CN108763670A - A kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method - Google Patents

A kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method Download PDF

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CN108763670A
CN108763670A CN201810463358.6A CN201810463358A CN108763670A CN 108763670 A CN108763670 A CN 108763670A CN 201810463358 A CN201810463358 A CN 201810463358A CN 108763670 A CN108763670 A CN 108763670A
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吴攀
单建强
高春天
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Xian Jiaotong University
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Abstract

The invention discloses a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process methods, initialize supercritical carbon dioxide reactor parameter first;Then the quality, interior energy of control volume and the flow taken in current iteration step are calculated and obtains the transient state core power of reactor;Then it using the state of circulating coolant as the boundary condition of reactor fuel rod Calculation of Heat Transfer, calculates Temperature Distribution in fuel rod and updates pressure, flow, the enthalpy parameter taken over;It calculates the change of internal energy rate of each fluid node and is judged, finally judge whether that reaching final calculates the time, to form the transient process of supercritical carbon dioxide Brayton cycle.This invention simplifies the solution flows of supercritical carbon dioxide reactor Brayton cycle transient process, in turn ensure computational accuracy.

Description

A kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method
Technical field
It is analyzed the invention belongs to nuclear reactor safety and calculates technical field, and in particular to a kind of solution supercritical carbon dioxide Reactor Brayton cycle transient process method.
Background technology
Supercritical carbon dioxide reactor has many advantages, such as that the thermal efficiency is high, system simplification is compact, is made using Brayton cycle For energy conversion system, whole system is made of the part such as reactor, regenerator, cooler, compressor, turbine, is to have very much The forth generation nuclear reactor concept of foreground.Supercritical carbon dioxide reactor uses direct cooling cycle, eliminates steam generation The equipment such as device, large-scale heat exchanger, simple system.Mechanical equipment in circulation loop is smaller, the startup of capital equipment and The motor-driven response time substantially reduces, and is conducive to flexibly the operating status of adjustment reactor cycle in time.Based on above-mentioned advantage, surpass Critical carbon dioxide reactor concept can be not only used for the high efficiency commercial reactor of exploitation different capacity level, can also become core Submarine, core aircraft carrier etc. require that equipment volume is small, the powered equipment of changed power timely military equipment, have wide city Field application prospect.
In the Brayton cycle of supercritical carbon dioxide reactor, the supercritical carbon dioxide at suction port of compressor, which is in, to be faced Near boundary's point.Supercritical carbon dioxide is acutely and rapid in the variation of Near The Critical Point physical property, leads to the cooling in Brayton cycle Agent physical property will undergo strong nonlinear change, and the characteristic of this coolant physical property acute variation had both improved overcritical titanium dioxide The cycle efficieny of carbon reactor Brayton cycle, also the Transient Numerical Simulation entirely to recycle bring challenge.Physical property it is violent Variation can cause to solve can encounter numerical computations and be difficult to restrain in supercritical carbon dioxide reactor Brayton cycle transient process The problem of, increase the difficulty of transient analysis software development.
However through investigation, rarely have open achievement and patent introduction anti-for solving supercritical carbon dioxide both at home and abroad at present Answer the numerical method of heap Brayton cycle transient process.
Invention content
In view of the above-mentioned deficiencies in the prior art, the technical problem to be solved by the present invention is that providing, a kind of solution is super to face Boundary's carbon dioxide reaction heap Brayton cycle transient process method carries out quasi-static place to the turbine machinery in Brayton cycle Reason, simplifies solution procedure, improves solving speed.
