drawings. Based on the design parameters of a deep-sea unmanned submersible using a heat pipe reactor as a power device, the technical solutions in the embodiments of the present invention will be clearly and completely described. These embodiments are provided to enable a more thorough understanding of the present disclosure and to fully convey the scope of the present disclosure to those skilled in the art.
[0032] The present invention provides a method for starting a Brayton cycle nuclear power system coupled with a heat pipe reactor and supercritical CO 2 2.
[0033] As Figure 1 shown, the structure of the Brayton cycle nuclear power system coupled with a heat pipe reactor and supercritical CO 2 2 is as follows: The reactor core 1 and the heat pipe 2 are successively connected to the recuperator 3, the compressor 6, the precooler 4, the recuperator 3 and the steam turbine 8 to form a circulation loop; the low-pressure side outlet of the recuperator 3 is connected to the inlet of the precooler 4, the outlet pipeline of the precooler 4 is connected to the throttle valve 10 at the inlet of the compressor, and the throttle valve 10 at the inlet of the compressor is connected to the inlet of the compressor after that. The compressor 6, the generator 7 and the steam turbine 8 are on the same rotating shaft 14; the outlet of the compressor 6 is connected to the high-pressure side inlet of the recuperator 3, and the high-pressure side of the recuperator 3 preheats the fluid and then enters the heat pipe heat exchanger 2. The outlet of the heat pipe heat exchanger 2 is divided into two paths. One path is connected to the throttle valve 11 at the inlet of the steam turbine and then to the inlet of the steam turbine 8, and the other path is connected to the low-pressure side inlet of the recuperator 3 through the bypass valve 12 of the steam turbine.
[0034] As Figure 2 shown in the startup flowchart of the method of the present invention, it mainly includes the startup of the reactor core heat pipe, the startup of the compressor and the switching of the circulation loop. The specific operation steps are as follows:
[0035] In the first step, when the system starts in the cold state, the control drum is first used to control the introduction of positive reactivity, and then the startup of the reactor core heat pipe is realized. The startup of the reactor core heat pipe is mainly divided into three stages: As Figure 6 shown at a in, the first stage is from subcritical to critical state. In order to reach the critical state quickly, the control drum is selected to rotate at a speed of 1° / s; as Figure 6 shown at b in, the second stage is to increase the power until the heat pipe is fully started. This process is controlled by the control drum (as Figure 3 shown). The specific implementation scheme is to rotate the control drum angle by 0.1° each time. The condition for rotating the control drum each time is that within the observation time of 35 s, the temperature change does not exceed 5K, and the maximum power increase speed is lower than 0.5% FP (full power); as Figure 6 shown at c in, the third stage is the introduction of the Brayton cycle. In this stage, the compressor starts and the loop flow rate increases. Since CO 2The condensation section of the cooling heat pipe, the heat of the core heat pipe is discharged, and the temperature negative feedback weakens, and the core power rises more rapidly.
[0036] In the second step, the compressor is started, and the flow rate of the circulation loop is increased to the rated state. As Figure 7 shown in a, the rotational speed of the rotating shaft rises stepwise with time, ensuring that a relatively low speed is controlled for a long time to warm up the steam turbine. At the same time, since the condensation section of the heat pipe already has a certain temperature when the compressor starts, a large thermal expansion will occur under the condition of increasing flow velocity, bringing flow disturbance. It is necessary to increase the rotational speed as quickly as possible to increase the compressor head to overcome the resistance. And then, a suitable rotational speed step needs to be maintained to overcome the resistance caused by the thermal expansion of the working fluid. After that, the rotational speed is increased stepwise to make the flow rate fluctuation of the circulation loop relatively stable. When the compressor starts, the compressor inlet temperature control and pressure control are introduced to reduce the fluctuation of the circulation loop during the start-up process. During the process of increasing the rotational speed, the circulation loop flow control needs to be introduced in advance to avoid excessive flow caused by the increase in rotational speed and increase the stability of the system.
