CN110060788A - A kind of general thermion nuclear reactor for space power supply thermal transient Analysis of Electrical Characteristics method - Google Patents

A kind of general thermion nuclear reactor for space power supply thermal transient Analysis of Electrical Characteristics method Download PDF

Info

Publication number
CN110060788A
CN110060788A CN201910283124.8A CN201910283124A CN110060788A CN 110060788 A CN110060788 A CN 110060788A CN 201910283124 A CN201910283124 A CN 201910283124A CN 110060788 A CN110060788 A CN 110060788A
Authority
CN
China
Prior art keywords
formula
fuel
reactor
emitter
reactivity
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201910283124.8A
Other languages
Chinese (zh)
Other versions
CN110060788B (en
Inventor
王成龙
代智文
陆恺霖
秋穗正
田文喜
苏光辉
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Xian Jiaotong University
Original Assignee
Xian Jiaotong University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Xian Jiaotong University filed Critical Xian Jiaotong University
Priority to CN201910283124.8A priority Critical patent/CN110060788B/en
Publication of CN110060788A publication Critical patent/CN110060788A/en
Application granted granted Critical
Publication of CN110060788B publication Critical patent/CN110060788B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G21NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21CNUCLEAR REACTORS
    • G21C17/00Monitoring; Testing ; Maintaining
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E30/00Energy generation of nuclear origin
    • Y02E30/30Nuclear fission reactors

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • General Engineering & Computer Science (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Monitoring And Testing Of Nuclear Reactors (AREA)

Abstract

A kind of general thermion nuclear reactor for space reactor core transient state pyroelecthc properties comprehensive analysis method, key step is as follows: 1, determining thermion nuclear reactor for space core structure and initial parameter 2, calculate current time thermion nuclear reactor for space core temperature distribution 3, the potential on calculating current time heap core electrode and current distribution 4, calculate current time reactor core output voltage, output electric current, electromotive power output 5, according to all known conditions, the calculating that step 2 carries out subsequent time is jumped to, cycle calculations are until reaching stable state;Method of the invention can calculate interchangeable heat ion space nuclear reactor power supply transient state pyroelecthc properties, and the available more accurate calculated result when calculating.