The present invention uses following technical scheme:
A kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method, initializes overcritical two first Carbon dioxide reaction heap parameter;Then the transient state core power of reactor is calculated;Then using the state of circulating coolant as The boundary condition of reactor fuel rod Calculation of Heat Transfer calculates Temperature Distribution in fuel rod;Update the pressure taken over, flow, enthalpy Parameter;It calculates the change of internal energy rate △ U/U of each fluid node and is compared with specified value, finally judge whether to reach final meter Evaluation time repeats the reactor that above step obtains supercritical carbon dioxide reactor Brayton cycle in each time step The flow regime of power rating, fuel rod state of temperature, turbine Mechanical Running Condition and cyclic internal cooling but agent is super to be formed The transient process of critical carbon dioxide Brayton cycle
Specifically, steps are as follows:
S1, initialize the core power of supercritical carbon dioxide reactor, Brayton cycle coolant channel fluid state, Calculate time step parameter;
The quality of supercritical carbon dioxide and energy conservation equation and the momentum taken over are kept in S2, discrete Brayton cycle Permanent equation;Quality, interior energy and the flow taken over of control volume in current iteration step is calculated;
S3, by the enthalpy and specific volume of each node in recycling, according to instantaneous in CO 2 fluid physical property packet calculate node Pressure;
S4, by calculate Point reactor nutron kinetics equation, the transient state core power of reactor is calculated;
Boundary condition of the state as reactor fuel rod Calculation of Heat Transfer of S5, circulating coolant, are changed by heat conduction, convection current Heat calculates Temperature Distribution each in fuel rod;
The parameters such as pressure, flow, the enthalpy that S6, update are taken over;
S7, the change of internal energy rate △ U/U for calculating each fluid node, if the △ U/U maximum values of each node are more than specified value, Then think that current iteration step calculates not restrain, time step halves, and returns to step S3 and recalculates;If the △ U/ of each fluid node U maximum values are less than specified value, then it is assumed that the calculating convergence of current iteration step, into next step;
S8, judge whether to reach the final calculating time, if reached, terminate calculating;If do not reached, redirect To step S2, the calculating of next time step is carried out.
Further, step S2 is specially:The quality and the conservation of energy of supercritical carbon dioxide in discrete Brayton cycle Equation and the momentum conservation equation taken over, using Gauss-Saden that iteration to being recycled about the solution of Jacobin matrix J Mass incremental, energy increment and the flow increment Δ Y respectively taken over of each node of fluid, to which next iteration step be calculated Node quality, energy and the flow taken over, the calculating of mass incremental, energy increment and flow increment Δ Y is as follows:
Δ Y=J-1·B
Wherein, Δ t is time step, and nv is number of nodes, and nj is take over quantity, YnFor the argument value at current time, n Indicate current time.
Further, the energy conservation equation of CO 2 fluid and mass-conservation equation are applied on control volume, meter The variation of the quality, interior energy and pressure of control volume is calculated, momentum conservation equation is applied to take over, and calculating flows in and out control The coolant flow of body, the conservation of mass of all control volumes, the difference equation of the conservation of energy and the conservation of momentum taken over is poor Equations simultaneousness is divided to obtain following formula together:
Above formula is substituted into after the right first item is carried out first order Taylor series expansion and the time-derivative in left side is carried out discrete Obtain the mass incremental and energy increment and take over flow increment Δ Y of node.
Further, the quality of CO 2 fluid, momentum and energy conservation equation are respectively:
Wherein, ρ is density;W is fluid flow;V is fluid flow rate;P is pressure;DhFor equivalent diameter;F is frictional resistance Coefficient;gzFor acceleration of gravity;U is fluid interior energy;H is fluid enthalpy;Q is fluid endogenous pyrogen, and j is the section for flowing into present node Point quantity, z is height of node.
Further, it when fluid flows through gas-turbine tool, uses and the node pressure that turbine machinery is brought is calculated with drag Variation and energy variation:
Δ P=P1 T(Rp-1)
Wherein, Δ P is turbine machinery pressure change, P1 TFor turbine mechanical inputs stagnation pressure, RpFor turbine machinery pressure ratio, by property Energy curve is inquired to obtain, Wc.v.For turbine mechanical convection body amount of work,For turbine mechanical flow, ηadFor the thermal insulation of turbine machinery Efficiency is inquired to obtain by performance curve,Enthalpy is exported for turbine machinery,Enthalpy is exported for turbine machinery;
Turbine machinery is the node pressure variation and energy variation that fluid is brought, and will be respectively acting on fluid fundamental equation Momentum conservation equation and energy conservation equation.