[0037] As Figure 4 and Figure 5 shown, the most mature proportional-integral (PI) controller in industrial experience is used to meet the control requirements of the compressor inlet temperature and the circulation loop flow rate. The formula is:
[0038]
[0039] where u(t) is the output signal of the PI controller; e(t) is the input signal of the PI controller; Kp is the gain parameter of the proportional link of the controller;
[0040] For the above-mentioned compressor inlet temperature and loop flow rate control, the specific implementation plan is to set up monitoring at the compressor inlet, and use the deviation between the monitored parameters (compressor inlet temperature and loop flow rate) and the target value as the input signal of the PI controller. The formula is:
[0041]
[0042] where Φ is the monitored parameter; Φ set is the set target value.
[0043] According to the output signal of the above PI controller, the change in the opening of the cooling water inlet valve can be calculated. The formula is:
[0044] O(t) = O(0) + u(t)
[0045] In the third step, the circulation loop is switched to connect the steam turbine to the circulation loop to do work, realizing the complete start-up of the circulation loop. The opening degrees of the steam turbine inlet throttle valve and the steam turbine bypass valve start to act after a switching signal is triggered when the steam turbine inlet temperature exceeds the set value, and the valve opening degrees change with time. The specific opening degree change is shown inFigure 7 As shown in b, before the valve action, the opening of the turbine inlet throttle valve is maintained at 0.1 to ensure turbine warm-up. During the valve action, the change in flow rate causes a change in the heat transfer amount of the regenerator, and the inlet temperature of the condensation section decreases. As Figure 7 shown in b for the valve opening change and Figure 7 shown in c for the system temperature change in the figure, adopting a stepped opening change is beneficial to reducing the temperature fluctuation during this transient process.
[0046] During the cold start process, considering the stability of the system operation, the details are as follows:
[0047] For the heat pipe reactor coupled supercritical CO2 Brayton cycle system, due to the limitation of the high-temperature heat pipe start-up limit, the core heat pipe needs to be started first. After the heat pipe is fully started, the speed-up process is carried out. Therefore, it will inevitably cause a large flow disturbance due to the thermal expansion of the fluid after flowing through the condensation section of the heat pipe. Adopting the control of the rotational speed of the rotating shaft to quickly increase the speed can minimize the influence of this process. During the subsequent speed-up process, it is necessary to introduce the loop flow control in advance to avoid excessive flow caused by the increase in speed and increase the stability of the system. During the switching process of the circulation loop, the closing and opening of the turbine bypass valve and the turbine inlet throttle valve will cause a change in flow rate, which will in turn affect the heat transfer amount of the regenerator and cause the inlet temperature of the condensation section to decrease. Adopting a stepped valve change can effectively reduce the temperature change caused by the valve change and reach the rated state more quickly.
[0048] During the cold start process, considering the safety of the system operation, the details are as follows:
[0049] 1. Core power increase limit
[0050] During the transient process of the cold start of the coupled system, the change in core power should not exceed the transient operation safety limit value.
[0051] 2. Core thermal stress
[0052] During the transient process of the cold start of the system, the change amplitude and rate of the core cladding, fuel, and heat pipe temperatures do not exceed the thermal stress limit values that the materials can withstand.
[0053] In summary, for a start-up method of a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system according to the present invention, the cold start control of the heat pipe reactor coupled supercritical CO2 Brayton cycle system can be realized by adopting this method. The control system in the method can effectively control the disturbance amplitude of the key parameters of the system during the transient process and takes into account the safety and stability during the transient operation process.
[0054] Although the present invention has been described in detail with general descriptions and specific embodiments, modifications or improvements can be made thereto based on the present invention, which will be obvious to those skilled in the art. Therefore, these modifications or improvements made without departing from the spirit of the present invention all fall within the scope of the present invention claimed.