Description

A kind of general thermion nuclear reactor for space power supply thermal transient Analysis of Electrical Characteristics method
Technical field
The present invention relates to nuclear reactor for space field of power supplies, and in particular to a kind of general thermion nuclear reactor for space heap Core transient state pyroelecthc properties comprehensive analysis method
Background technique
With space exploration task demand be continuously increased and solar energy and chemical cell are in deep space mission or planet table The space power producer of limitation in the task of face, technology maturation and high reliablity is following the main direction of development.Heat Ion space nuclear reactor power supply is a kind of current research nuclear reactor for space power supply the most mature, and the U.S. and Russia are upper The nineties in century has carried out a large amount of research work.Up to the present, Russia is still carrying out high-power thermion nuclear reactor The research work of power supply.
Nuclear reactor for space is studied in the world at present, can all consider influence of the pyroelecthc properties to system substantially.It is international On carried out the related pyroelecthc properties research of a large amount of thermion spaces heap, these researchs are broadly divided into two classes, and one kind is using examination Proved recipe method measures the pyroelecthc properties of thermion nuclear reactor for space power supply, and one kind is anti-to thermion space core using theoretical model Heap power supply is answered to be analyzed, but most experimental and theoretical analysis is all based on single thermionic fuel element in heap and carries out , and focus on stable state pyroelecthc properties more.In order to determine the influence of reactor core transient state pyroelecthc properties, thermal-hydraulic is established to reactor core Model, heat and power system model, thus for more fully and effectively assess thermion nuclear reactor for space pyroelecthc properties provide according to According to.
Summary of the invention
In order to overcome the above-mentioned problems of the prior art, the purpose of the present invention is to provide a kind of general thermion is empty Between nuclear reactor transient state pyroelecthc properties comprehensive analysis method, general thermion nuclear reactor for space entirety reactor core is carried out Research, can accurately reflect the pyroelecthc properties of full heap, the thermion space nuclear reaction of different structure and power may be implemented Heap pyroelecthc properties calculate, and reduce the requirement to the structure and parameter of thermion nuclear reactor for space, effectively increase this method To the adaptability of different problems.
To achieve the goals above, this invention takes following technical schemes:
A kind of general thermion nuclear reactor for space reactor core transient state pyroelecthc properties comprehensive analysis method, this method include with Lower step:
Step 1: thermionic fuel element structure and parameter being determined according to user demand, determine each layer of thermionic fuel element Size, the temperature of the power distribution and coolant of fuel of structure, divide radial and axial node number according to demand;
Step 2: calculating current t moment thermion nuclear reactor for space core temperature distribution, the structure obtained using step 1 Establish the non-linear differential equation of heat balance group about the diabatic process of thermion nuclear reactor for space reactor core respectively with parameter;
General thermion nuclear reactor for space reactor core is made of thermionic fuel element and moderator matrix, thermion combustion Expect element mainly by fuel region, fission gas gap, emitter, caesium gas-bearing formation, receiving pole, helium layer, stainless steel inner sleeve, cold But agent and stainless steel outer sleeve pipe are constituted;
Reactor fission power is solved using the point reactor model dynamical equation of six groups of delayed neutrons is considered first;Point heap mould Type considers the influence of delayed neutron counterincision Variable power and the Reactivity feedback of fuel, coolant and structure member simultaneously, because This is the first order differential equation system of a coupling;Simultaneously as reactivity is time correlation variable, therefore equation group is non-linear 's;Point reactor model dynamical equation is calculated by formula (1) and formula (2);
In formula:
P (t) --- t moment reactor fission power/W;
T --- calculate time/s;
Λ --- neutron generation time/s;
β --- total effective delayed neutron fraction;
βi--- i-th group of delayed neutron fraction;
λi--- decay coefficient/s of i-th group of delayed neutron-1
Ci(t) --- the concentration/m of i-th group of delayed neutron of t moment-3
nc--- delayed neutron group number;
ρ (t) --- total reactivity/$;
The reactivity of reactor can because out-pile reactivity introduce or heap in Reactivity feedback due to change;Pass through corresponding machine Reason model or rule-of-thumb relation establish the reactive solving model of each section;The total reactivity of reactor is calculated by formula (3);
ρ (t)=ρD(t)+∑ρi(t) formula (3)
In formula:
ρ (t) --- total reactivity/$;
ρD(t) --- reactivity/$ that control rotary drum and shutdown rotary drum introduce;
ρi(t) --- each material Reactivity feedback/$;
The Reactivity feedback considered in reactor physics model includes: UO2The temperature of the Doppler effect of fuel, electrode Feedback, moderator temperature feedback and reflecting layer temperature feedback;It is most important for most of operating conditions of thermionic reactor Be the positive-effect of moderator and the negative effect of thermionic fuel element;