Further, in step S2, the pipeline in Brayton cycle is indicated with node, spatially fluid recirculation system Discrete using staggered-mesh, momentum grid cell deviates quality and energy grid unit half space increment.
Further, in step S4, the reactor Point reactor nutron kinetics equation of six groups of delayed neutrons is as follows:
Wherein:N (t) is reactor core fission power;T is the time;ρ (t) is global reactivity;β is total delayed neutron fraction;Λ It is prompt neutron for the time;λiFor the decay coefficient of i-th group of delayed neutron;Ci(t) it is the fission power of i-th group of delayed neutron.
Further, in step S5, the Temperature Distribution in fuel rod is as follows:
Wherein:ρ is density;cpFor specific heat;T is temperature;T is the time;K is thermal coefficient;Q is endogenous pyrogen power density.
Further, the efficiency and pressure ratio for solving turbine machinery come interpolation using the performance curve of turbine machinery, in transient state When analyzing program solution, turbine machinery is one and takes over a node that the pressure liter being calculated by pressure ratio or pressure drop will act on In the work(that the rotation axis on the equation of momentum of turbine machinery entrance sleeve, being calculated does turbine machinery internal flow, with source The form of item increases the energy conservation equation in turbine mechanical fluid node.
Compared with prior art, the present invention at least has the advantages that:
A kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method of the present invention, with fluid homogeneous flow Based on model and reactor point pile neutron equation, in conjunction with the physical property of supercritical carbon dioxide, friction and heat transfer characteristic, face super Boundary CO 2 fluid fundamental equation carries out time and spatially discrete, uses transformation period step-length or for Jacobian matrix Increase the modes such as multiplication factor to promote convergence of this method near carbon dioxide critical point, efficiently solves Bretton and follow The numerical divergence problem and turbine machinery transient process Solve problems that ring transient state can encounter when solving.
Further, state of the supercritical carbon dioxide in Brayton cycle is essentially single-phase, using homogeneous phase model The fundamental equation of fluid is calculated, the number of fundamental equation can be effectively reduced, is reduced required alternate when fundamental equation calculates Constitutive relationship not only simplifies calculating step, and ensures that this method can accurately obtain the state change of supercritical carbon dioxide Change.
Further, it uses and shortens the time step calculated or increase the modes such as multiplication factor for Jacobian matrix, it can Effectively to solve the problems, such as that the numerical solution that physical property mutation is brought when supercritical carbon dioxide intends Near The Critical Point is not restrained.
Further, fuel Doppler effect, cooling succinctly can effectively be solved using Point reactor nutron kinetics equation The reactor capability feedback that agent temperature effect and control rod action are brought.
Further, one-dimension conduct equation can accurately calculate the distribution of temperature radially in fuel rod, be followed for Bretton Ring transient analysis provides the fuel pellet and wall surface temperature result of variations that researcher is concerned about.
Further, the turbine machinery performance curve being input from the outside provides the pressure ratio and efficiency of turbine machinery, can be fast The transient operating condition of fast accurate simulation gas-turbine tool, meanwhile, this method can unify the substantially square of fluid in turbine machinery Journey form and the fluid fundamental equation form in common pipe are the key that realize that Closed Brayton Power Cycle transient process calculates.
Further, accurate supercritical carbon dioxide physical property, heat exchange and friction law formula, ensure that this method just True property.
In conclusion the present invention is based on simplified fluid fundamental equation, Point reactor nutron kinetics equation, rational gas-turbines Tool model, accurate supercritical carbon dioxide physical property and heat exchange friction law formula and effective method of value solving, not only simplify The solution flow of supercritical carbon dioxide reactor Brayton cycle transient process in turn ensures computational accuracy, ensures to be based on being somebody's turn to do The transient process of method solves the transient physical process that can accurately react supercritical carbon dioxide reactor Brayton cycle.