Claims
1. A startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system, characterized in that: The cycle process of the heat pipe stack coupled supercritical CO2 Brayton cycle nuclear power system is as follows: the core transfers heat to the CO2 gas flowing through the heat pipe condensation section through the heat pipe, and the CO2 gas enters the gas turbine to expand and do work after absorbing heat in the condensation section, driving the rotating shaft to rotate, and then driving the compressor to rotate to provide driving force for the circulation loop of the entire heat pipe stack coupled supercritical CO2 Brayton cycle nuclear power system, driving the generator to output power outward, and after the exhaust steam after the gas turbine does work outputs part of the heat energy again in the regenerator, it enters the precooler to exchange heat with the cooling water, and after the gas reaches the compressor inlet target temperature, it enters the compressor for pressurization, and then enters the regenerator to absorb the heat energy released by the exhaust steam, completing the cycle process; The cold start of the heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system includes core heat pipe start-up, compressor start-up and circulation loop switching; when the system is started for the first time, an active start-up method is adopted, and the neutron source is placed at the lower end of the control rod absorber in the center of the core; the core heat pipe start-up is adjusted by the rotating drum control system to meet the core start-up restriction conditions and realize autonomous control of the core power and temperature; the compressor inlet temperature is controlled by the compressor inlet temperature control during the startup process; the compressor inlet pressure is controlled by the compressor inlet pressure control during the startup process; the compressor speed is increased in a step-by-step manner by the rotating shaft speed control; the system circulation loop flow is controlled by the compressor inlet throttle valve to realize the system circulation loop flow regulation during the startup process; the system circulation loop switching control is controlled by the turbine bypass valve and the turbine inlet throttle valve opening control to realize the gradual switching of the working fluid from the bypass branch to the turbine branch during the startup process; When the compressor inlet temperature changes, the difference between the actual compressor inlet temperature and the set compressor inlet temperature is input into the PI controller as an input signal. The cooling water inlet valve opening is changed according to the signal output by the PI controller, thereby changing the cooling water mass flow rate to maintain the compressor inlet temperature stable. The opening O(t) of the cooling water inlet valve is: O(t)=O(0)+u(t) Where O(0) is the initial opening of the cooling water inlet valve, and u(t) is the compressor inlet temperature control output signal.
2. The startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system according to claim 1, characterized in that: The rotating drum control system adjusts the start-up of the core heat pipe to meet the core start-up restriction conditions, and changes the core power increase rate by adjusting the control drum rotation angle and observation time.
3. The startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system according to claim 2, characterized in that: Control the rotation angle of the drum in a single rotation. After each rotation of the drum, the next rotation will be performed if the maximum rising rate is less than 0.5% FP within the observation time, otherwise it will enter the next observation time.
4. The startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system according to claim 1, characterized in that: The compressor inlet pressure control is achieved by connecting an air extraction and replenishment box at the compressor inlet to extract air in time during the system circulation loop heating process to prevent the system circulation loop from overpressure.
5. The startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system according to claim 1, characterized in that: In the early stage of starting the system circulation loop, the generator drives the compressor to work and maintain a step-by-step increase in speed. By controlling the power of the electric motor coaxially connected to the compressor, the torque on the rotating shaft is changed, so that the compressor runs at the set speed.
6. The startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system according to claim 1, characterized in that: The system circulation loop flow control is controlled and adjusted through the compressor inlet throttle valve control. During the startup process, the control signal is triggered when the flow exceeds the set value. The calibrated flow of the system circulation loop under rated speed operation is used as the reference value. The difference between the real-time flow and the reference value is the input signal. The PI controller is used to adjust the compressor inlet throttle valve opening to stabilize the flow.
7. The startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system according to claim 1, characterized in that: The opening of the turbine bypass valve and the opening of the turbine inlet throttle valve change with time.
8. The startup method for a heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system according to claim 1, characterized in that: The heat pipe reactor coupled supercritical CO2 Brayton cycle nuclear power system is constructed as follows: the core (1) and the heat pipe (2) are connected to the regenerator (3), the compressor (6), the precooler (4), the regenerator (3) and the gas turbine (8) in sequence to form a circulation loop; the low-pressure side outlet of the regenerator (3) is connected to the inlet of the precooler (4), the outlet pipeline of the precooler (4) is connected to the compressor inlet throttle valve (10), the compressor inlet throttle valve (10) is connected to the compressor inlet, the compressor (6), the generator (7) and the gas turbine (8) are on the same rotating shaft (14); the compressor (6) outlet is connected to the high-pressure side inlet of the regenerator (3), the high-pressure side of the regenerator (3) preheats the fluid and then enters the heat pipe heat exchanger, the heat pipe heat exchanger outlet is divided into two paths, one path is connected to the gas turbine inlet throttle valve (11) and then connected to the gas turbine (8) inlet, and the other path is connected to the low-pressure side inlet of the regenerator (3) through the gas turbine bypass valve (12).
Citation Information
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