The Doppler of fuel, which feeds back to formula (4), to be calculated:
In formula:
--- the Doppler of fuel feeds back;
TU--- fuel temperature/K;
T0--- reference temperature/K;
Emitter and receiving pole Reactivity feedback are calculated by formula (5):
In formula:
--- emitter and receiving pole Reactivity feedback;
TE--- emitter temperature/K;
TC--- receiving pole temperature/K;
Moderator Reactivity feedback coefficient is calculated by formula (6):
--- moderator Reactivity feedback;
TM--- zircoium hydride moderator temperature/K;
Wherein parameter phi is determined by formula (7):
Reflecting layer Reactivity feedback coefficient is calculated by formula (8):
In formula:
--- reflecting layer Reactivity feedback;
TR--- reflecting layer temperature/K;
Rotary drum reactivity is controlled to introduce by formula (9) calculating:
In formula:
ρD--- control rotary drum reactivity introduces;
θ --- control rotary drum rotational angle/degree;
Decay power mainly includes that the radioactive decay of neutron absorption product and fission product is decayed by simplification Heat is solved and is calculated by formula (10) and formula (11):
In formula:
Pd(t) --- t moment reactor decay power/W;
Hi(t) --- the concentration/m of i-th group of fission product of t moment-3
--- the share of i-th group of fission product;
--- decay coefficient/s of i-th group of fission product-1
According to the reactor core general power that the solving model of fission power and decay power obtains, according to shared by each control volume of fuel Power fraction be added in fuel control volume as inner heat source, in reactor core thermal-hydraulic solving model, by formula (12) It calculates;
QV=P φ/V formula (12)
In formula:
QV--- volume inner heat source/Wm of fuel control volume-3
P --- reactor general power/W;
φ --- fuel control volume heat release rate accounts for the share of reactor general power;
Volume/m of V --- fuel control volume3
Middle submodel utilized above obtains inner heat source, and fuel region equation of heat balance is calculated by formula (13):
In formula:
ρU--- density/kgm of fuel pellet-3
cU--- specific heat/Jkg of fuel pellet-1·K-1
TU--- temperature/K of fuel pellet;
λU--- thermal coefficient/Wm of fuel pellet-1·K-1
Radius/m of r --- fuel pellet;
QV--- heat source density/Wm of fuel control volume-3
Emitter equation of heat balance is calculated by formula (14):
In formula:
ρE--- density/kgm of emitter-3
VE--- volume/kgm of emitter-3
cE--- specific heat/Jkg of emitter-1·K-1
λG--- thermal coefficient/Wm of fission gas-1·K-1
δG--- fission gas gap width/m;
εUE--- the emissivity of fuel and emitter surface;
εEC--- emitter and the emissivity for receiving pole surface;
λU--- thermal coefficient/Wm of fuel pellet-1·K-1
ПE--- unit length emitter exterior surface area/m2
AE--- emitter cross-sectional area/m2
λCs--- thermal coefficient/Wm of caesium steam-1·K-1
δCs--- caesium steam width of air gap/m;
φE--- transmitting electrode potential;
φC--- receive electrode potential;
E --- electron charge;
σ --- black body radiation constant, 5.67E-14W/ (mm2·K4);
L --- emitter and receiving pole length;
χC--- receiving pole work function;
Receiving pole equation of heat balance is calculated by formula (15):
In formula:
ρC--- density/kgm of receiving pole-3
VC--- volume/kgm of receiving pole-3
cC--- specific heat/Jkg of receiving pole-1·K-1
AC--- receiving pole cross-sectional area/m2
λHe--- thermal coefficient/Wm of helium-1·K-1
δHe--- helium width of air gap/m;
εIS--- stainless steel inner sleeve and the emissivity for receiving pole surface;
K --- Boltzmann constant;
Stainless steel inner sleeve equation of heat balance is calculated by formula (16):
In formula:
ρSI--- density/kgm of stainless steel inner sleeve-3
cSI--- specific heat/Jkg of stainless steel inner sleeve-1·K-1
ПC--- unit length receiving pole exterior surface area/m2
εCS--- pole surface is received to the emissivity of stainless steel sleeve pipe;
Tf--- temperature/K of coolant;
ПSI--- unit length stainless steel exterior surface area/m2
ASI--- stainless steel inner sleeve cross-sectional area/m2
hfI--- coolant and the inner sleeve wall surface coefficient of heat transfer/Wm-2·K-1
Above-mentioned thermion nuclear reactor for space reactor core heat transfer Nonlinear differential eguations are solved using GEAR algorithm, obtain electricity The Temperature Distribution of pole;
Step 3, the potential and current distribution for calculating t moment heap core electrode, establish the electric potential balancing of emitter and receiving pole Ordinary differential system:
Emitter electric potential balancing is calculated by formula (17):
In formula:
φE--- transmitting electrode potential;
J --- current density/Acm-2
L --- electrode axial length/cm;
Formula (17) boundary condition is given by formula (18) and formula (19):
In formula:
Voutput--- emitter output voltage/V;
RE1--- emitter head end connection resistance/Ω;
RE2--- emitter end connection resistance/Ω;
Emitter electric potential balancing is calculated by formula (20):
In formula: φC--- receive electrode potential;
Wherein, formula (20) boundary condition is given by formula (21) and formula (22):
In formula:
RC1--- receiving pole head end connection resistance/Ω;
RC2--- receiving pole end connection resistance/Ω;
Using solution by iterative method potential and current distribution, Potential Distributing is first assumed, obtained according to Potential Distributing and Temperature Distribution To current distribution, the ordinary differential system of electrode potential is solved using chasing method, new Potential Distributing is obtained, as iterative process New Potential Distributing is iterated calculating until meeting required precision, just obtains the potential current distribution of electrode;