Below by drawings and examples, technical scheme of the present invention will be described in further detail.
Description of the drawings
Fig. 1 is flow chart of the present invention;
Fig. 2 is the discrete figure of Brayton cycle coolant channel of the present invention;
Fig. 3 is turbine machinery model schematic.
Specific implementation mode
The present invention provides a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process methods, first just The core power of beginningization supercritical carbon dioxide reactor, calculates time step at Brayton cycle coolant channel fluid state Parameter;Then quality, interior energy and the flow taken over of control volume in current iteration step is calculated;Pass through the wink in node When pressure;Obtain the transient state core power of reactor;Then using the state of circulating coolant as reactor fuel rod in terms of heat transfer The boundary condition of calculation calculates Temperature Distribution in fuel rod;Update pressure, flow, the enthalpy parameter taken over;Calculate each fluid node Change of internal energy rate △ U/U, if the change of internal energy rate maximum value of each node be more than specified value, then it is assumed that current iteration step calculate It does not restrain, time step halves, and recalculates the instantaneous pressure in node;If the maximum value of the change of internal energy rate of each fluid node Less than specified value, then it is assumed that the calculating convergence of current iteration step finally judges whether to reach the final calculating time.More than being based on Method for solving can obtain the reactor capability shape of supercritical carbon dioxide reactor Brayton cycle in each time step The flow regime of state, fuel rod state of temperature, turbine Mechanical Running Condition and cyclic internal cooling but agent, to form overcritical two The transient process of carbonoxide Brayton cycle.
The present invention can accurately and effectively solve the transient process that supercritical carbon dioxide reactor Bretton follows, and can be used for The crash analysis of supercritical carbon dioxide reactor Brayton cycle and control strategy research.
Referring to Fig. 1, a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method of the present invention, packet Include following steps:
S1, initialize the core power of supercritical carbon dioxide reactor, Brayton cycle coolant channel fluid state, Calculate the parameters such as time step;
The quality of supercritical carbon dioxide and energy conservation equation and the momentum taken over are kept in S2, discrete Brayton cycle Permanent equation;Quality, interior energy and the flow taken over of control volume in current iteration step is calculated;
Quality, momentum and the energy conservation equation of CO 2 fluid be respectively:
Wherein:ρ is density, kg/m3;A is area, m2;W is fluid flow, kg/s;V is fluid flow rate, m/s;P is pressure Power, MPa;DhFor equivalent diameter, m;F is coefficient of frictional resistance;gzFor acceleration of gravity, m/s2;U is fluid interior energy, kJ/kg;h For fluid enthalpy, kJ/kg;Q is fluid endogenous pyrogen, kW/kg;J is the number of nodes for flowing into present node, and z is height of node;
When fluid flows through gas-turbine tool (gas-turbine and compressor), it will use and calculate what steamer machinery was brought with drag Node pressure changes and energy variation:
Δ P=P1 T(Rp-1)
Wherein, Δ P is turbine machinery pressure change, P1 TFor turbine mechanical inputs stagnation pressure, RpFor turbine machinery pressure ratio, by property Energy curve is inquired to obtain, Wc.v.For turbine mechanical convection body amount of work,For turbine mechanical flow, ηadFor the thermal insulation of turbine machinery Efficiency is inquired to obtain by performance curve,Enthalpy is exported for turbine machinery,Enthalpy is exported for turbine machinery.
Turbine machinery is the node pressure variation and energy variation that fluid is brought, and will be respectively acting on fluid fundamental equation Momentum conservation equation and energy conservation equation.
In numerical computations, the pipeline in Brayton cycle is all indicated with node.Spatially fluid recirculation system Discrete using staggered-mesh, momentum grid cell deviates quality and energy grid unit half space increment.Fig. 2 gives two Intersection mesh generation between adjacent node K and node L.It is take over j between node K and node L.Energy conservation equation and matter It measures conservation equation to be applied on node, the variation of the quality, interior energy and pressure of calculate node, momentum conservation equation is applied to connect Guan Shang calculates the coolant flow for flowing in and out control volume, Wj-1, Wj and Wj+1 as shown.
By the conservation of mass of all nodes, the difference equation of the conservation of energy and the conservation of momentum difference equation simultaneous taken over Together, following form can be obtained:
First order Taylor series expansion is carried out to first item on the right of formula (4), can be obtained:
f(Yn+1)=f (Yn)+J(Yn)·(Yn+1-Yn) (5)
Formula (5) substitutes into formula (4) and can obtain:
It is discrete to the time-derivative progress on the left of formula (6), it can obtain:
Formula (7), which is substituted into formula (6), can finally obtain:
J Δs Y=B (8)
Wherein,
Δ Y=[Δ W1... Δ Wj... Δ Wnj,ΔM1... Δ MK... Δ Mnv,ΔU1... Δ UK... Δ Unv]T
Wherein, Δ t is time step, and nv is number of nodes, and nj is take over quantity, YnFor the argument value at current time, n Indicate current time.
Using Gauss-Saden your iteration can solution formula (8), obtain the mass incremental of each node of circulation of fluid, energy increases Amount and the flow increment respectively taken over, to be calculated next iteration step node quality, energy and the flow taken over.
S3, by the enthalpy and specific volume of each node in recycling, according to instantaneous in CO 2 fluid physical property packet calculate node Pressure;
S4, by calculate Point reactor nutron kinetics equation, the transient state core power of reactor is calculated;
Consider that the reactor Point reactor nutron kinetics equation of six groups of delayed neutrons is:
In formula:N (t) is reactor core fission power, W;T is time, s;ρ (t) is global reactivity, $;β is total delayed neutron Share;Λ is prompt neutron for time, s;λiFor the decay coefficient of i-th group of delayed neutron, s-1;Ci(t) it is i-th group of delayed neutron Fission power, W.
Boundary condition of the state as reactor fuel rod Calculation of Heat Transfer of S5, circulating coolant, are changed by heat conduction, convection current Heat calculates Temperature Distribution each in fuel rod;
In formula:ρ is density;cpFor specific heat;T is temperature;T is the time;K is thermal coefficient;Q is endogenous pyrogen power density.
The parameters such as pressure, flow, the enthalpy that S6, update are taken over;
S7, the change of internal energy rate △ U/U for calculating each fluid node, if the maximum value of the change of internal energy rate of each node is more than Specified value, then it is assumed that current iteration step, which calculates, not to be restrained, and time step halves, and returns to step S3 and recalculates;If each fluid section The maximum value of the change of internal energy rate of point is less than specified value, then it is assumed that the calculating convergence of current iteration step, into next step;
S8, judge whether to reach the final calculating time, if reached, terminate calculating;If do not reached, redirect To step S2, the calculating of next time step is carried out.
In order to make the object, technical scheme and advantages of the embodiment of the invention clearer, below in conjunction with the embodiment of the present invention In attached drawing, technical scheme in the embodiment of the invention is clearly and completely described, it is clear that described embodiment is A part of the embodiment of the present invention, instead of all the embodiments.The present invention being described and shown in usually here in attached drawing is real Applying the component of example can be arranged and be designed by a variety of different configurations.Therefore, the present invention to providing in the accompanying drawings below The detailed description of embodiment be not intended to limit the range of claimed invention, but be merely representative of the selected of the present invention Embodiment.Based on the embodiments of the present invention, those of ordinary skill in the art are obtained without creative efforts The every other embodiment obtained, shall fall within the protection scope of the present invention.
Supercritical carbon dioxide heat exchange, which calculates, uses disclosed Gnielinski relational expressions, disclosed in the use of friction law formula Zigrang-Sylvester relational expressions.