Step 4: according to the potential current distribution of acquired electrode, the concatenated connection type of thermionic fuel element, heat The output power of ion space nuclear reactor power supply reactor core adds for single thermionic fuel element power with voltage with output voltage It is a thermionic fuel element electric current with, electric current;
Step 5: according to the distribution of thermion nuclear reactor for space power supply core temperature, electrode potential current distribution, carrying out down The calculating of one step, cycle calculations are until reaching end time;
Compared with prior art, the present invention has following outstanding feature:
General thermion nuclear reactor for space entirety reactor core is studied, can accurately reflect the thermoelectricity of full heap Characteristic, the thermion nuclear reactor for space pyroelecthc properties that different structure and power may be implemented calculate, and reduce to thermion sky Between nuclear reactor structure and parameter requirement, effectively increase this method to the adaptability of different problems.This method can calculate The pyroelecthc properties of general thermion nuclear reactor for space power supply transient state run plan when being nuclear reactor for space power supply transient operation Summary, electrical system control scheme etc. provide research method.
Detailed description of the invention
Fig. 1 is the method for the present invention flow chart.
Specific embodiment
Invention is further described in detail with reference to the accompanying drawings and detailed description:
A kind of general thermion nuclear reactor for space reactor core transient state pyroelecthc properties comprehensive analysis method of the invention, uses GEAR algorithm solves the distribution of thermion nuclear reactor for space core temperature, solves electrode potential distribution using chasing method, iteration is asked Solve each moment reactor core electromotive power output, output voltage, output electric current.As shown in Figure 1, this method detailed process includes with lower section Face:
Step 1: thermionic fuel element structure and parameter being determined according to user demand, determine each layer of thermionic fuel element Size, the temperature of the power distribution and coolant of fuel of structure, divide radial and axial node number according to demand;
Step 2: calculating current t moment thermion nuclear reactor for space core temperature distribution, the structure obtained using step 1 Establish the non-linear differential equation of heat balance group about the diabatic process of thermion nuclear reactor for space reactor core respectively with parameter;
General thermion nuclear reactor for space reactor core is made of thermionic fuel element and moderator matrix, thermion combustion Expect element mainly by fuel region, fission gas gap, emitter, caesium gas-bearing formation, receiving pole, helium layer, stainless steel inner sleeve, cold But agent and stainless steel outer sleeve pipe are constituted;
Reactor fission power is solved using the point reactor model dynamical equation of six groups of delayed neutrons is considered first;Point heap mould Type considers the influence of delayed neutron counterincision Variable power and the Reactivity feedback of fuel, coolant and structure member simultaneously, because This is the first order differential equation system of a coupling;Simultaneously as reactivity is time correlation variable, therefore equation group is non-linear 's;Point reactor model dynamical equation is calculated by formula (1) and formula (2);
In formula:
P (t) --- t moment reactor fission power/W;
T --- calculate time/s;
Λ --- neutron generation time/s;
β --- total effective delayed neutron fraction;
βi--- i-th group of delayed neutron fraction;
λi--- decay coefficient/s of i-th group of delayed neutron-1
Ci(t) --- the concentration/m of i-th group of delayed neutron of t moment-3
nc--- delayed neutron group number;
ρ (t) --- total reactivity/$;
The reactivity of reactor can because out-pile reactivity introduce or heap in Reactivity feedback due to change;Pass through corresponding machine Reason model or rule-of-thumb relation establish the reactive solving model of each section;The total reactivity of reactor is calculated by formula (3);
ρ (t)=ρD(t)+∑ρi(t) formula (3)
In formula:
ρ (t) --- total reactivity/$;
ρD(t) --- reactivity/$ that control rotary drum and shutdown rotary drum introduce;
ρi(t) --- each material Reactivity feedback/$;
The Reactivity feedback considered in reactor physics model includes: UO2The temperature of the Doppler effect of fuel, electrode Feedback, moderator temperature feedback and reflecting layer temperature feedback;It is most important for most of operating conditions of thermionic reactor Be the positive-effect of moderator and the negative effect of thermionic fuel element;
The Doppler of fuel, which feeds back to formula (4), to be calculated:
In formula:
--- the Doppler of fuel feeds back;
TU--- fuel temperature/K;
T0--- reference temperature/K;
Emitter and receiving pole Reactivity feedback are calculated by formula (5):
In formula:
--- emitter and receiving pole Reactivity feedback;
TE--- emitter temperature/K;
TC--- receiving pole temperature/K;
Moderator Reactivity feedback coefficient is calculated by formula (6):
--- moderator Reactivity feedback;
TM--- zircoium hydride moderator temperature/K;
Wherein parameter phi is determined by formula (7):
Reflecting layer Reactivity feedback coefficient is calculated by formula (8):