Referring to Fig. 3, for the solution of the turbine mechanical (compressor and gas-turbine) in Brayton cycle, it is believed that transient state mistake The change of fluid of turbine machine internal is in quasi-static state in journey.Under the assumptions, using the performance curve of turbine machinery come Interpolation solves the efficiency and pressure ratio of turbine mechanical (compressor and gas-turbine).In transient analysis program solution, by turbine machinery One is regarded as to take over and a node.The pressure liter (or pressure drop) being calculated by pressure ratio will act on turbine machinery entrance sleeve The equation of momentum on, and the work(that the rotation axis being calculated does turbine machinery internal flow, it will increased in the form of source item In the energy conservation equation of turbine mechanical fluid node.
The above content is merely illustrative of the invention's technical idea, and protection scope of the present invention cannot be limited with this, every to press According to technological thought proposed by the present invention, any change done on the basis of technical solution each falls within claims of the present invention Protection domain within.

Claims (10)

1. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method, which is characterized in that initial first Change supercritical carbon dioxide reactor parameter;Then the transient state core power of reactor is calculated;Then with circulating coolant Boundary condition of the state as reactor fuel rod Calculation of Heat Transfer, calculate Temperature Distribution in fuel rod;Update take over pressure, Flow, enthalpy parameter;It calculates the change of internal energy rate △ U/U of each fluid node and is compared with specified value, finally judged whether Reach final and calculate the time, repetition above step obtains supercritical carbon dioxide reactor Bretton in each time step and follows The flow regime of reactor capability state, fuel rod state of temperature, turbine Mechanical Running Condition and the cyclic internal cooling of ring but agent, To form the transient process of supercritical carbon dioxide Brayton cycle.
2. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method according to claim 1, It is characterized in that, being as follows:
S1, it the core power for initializing supercritical carbon dioxide reactor, Brayton cycle coolant channel fluid state, calculates Time step parameter;
The quality of supercritical carbon dioxide and energy conservation equation and the conservation of momentum side taken in S2, discrete Brayton cycle Journey;Quality, interior energy and the flow taken over of control volume in current iteration step is calculated;
S3, by the enthalpy and specific volume of each node in recycling, according to the instantaneous pressure in CO 2 fluid physical property packet calculate node;
S4, by calculate Point reactor nutron kinetics equation, the transient state core power of reactor is calculated;
Boundary condition of the state as reactor fuel rod Calculation of Heat Transfer of S5, circulating coolant, pass through heat conduction, heat convection meter Calculate Temperature Distribution each in fuel rod;
The parameters such as pressure, flow, the enthalpy that S6, update are taken over;
S7, the change of internal energy rate △ U/U for calculating each fluid node recognize if the △ U/U maximum values of each node are more than specified value It calculates and does not restrain for current iteration step, time step halves, and returns to step S3 and recalculates;If the △ U/U of each fluid node are most Big value is less than specified value, then it is assumed that the calculating convergence of current iteration step, into next step;
S8, judge whether to reach the final calculating time, if reached, terminate calculating;If do not reached, step is jumped to Rapid S2 carries out the calculating of next time step.
3. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method according to claim 2, It is characterized in that, step S2 is specially:In discrete Brayton cycle the quality of supercritical carbon dioxide and energy conservation equation with And the momentum conservation equation taken over, using Gauss-Saden, your iteration is each to obtaining circulation of fluid about the solution of Jacobin matrix J Mass incremental, energy increment and the flow increment Δ Y respectively taken over of node, to which the node of next iteration step be calculated Quality, energy and the flow taken over, the calculating of mass incremental, energy increment and flow increment Δ Y is as follows:
Δ Y=J-1·B
Wherein, Δ t is time step, and nv is number of nodes, and nj is take over quantity, YnFor the argument value at current time, n is indicated Current time.
4. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method according to claim 3, It is characterized in that, the energy conservation equation of CO 2 fluid and mass-conservation equation are applied on control volume, control is calculated The variation of the quality, interior energy and pressure of body, momentum conservation equation are applied to take over, and calculating flows in and out the cold of control volume But agent flux, by the conservation of mass of all control volumes, the difference equation of the conservation of energy and the conservation of momentum difference equation taken over Simultaneous obtains following formula together:
Above formula is substituted into after the right first item is carried out first order Taylor series expansion and discrete obtain is carried out to the time-derivative in left side The mass incremental and energy increment and take over flow increment Δ Y of node.
5. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method according to claim 4, It is characterized in that, the quality of CO 2 fluid, momentum and energy conservation equation are respectively:
Wherein, ρ is density;W is fluid flow;V is fluid flow rate;P is pressure;DhFor equivalent diameter;F is coefficient of frictional resistance; gzFor acceleration of gravity;U is fluid interior energy;H is fluid enthalpy;Q is fluid endogenous pyrogen, and j is the number of nodes for flowing into present node Amount, z is height of node.
6. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method according to claim 5, It is characterized in that, when fluid flows through gas-turbine tool, use with drag calculate node pressure variation that turbine machinery is brought and Energy variation:
Δ P=P1 T(Rp-1)
Wherein, Δ P is turbine machinery pressure change, P1 TFor turbine mechanical inputs stagnation pressure, RpIt is bent by performance for turbine machinery pressure ratio Line is inquired to obtain, Wc.v.For turbine mechanical convection body amount of work,For turbine mechanical flow, ηadFor the adiabatic effect of turbine machinery Rate is inquired to obtain by performance curve,Enthalpy is exported for turbine machinery,Enthalpy is exported for turbine machinery;
Turbine machinery is the node pressure variation and energy variation that fluid is brought, and will be respectively acting on the momentum of fluid fundamental equation Conservation equation and energy conservation equation.
7. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process side according to claim 2 or 5 Method, which is characterized in that in step S2, the pipeline in Brayton cycle is indicated with node, and spatially fluid recirculation system is adopted Discrete with staggered-mesh, momentum grid cell deviates quality and energy grid unit half space increment.
8. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method according to claim 2, It is characterized in that, in step S4, the reactor Point reactor nutron kinetics equation of six groups of delayed neutrons is as follows:
Wherein:N (t) is reactor core fission power;T is the time;ρ (t) is global reactivity;β is total delayed neutron fraction;Λ is wink Send out neutron generation time;λiFor the decay coefficient of i-th group of delayed neutron;Ci(t) it is the fission power of i-th group of delayed neutron.
9. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process method according to claim 2, It is characterized in that, in step S5, the Temperature Distribution in fuel rod is as follows:
Wherein:ρ is density;cpFor specific heat;T is temperature;T is the time;K is thermal coefficient;Q is endogenous pyrogen power density.
10. a kind of solution supercritical carbon dioxide reactor Brayton cycle transient process side according to claim 1 or 2 Method, which is characterized in that the efficiency and pressure ratio for solving turbine machinery come interpolation using the performance curve of turbine machinery, in transient analysis When program solution, turbine machinery is taken over for one and will act on gas with a node, the pressure liter being calculated by pressure ratio or pressure drop On the equation of momentum of wheel mechanical entrance sleeve, the work(that the rotation axis that is calculated does turbine machinery internal flow, with source item Form increases the energy conservation equation in turbine mechanical fluid node.