In formula:
--- reflecting layer Reactivity feedback;
TR--- reflecting layer temperature/K;
Rotary drum reactivity is controlled to introduce by formula (9) calculating:
In formula:
ρD--- control rotary drum reactivity introduces;
θ --- control rotary drum rotational angle/degree;
Decay power mainly includes that the radioactive decay of neutron absorption product and fission product is decayed by simplification Heat is solved and is calculated by formula (10) and formula (11):
In formula:
Pd(t) --- t moment reactor decay power/W;
Hi(t) --- the concentration/m of i-th group of fission product of t moment-3
--- the share of i-th group of fission product;
--- decay coefficient/s of i-th group of fission product-1
According to the reactor core general power that the solving model of fission power and decay power obtains, according to shared by each control volume of fuel Power fraction be added in fuel control volume as inner heat source, in reactor core thermal-hydraulic solving model, by formula (12) It calculates;
QV=P φ/V formula (12)
In formula:
QV--- volume inner heat source/Wm of fuel control volume-3
P --- reactor general power/W;
φ --- fuel control volume heat release rate accounts for the share of reactor general power;
Volume/m of V --- fuel control volume3
Middle submodel utilized above obtains inner heat source, and fuel region equation of heat balance is calculated by formula (13):
In formula:
ρU--- density/kgm of fuel pellet-3
cU--- specific heat/Jkg of fuel pellet-1·K-1
TU--- temperature/K of fuel pellet;
λU--- thermal coefficient/Wm of fuel pellet-1·K-1
Radius/m of r --- fuel pellet;
QV--- heat source density/Wm of fuel control volume-3
Emitter equation of heat balance is calculated by formula (14):
In formula:
ρE--- density/kgm of emitter-3
VE--- volume/kgm of emitter-3
cE--- specific heat/Jkg of emitter-1·K-1
λG--- thermal coefficient/Wm of fission gas-1·K-1
δG--- fission gas gap width/m;
εUE--- the emissivity of fuel and emitter surface;
εEC--- emitter and the emissivity for receiving pole surface;
λU--- thermal coefficient/Wm of fuel pellet-1·K-1
ПE--- unit length emitter exterior surface area/m2
AE--- emitter cross-sectional area/m2
λCs--- thermal coefficient/Wm of caesium steam-1·K-1
δCs--- caesium steam width of air gap/m;
φE--- transmitting electrode potential;
φC--- receive electrode potential;
E --- electron charge;
σ --- black body radiation constant, 5.67E-14W/ (mm2·K4);
L --- emitter and receiving pole length;
χC--- receiving pole work function;
Receiving pole equation of heat balance is calculated by formula (15):
In formula:
ρC--- density/kgm of receiving pole-3
VC--- volume/kgm of receiving pole-3
cC--- specific heat/Jkg of receiving pole-1·K-1
AC--- receiving pole cross-sectional area/m2
λHe--- thermal coefficient/Wm of helium-1·K-1
δHe--- helium width of air gap/m;
εIS--- stainless steel inner sleeve and the emissivity for receiving pole surface;
K --- Boltzmann constant;
Stainless steel inner sleeve equation of heat balance is calculated by formula (16):
In formula:
ρSI--- density/kgm of stainless steel inner sleeve-3
cSI--- specific heat/Jkg of stainless steel inner sleeve-1·K-1
ПC--- unit length receiving pole exterior surface area/m2
εCS--- pole surface is received to the emissivity of stainless steel sleeve pipe;
Tf--- temperature/K of coolant;
ПSI--- unit length stainless steel exterior surface area/m2
ASI--- stainless steel inner sleeve cross-sectional area/m2
hfI--- coolant and the inner sleeve wall surface coefficient of heat transfer/Wm-2·K-1
Above-mentioned thermion nuclear reactor for space reactor core heat transfer Nonlinear differential eguations are solved using GEAR algorithm, obtain electricity The Temperature Distribution of pole;
Step 3, the potential and current distribution for calculating t moment heap core electrode, establish the electric potential balancing of emitter and receiving pole Ordinary differential system:
Emitter electric potential balancing is calculated by formula (17):
In formula:
φE--- transmitting electrode potential;
J --- current density/Acm-2
L --- electrode axial length/cm;
Formula (17) boundary condition is given by formula (18) and formula (19):
In formula:
Voutput--- emitter output voltage/V;
RE1--- emitter head end connection resistance/Ω;
RE2--- emitter end connection resistance/Ω
Emitter electric potential balancing is calculated by formula (20):
In formula: φC--- receive electrode potential;
Wherein, formula (20) boundary condition is given by formula (21) and formula (22):
In formula:
RC1- receiving pole head end connection resistance/Ω;
RC2- receiving pole end connection resistance/Ω;
Using solution by iterative method potential and current distribution, Potential Distributing is first assumed, obtained according to Potential Distributing and Temperature Distribution To current distribution, the ordinary differential system of electrode potential is solved using chasing method, new Potential Distributing is obtained, as iterative process New Potential Distributing is iterated calculating until meeting required precision, just obtains the potential current distribution of electrode;
Step 4: according to the potential current distribution of acquired electrode, the concatenated connection type of thermionic fuel element, heat The output power of ion space nuclear reactor power supply reactor core adds for single thermionic fuel element power with voltage with output voltage It is a thermionic fuel element electric current with, electric current;
Step 5: according to the distribution of thermion nuclear reactor for space power supply core temperature, electrode potential current distribution, carrying out down The calculating of one step, cycle calculations are until reaching end time.