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CN111680405A (en) * 2020-05-25 2020-09-18 西安理工大学 Natural circulation capacity hydraulic characteristic calculation method
CN111723451A (en) * 2019-03-04 2020-09-29 国家电投集团科学技术研究院有限公司 Sub-channel solving method of Newton-Rafferson algorithm
CN112071457A (en) * 2020-08-07 2020-12-11 西安交通大学 Load tracking method for supercritical carbon dioxide direct cooling reactor system
CN112733469A (en) * 2020-12-30 2021-04-30 西安交通大学 Supercritical fluid applicability evaluation method of Brayton cycle system of special reactor
CN113255268A (en) * 2021-05-21 2021-08-13 北京华大九天科技股份有限公司 Method for detecting and repairing transient analysis non-convergence in circuit simulation
CN115374724A (en) * 2022-08-29 2022-11-22 中国核动力研究设计院 Fluid critical heat flux density analysis method in natural circulation system under motion condition
CN117521560A (en) * 2024-01-03 2024-02-06 中国核动力研究设计院 Modeling method and device for supercritical carbon dioxide turbine model and computing equipment

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1775732B1 (en) * 2005-08-31 2013-07-31 Westinghouse Electric Sweden AB A method of estimating dryout properties in a nuclear light water reactor
CN103902784A (en) * 2014-04-11 2014-07-02 华北电力大学 Safety analysis calculating device for transient nuclear heat coupling of supercritical water reactor
CN105653869A (en) * 2016-01-05 2016-06-08 中国核动力研究设计院 Three-dimensional transient performance analysis method for supercritical water reactor core
CN106202866A (en) * 2016-06-24 2016-12-07 西安交通大学 One stablizes accurate reactor physics thermal technology's coupling calculation

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1775732B1 (en) * 2005-08-31 2013-07-31 Westinghouse Electric Sweden AB A method of estimating dryout properties in a nuclear light water reactor
CN103902784A (en) * 2014-04-11 2014-07-02 华北电力大学 Safety analysis calculating device for transient nuclear heat coupling of supercritical water reactor
CN105653869A (en) * 2016-01-05 2016-06-08 中国核动力研究设计院 Three-dimensional transient performance analysis method for supercritical water reactor core
CN106202866A (en) * 2016-06-24 2016-12-07 西安交通大学 One stablizes accurate reactor physics thermal technology's coupling calculation

Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109783904A (en) * 2018-12-28 2019-05-21 西安交通大学 A kind of width parameter area carbon dioxide physical property method for solving
CN111723451A (en) * 2019-03-04 2020-09-29 国家电投集团科学技术研究院有限公司 Sub-channel solving method of Newton-Rafferson algorithm
CN111680405A (en) * 2020-05-25 2020-09-18 西安理工大学 Natural circulation capacity hydraulic characteristic calculation method
CN112071457B (en) * 2020-08-07 2023-04-07 西安交通大学 Load tracking method for supercritical carbon dioxide direct cooling reactor system
CN112071457A (en) * 2020-08-07 2020-12-11 西安交通大学 Load tracking method for supercritical carbon dioxide direct cooling reactor system
CN112733469A (en) * 2020-12-30 2021-04-30 西安交通大学 Supercritical fluid applicability evaluation method of Brayton cycle system of special reactor
CN112733469B (en) * 2020-12-30 2022-09-30 西安交通大学 Supercritical fluid applicability evaluation method for Brayton cycle system of special reactor
CN113255268A (en) * 2021-05-21 2021-08-13 北京华大九天科技股份有限公司 Method for detecting and repairing transient analysis non-convergence in circuit simulation
CN113255268B (en) * 2021-05-21 2022-05-24 北京华大九天科技股份有限公司 Method for detecting and repairing transient analysis non-convergence in circuit simulation
CN115374724A (en) * 2022-08-29 2022-11-22 中国核动力研究设计院 Fluid critical heat flux density analysis method in natural circulation system under motion condition
CN115374724B (en) * 2022-08-29 2023-08-22 中国核动力研究设计院 Fluid critical heat flow density analysis method in natural circulation system under motion condition
CN117521560A (en) * 2024-01-03 2024-02-06 中国核动力研究设计院 Modeling method and device for supercritical carbon dioxide turbine model and computing equipment
CN117521560B (en) * 2024-01-03 2024-03-26 中国核动力研究设计院 Modeling method and device for supercritical carbon dioxide turbine model and computing equipment

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