Claims (1)

1. a kind of general thermion nuclear reactor for space reactor core transient state pyroelecthc properties comprehensive analysis method, it is characterised in that: packet Include following steps:
Step 1: thermionic fuel element structure and parameter being determined according to user demand, determine each layer structure of thermionic fuel element Size, fuel power distribution and coolant temperature, divide according to demand radial with axial node number;
Step 2: calculating current t moment thermion nuclear reactor for space core temperature distribution, the structure and ginseng obtained using step 1 Number establishes the non-linear differential equation of heat balance group about the diabatic process of thermion nuclear reactor for space reactor core respectively;
General thermion nuclear reactor for space reactor core is made of thermionic fuel element and moderator matrix, thermionic fuel member Part is mainly by fuel region, fission gas gap, emitter, caesium gas-bearing formation, receiving pole, helium layer, stainless steel inner sleeve, coolant It is constituted with stainless steel outer sleeve pipe;
Reactor fission power is solved using the point reactor model dynamical equation of six groups of delayed neutrons is considered first;Point reactor model is same When consider the influence of delayed neutron counterincision Variable power and the Reactivity feedback of fuel, coolant and structure member, therefore be The first order differential equation system of one coupling;Simultaneously as reactivity is time correlation variable, therefore equation group is nonlinear;Point Heap model dynamical equation is calculated by formula (1) and formula (2);
In formula:
P (t) --- t moment reactor fission power/W;
T --- calculate time/s;
Λ --- neutron generation time/s;
β --- total effective delayed neutron fraction;
βi--- i-th group of delayed neutron fraction;
λi--- decay coefficient/s of i-th group of delayed neutron-1
Ci(t) --- the concentration/m of i-th group of delayed neutron of t moment-3
nc--- delayed neutron group number;
ρ (t) --- total reactivity/$;
The reactivity of reactor can because out-pile reactivity introduce or heap in Reactivity feedback due to change;Pass through corresponding mechanism mould Type or rule-of-thumb relation establish the reactive solving model of each section;The total reactivity of reactor is calculated by formula (3);
ρ (t)=ρD(t)+∑ρi(t) formula (3)
In formula:
ρ (t) --- total reactivity/$;
ρD(t) --- reactivity/$ that control rotary drum and shutdown rotary drum introduce;
ρi(t) --- each material Reactivity feedback/$;
The Reactivity feedback considered in reactor physics model includes: UO2The Doppler effect of fuel, electrode temperature feedback, Moderator temperature feedback and reflecting layer temperature feedback;For most of operating conditions of thermionic reactor, it is most important that The positive-effect of moderator and the negative effect of thermionic fuel element;
The Doppler of fuel, which feeds back to formula (4), to be calculated:
In formula:
--- the Doppler of fuel feeds back;
TU--- fuel temperature/K;
T0--- reference temperature/K;
Emitter and receiving pole Reactivity feedback are calculated by formula (5):
In formula:
--- emitter and receiving pole Reactivity feedback;
TE--- emitter temperature/K;
TC--- receiving pole temperature/K;
Moderator Reactivity feedback coefficient is calculated by formula (6):
--- moderator Reactivity feedback;
TM--- zircoium hydride moderator temperature/K;
Wherein parameter phi is determined by formula (7):
Reflecting layer Reactivity feedback coefficient is calculated by formula (8):
In formula:
--- reflecting layer Reactivity feedback;
TR--- reflecting layer temperature/K;
Rotary drum reactivity is controlled to introduce by formula (9) calculating:
In formula:
ρD--- control rotary drum reactivity introduces;
θ --- control rotary drum rotational angle/degree;
Decay power mainly includes that the radioactive decay of neutron absorption product and fission product by simplification obtains decay heat, is asked Solution is calculated by formula (10) and formula (11):
In formula:
Pd(t) --- t moment reactor decay power/W;
Hi(t) --- the concentration/m of i-th group of fission product of t moment-3
--- the share of i-th group of fission product;
--- decay coefficient/s of i-th group of fission product-1
According to the reactor core general power that the solving model of fission power and decay power obtains, according to function shared by each control volume of fuel Rate share is added in fuel control volume as inner heat source, for being calculated in reactor core thermal-hydraulic solving model by formula (12);
QV=P φ/V formula (12)
In formula:
QV--- volume inner heat source/Wm of fuel control volume-3
P --- reactor general power/W;
φ --- fuel control volume heat release rate accounts for the share of reactor general power;
Volume/m of V --- fuel control volume3
Middle submodel utilized above obtains inner heat source, and fuel region equation of heat balance is calculated by formula (13):
In formula:
ρU--- density/kgm of fuel pellet-3
cU--- specific heat/Jkg of fuel pellet-1·K-1
TU--- temperature/K of fuel pellet;
λU--- thermal coefficient/Wm of fuel pellet-1·K-1
Radius/m of r --- fuel pellet;
QV--- heat source density/Wm of fuel control volume-3
Emitter equation of heat balance is calculated by formula (14):
In formula:
ρE--- density/kgm of emitter-3
VE--- volume/kgm of emitter-3
cE--- specific heat/Jkg of emitter-1·K-1
λG--- thermal coefficient/Wm of fission gas-1·K-1
δG--- fission gas gap width/m;
εUE--- the emissivity of fuel and emitter surface;
εEC--- emitter and the emissivity for receiving pole surface;
λU--- thermal coefficient/Wm of fuel pellet-1·K-1
ПE--- unit length emitter exterior surface area/m2
AE--- emitter cross-sectional area/m2
λCs--- thermal coefficient/Wm of caesium steam-1·K-1
δCs--- caesium steam width of air gap/m;
φE--- transmitting electrode potential;
φC--- receive electrode potential;
E --- electron charge;
σ --- black body radiation constant, 5.67E-14W/ (mm2·K4);
L --- emitter and receiving pole length;
χC--- receiving pole work function;
Receiving pole equation of heat balance is calculated by formula (15):
In formula:
ρC--- density/kgm of receiving pole-3
VC--- volume/kgm of receiving pole-3
cC--- specific heat/Jkg of receiving pole-1·K-1
AC--- receiving pole cross-sectional area/m2
λHe--- thermal coefficient/Wm of helium-1·K-1
δHe--- helium width of air gap/m;
εIS--- stainless steel inner sleeve and the emissivity for receiving pole surface;
K --- Boltzmann constant;
Stainless steel inner sleeve equation of heat balance is calculated by formula (16):
In formula:
ρSI--- density/kgm of stainless steel inner sleeve-3
cSI--- specific heat/Jkg of stainless steel inner sleeve-1·K-1
ΠC--- unit length receiving pole exterior surface area/m2
εCS--- pole surface is received to the emissivity of stainless steel sleeve pipe;
Tf--- temperature/K of coolant;
ΠSI--- unit length stainless steel exterior surface area/m2
ASI--- stainless steel inner sleeve cross-sectional area/m2
hfI--- coolant and the inner sleeve wall surface coefficient of heat transfer/Wm-2·K-1
Above-mentioned thermion nuclear reactor for space reactor core heat transfer Nonlinear differential eguations are solved using GEAR algorithm, obtain electrode Temperature Distribution;
Step 3, the potential and current distribution for calculating t moment heap core electrode, establish the normal of the electric potential balancing of emitter and receiving pole Differential equation group:
Emitter electric potential balancing is calculated by formula (17):
In formula:
φE--- transmitting electrode potential;
J --- current density/Acm-2
L --- electrode axial length/cm;
Formula (17) boundary condition is given by formula (18) and formula (19):
In formula:
Voutput--- emitter output voltage/V;
RE1--- emitter head end connection resistance/Ω;
RE2--- emitter end connection resistance/Ω;
Emitter electric potential balancing is calculated by formula (20):
In formula: φC--- receive electrode potential;
Wherein, formula (20) boundary condition is given by formula (21) and formula (22):
In formula:
RC1--- receiving pole head end connection resistance/Ω;
RC2--- receiving pole end connection resistance/Ω;
Using solution by iterative method potential and current distribution, Potential Distributing is first assumed, electricity is obtained according to Potential Distributing and Temperature Distribution Flow distribution is solved the ordinary differential system of electrode potential using chasing method, obtains new Potential Distributing, new as iterative process Potential Distributing is iterated calculating until meeting required precision, just obtains the potential current distribution of electrode;
Step 4: according to the potential current distribution of acquired electrode, the concatenated connection type of thermionic fuel element, thermion The output power and output voltage of nuclear reactor for space power supply reactor core are that single thermionic fuel element power and voltage sum it up, electricity Stream is a thermionic fuel element electric current;
Step 5: according to the distribution of thermion nuclear reactor for space power supply core temperature, electrode potential current distribution, carrying out in next step Calculating, cycle calculations are until reaching end time.
CN201910283124.8A 2019-04-10 2019-04-10 Universal method for analyzing transient thermoelectric characteristics of power supply of thermionic space nuclear reactor Active CN110060788B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910283124.8A CN110060788B (en) 2019-04-10 2019-04-10 Universal method for analyzing transient thermoelectric characteristics of power supply of thermionic space nuclear reactor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910283124.8A CN110060788B (en) 2019-04-10 2019-04-10 Universal method for analyzing transient thermoelectric characteristics of power supply of thermionic space nuclear reactor

Publications (2)

Publication Number Publication Date
CN110060788A true CN110060788A (en) 2019-07-26
CN110060788B CN110060788B (en) 2020-08-25

Family

ID=67318642

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910283124.8A Active CN110060788B (en) 2019-04-10 2019-04-10 Universal method for analyzing transient thermoelectric characteristics of power supply of thermionic space nuclear reactor

Country Status (1)

Country Link
CN (1) CN110060788B (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110853777A (en) * 2019-11-07 2020-02-28 西安交通大学 Fuel assembly structure for enhancing negative feedback of temperature of gas-cooled fast reactor and reactor core structure
CN111048221A (en) * 2019-12-26 2020-04-21 西安交通大学 Method for accurately obtaining reactivity feedback change in fast neutron reactor transient process
CN113255249A (en) * 2021-06-07 2021-08-13 清华大学 Multi-physical coupling transient calculation method and device for heat pipe solid state stack
CN113779723A (en) * 2021-09-13 2021-12-10 西安交通大学 Method for analyzing heat transfer characteristics of heat pipe radiator of space pile under near-earth orbit
CN113793711A (en) * 2021-09-13 2021-12-14 西安交通大学 Method for analyzing coupling heat transfer characteristics of lithium-cooled nuclear reactor and Stirling generator
CN115270660A (en) * 2022-08-04 2022-11-01 上海交通大学 Multi-scale multi-physical field coupling analysis method for transient behavior of space thermionic reactor

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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
RU159871U1 (en) * 2015-05-18 2016-02-20 Российская Федерация, от имени которой выступает Государственная корпорация по атомной энергии "Росатом" FUEL FUEL ELEMENT OF SPACE ENERGY PLANT NUCLEAR REACTOR
CN107122331A (en) * 2017-04-20 2017-09-01 西安交通大学 A kind of coupling of multiple physics method in presurized water reactor transient state calculating
CN108122623A (en) * 2017-12-25 2018-06-05 中国科学院合肥物质科学研究院 A kind of deep-sea nuclear power apparatus

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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
RU159871U1 (en) * 2015-05-18 2016-02-20 Российская Федерация, от имени которой выступает Государственная корпорация по атомной энергии "Росатом" FUEL FUEL ELEMENT OF SPACE ENERGY PLANT NUCLEAR REACTOR
CN107122331A (en) * 2017-04-20 2017-09-01 西安交通大学 A kind of coupling of multiple physics method in presurized water reactor transient state calculating
CN108122623A (en) * 2017-12-25 2018-06-05 中国科学院合肥物质科学研究院 A kind of deep-sea nuclear power apparatus

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
刘逍等: "空间堆辐射散热器设计分析", 《原子能科学技术》 *
张文文等: "新型热管反应堆堆芯热工安全分析", 《原子能科学技术》 *
张文文等: "热管改进型热离子反应堆瞬态分析程序开发", 《原子能科学技术》 *

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110853777A (en) * 2019-11-07 2020-02-28 西安交通大学 Fuel assembly structure for enhancing negative feedback of temperature of gas-cooled fast reactor and reactor core structure
CN111048221A (en) * 2019-12-26 2020-04-21 西安交通大学 Method for accurately obtaining reactivity feedback change in fast neutron reactor transient process
CN111048221B (en) * 2019-12-26 2021-08-13 西安交通大学 Method for accurately obtaining reactivity feedback change in fast neutron reactor transient process
CN113255249A (en) * 2021-06-07 2021-08-13 清华大学 Multi-physical coupling transient calculation method and device for heat pipe solid state stack
CN113255249B (en) * 2021-06-07 2022-06-10 清华大学 Multi-physical coupling transient calculation method and device for heat pipe solid state stack
CN113779723A (en) * 2021-09-13 2021-12-10 西安交通大学 Method for analyzing heat transfer characteristics of heat pipe radiator of space pile under near-earth orbit
CN113793711A (en) * 2021-09-13 2021-12-14 西安交通大学 Method for analyzing coupling heat transfer characteristics of lithium-cooled nuclear reactor and Stirling generator
CN113793711B (en) * 2021-09-13 2022-12-02 西安交通大学 Method for analyzing coupling heat transfer characteristics of lithium-cooled nuclear reactor and Stirling generator
CN113779723B (en) * 2021-09-13 2022-12-09 西安交通大学 Method for analyzing heat transfer characteristics of heat pipe radiator of space pile under near-ground orbit
CN115270660A (en) * 2022-08-04 2022-11-01 上海交通大学 Multi-scale multi-physical field coupling analysis method for transient behavior of space thermionic reactor

Also Published As

Publication number Publication date
CN110060788B (en) 2020-08-25

Similar Documents

Publication Publication Date Title
CN110060788A (en) A kind of general thermion nuclear reactor for space power supply thermal transient Analysis of Electrical Characteristics method
Okano et al. Compact reversed shear tokamak reactor with a superheated steam cycle
Steiner The technological requirements for power by fusion
Yang et al. Core design study on CANDU-SCWR with 3D neutronics/thermal-hydraulics coupling
CN115793432B (en) Spatial thermal ion nuclear power source control method based on model predictive control
US11289236B2 (en) Combination reactor gamma radiation power harvesting reactor power distribution measurement, and support to coolant freezing protection system for liquid metal and molten salt-cooled reactor systems
Boczar et al. Reactor physics studies for a pressure tube supercritical water reactor (PT-SCWR)
CN106991272A (en) A kind of accurate method for calculating nucleic atom cuclear density in calculating for burnup
Guo et al. Concept design and neutronics analysis of a heat pipe cooled nuclear reactor with CERMET fuel
Şahi̇n et al. Fast hybrid thermionic blankets with actinide waste fuel
Lu et al. Progress on neutronic analysis for CFETR
Wulandari et al. Neutronic Performances of 100 MWe MSR with Weapon Grade Plutonium Fuel
Şahіn Investigation of lanthanides as neutron multipliers for hybrid and fusion reactor blankets
Shaposhnik et al. Shutdown margin for high conversion BWRs operating in Th-233U fuel cycle
El-Genk et al. An analysis of disassembling the radial reflector of a thermionic space nuclear reactor power system
Marshall RSMASS-D models: An improved method for estimating reactor and shield mass for space reactor applications
King et al. Thermal Aspects of Using ThO2 in a 54-and 64-Element Fuel Bundle Designed for SCWR Application
Stubbins Thermal performance of thermionic diodes for fusion power production
Şahin et al. Hybrid thermionic space reactors for power and propulsion
Dai et al. Physical and thermal coupling calculation for accelerator driven subcritical core
El‐Genk et al. An analysis of thermionic space nuclear reactor power system: I. Effect of disassembling radial reflector, following a reactivity initiated accident
Tang et al. Thermal-Hydraulic Analysis of TOPAZ-II With Modified RELAP5
Magelssen Gain Scaling Relations—Heavy-Ion Targets
Davis et al. Review of industry-proposed in-pile thermionic space reactors. Volume I-General
Jiao et al. TRANSIENT NUCLEAR THERMAL COUPLING CHARACTERISTICS OF A MEGAWATT HEAT PIPE COOLED REACTOR

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant