JPH0249678B2 - - Google Patents
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- Publication number
- JPH0249678B2 JPH0249678B2 JP58070090A JP7009083A JPH0249678B2 JP H0249678 B2 JPH0249678 B2 JP H0249678B2 JP 58070090 A JP58070090 A JP 58070090A JP 7009083 A JP7009083 A JP 7009083A JP H0249678 B2 JPH0249678 B2 JP H0249678B2
- Authority
- JP
- Japan
- Prior art keywords
- control
- power
- output
- control rod
- rods
- 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.)
- Expired - Lifetime
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Classifications
-
- Y—GENERAL 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
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E30/00—Energy generation of nuclear origin
- Y02E30/30—Nuclear fission reactors
Landscapes
- Monitoring And Testing Of Nuclear Reactors (AREA)
- Photoreceptors In Electrophotography (AREA)
Description
【発明の詳細な説明】
本発明は、早い出力変化に対応できかつ出力分
布制御可能な出力制御装置に特徴を有する加圧水
型原子炉に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a pressurized water nuclear reactor characterized by a power control device that can respond to rapid power changes and can control power distribution.
従来、原子炉における出力制御の一手段とし
て、中性子吸収材によつて構成した制御棒が使用
されており、通常、前記制御棒の中性子吸収材は
上端から下端まで軸方向均等に設定されている。 Conventionally, a control rod made of neutron absorbing material has been used as a means of power control in a nuclear reactor, and the neutron absorbing material of the control rod is usually set evenly in the axial direction from the upper end to the lower end. .
また、前記制御棒によつて原子炉の出力を制御
する場合には、制御棒の上下方向移動操作によつ
て原子炉内の出力分布が変化するとともに、出力
の変化に伴う原子炉固有の反応度フイードバツク
による出力分布変化が生じ、一方、原子炉を安全
かつ効率的に運転するためには、出力分布は一定
の範囲内に制限する必要がある。(例えば、炉内
出力が過大になると、その部分の燃料が損傷する
ため。)
即ち、原子炉の出力制御には、中性子束の制
御、つまり反応度の制御と、出力分布の制御とを
行なう必要があつて、例えば、特公昭43−20225
号公報のように、中性子吸収能力の異なる素子を
中性子吸収能力の大きい順に履帯状に配列した制
御棒が提案されているが、その具体的な中性子吸
収能力の分布については明らかにされてなく、ま
た、前記履帯状の制御棒は、現在の加圧水型原子
炉には適用できない。 In addition, when controlling the output of a nuclear reactor using the control rods, the power distribution within the reactor changes due to the vertical movement of the control rods, and the reactor-specific reactions associated with changes in output change. Power distribution changes due to temperature feedback, and on the other hand, in order to operate a nuclear reactor safely and efficiently, the power distribution must be limited within a certain range. (For example, if the power in the reactor becomes excessive, the fuel in that area will be damaged.) In other words, the power of the reactor is controlled by controlling the neutron flux, that is, the reactivity, and the power distribution. For example, if there is a need,
As in the publication, a control rod in which elements with different neutron absorption capacities are arranged in a track-like manner in descending order of neutron absorption capacity has been proposed, but the specific distribution of neutron absorption capacity has not been clarified. Further, the track-shaped control rod cannot be applied to current pressurized water reactors.
さらに、出力分布制御手段として現在採用され
ているものに、軸方向中性子束一定値運転法があ
り該運転法についてさらに説明すると、例えば、
定格出力運転状態から出力を低下させると、炉心
の軸方向出力分布は炉心上部に片寄る傾向がある
が、これは原子炉の減速材温度係数が負であるた
め、出力低下によつて炉心上部の減速材温度か低
下し、これにより炉心上部に正の反応度が添加さ
れるためによるものである。前記出力分布の歪を
修正するとともに出力低下に必要な反応度制御を
行なうために炉心へ上方から制御棒が挿入され
る。しかし、その際の制御棒挿入は、出力分布制
御が主になつており、出力低下に十分な反応度を
補償するところまで制御棒を挿入することは、出
力分布制御上から許されない(異常分布が生ず
る)。 Furthermore, the method currently employed as a power distribution control means is a constant axial neutron flux operation method, and to further explain this operation method, for example,
When the power is reduced from the rated power operating state, the axial power distribution of the core tends to shift toward the upper part of the core. This is because the moderator temperature decreases, which adds positive reactivity to the upper part of the core. Control rods are inserted into the reactor core from above in order to correct the distortion in the power distribution and perform reactivity control necessary to reduce the power. However, control rod insertion at this time is mainly for power distribution control, and inserting control rods to the point where sufficient reactivity is compensated for the output drop is not allowed from the perspective of power distribution control (abnormal distribution occurs).
よつて、別の反応制御法、即ち一次冷却材中の
中性子吸収材濃度の制御が行われる。該制御法で
は、中性子吸収材が原子炉内に一様に分散される
ため出力分布制御上問題となる出力分布の変化は
発生しない。また、低出力状態から定格出力へ復
帰する際は、概ね前記の逆操作にて行われる。し
かし、この方法は、冷却材中の中性子吸収材濃度
の調整による反応度制御を併用している点で弱点
になつている。また、冷却材中の中性子吸収材と
しては通常ほう酸が用いられており、その濃度調
整方法には現在後記の2方法を単独または併用し
ている。その方法の一つは、ほう酸濃度を希釈す
る場合には、一次冷却材を抽出し同時に等量の純
水を注入して行ない、また、濃縮する場合には、
前記希釈の際の純水の代りに高濃度のほう酸水を
注入して行なつて、一次系全体のほう酸濃度を調
整するのであるが、一次系冷却材の量に比べ注入
量が限られるため、時間遅れになる難点がある。
また、他の方法は、イオン交換樹脂を用いてその
樹脂の温度によるほう素の吸着力差を利用したも
のであつて、この場合も一次冷却材全体を前記樹
脂に接触させるとともに樹脂温度の制御を行なう
ため、時間遅れになるのを避けることができず、
制御棒のような素早い対応が得られず早い出力変
化に対処できない。即ち、出力変化割合は一次冷
却材中の中性子吸収材濃度の制御能力によつて制
限される。 Therefore, another reaction control method is used, namely control of the neutron absorber concentration in the primary coolant. In this control method, since the neutron absorbing material is uniformly distributed within the reactor, changes in the power distribution that pose a problem in power distribution control do not occur. Furthermore, when returning from a low output state to the rated output, the above-mentioned operation is generally reversed. However, this method has a weakness in that it also uses reactivity control by adjusting the neutron absorber concentration in the coolant. Further, boric acid is usually used as a neutron absorbing material in the coolant, and the two methods described below are currently used alone or in combination to adjust its concentration. One method is to dilute the boric acid concentration by extracting the primary coolant and simultaneously injecting an equal amount of pure water, and to concentrate it,
Highly concentrated boric acid water is injected instead of pure water during the dilution to adjust the boric acid concentration in the entire primary system, but since the amount of injection is limited compared to the amount of primary system coolant. However, there is a problem with time delays.
Another method uses an ion exchange resin and takes advantage of the difference in adsorption power of boron depending on the temperature of the resin. In this case as well, the entire primary coolant is brought into contact with the resin and the resin temperature is controlled. Due to this, we are unable to avoid delays due to
They cannot respond quickly like control rods and cannot deal with rapid output changes. That is, the rate of output change is limited by the ability to control the neutron absorber concentration in the primary coolant.
さらに、大きい出力分布変化をもたらす制御棒
の炉心への挿入度合を小さくするための運転方法
として、特公昭51−47837号公報のように、多数
の制御集合体を同一構造および同一使用態様(任
務)の群即ちパンクとした出力制御バンク、ドツ
プラ制御バンク、キセノン制御バンクの3種の制
御バンクによつて出力変動を行なうようにしたも
のが開発されており、前記のドツプラ制御バンク
は、出力低下によるドツプラ効果反応度のみを制
御するものであつて、低出力時には全挿入とし、
定格出力時には全引抜として使用されるようにな
つている。しかし、該方法では、出力制御に必要
な反応度制御は全て制御棒で行なわれるため、早
い出力変化に対応できるものと考えられるが、減
速材温度変化による反応度変化が無視され、ま
た、出力分布制御についての配慮がなされていな
い。 Furthermore, as an operating method to reduce the degree of insertion of control rods into the reactor core, which causes large changes in power distribution, as in Japanese Patent Publication No. 51-47837, a large number of control assemblies are arranged with the same structure and the same usage (mission). ), that is, a punctured output control bank, a Doppler control bank, and a xenon control bank, have been developed to perform output fluctuations. It controls only the Doppler effect reactivity, and at low output it is fully inserted,
At the rated output, it is used as a full drawer. However, in this method, all reactivity control necessary for output control is performed by the control rods, so it is thought that it can cope with rapid output changes, but it ignores reactivity changes due to moderator temperature changes, and output No consideration was given to distribution control.
本発明は、前記のような実状に鑑みて開発され
たものであつて、多数の核燃料集合体によつて形
成された炉心内に挿入される複数の制御棒集合体
を、出力制御用制御棒集合体群と、出力分布制御
用集合体群とから構成し、前記出力制御用制御棒
集合体群の制御棒を前記炉心の全高にわたつて挿
脱自在とすると共に、その全長にわたつて中性子
吸収能力を一様とし、一方前記出力分布制御用制
御棒集合体群の制御棒を部分出力運転時にのみ前
記炉心に全挿入され、同部分出力運転時外では全
引抜とすると共にその中性子吸収能力の分布を前
記出力制御用制御棒集合体群の制御棒より小さい
上半部と同上半部より更に低い下半部とに分けた
点に特徴を有し、早い出力変化に対応できかつ出
力分布制御が可能であつて、出力分布歪の少ない
素早い反応度制御機能を有し前記のような欠点を
解消した加圧水型原子炉を供する点にある。 The present invention was developed in view of the above-mentioned actual situation, and it is possible to use a plurality of control rod assemblies inserted into a reactor core formed by a large number of nuclear fuel assemblies as power control control rods. The control rods of the power control rod assemblies can be inserted and removed over the entire height of the reactor core, and the control rods of the power distribution control rod assemblies can be freely inserted and removed over the entire height of the reactor core. The absorption capacity is made uniform, while the control rods of the power distribution control control rod assembly group are fully inserted into the core only during partial power operation, and are fully withdrawn outside of the same partial power operation, and their neutron absorption capacity is It is characterized by dividing the distribution into an upper half that is smaller than the control rods of the control rod assembly group for output control and a lower half that is even lower than the upper half. The object of the present invention is to provide a pressurized water nuclear reactor that is controllable, has a quick reactivity control function with little distortion in power distribution, and eliminates the above-mentioned drawbacks.
本発明は、前記の構成になつており、制御棒の
中性子吸収能力を上下軸方向均等に設定した上下
方向移動操作自在の制御棒集合体群と、制御棒の
中性子吸収能力を下方が小さく上方が大きく設定
した上下方向移動操作自在であつて定格出力運転
時には炉心外に配置される出力分布制御用制御棒
集合体群とを具備しているので、前記制御棒集合
体群を使用するとともに前記出力分布制御用制御
棒集合体群を全挿入にして加圧水型原子炉の低出
力制御を行なうことができ、制御棒のみの出力制
御であるとともに下方が小さく上方が大きく設定
された中性子吸収能力を有する制御棒を全挿入す
ることにより、早い出力変化に対応できかつ出力
分布制御が可能であつて、安全、高効率で出力分
布の歪の少ない素早い反応度制御機能を有し、加
圧水型原子炉の出力制御性能、その信頼性が著し
く向上される。 The present invention has the above-mentioned configuration, and includes a group of control rods that can be freely moved in the vertical direction, in which the neutron absorption capacity of the control rods is set equally in the vertical axis direction, and a group of control rods that can be freely moved in the vertical direction, and the neutron absorption capacity of the control rods is set such that the neutron absorption capacity of the control rods is set to be equal in the upper and lower directions. The control rod assembly group is provided with a control rod assembly group for power distribution control that is set to a large value and is operable to move vertically in the vertical direction and is placed outside the reactor core during rated power operation. It is possible to control the low power of a pressurized water reactor by fully inserting the control rod assembly group for power distribution control, and it is possible to perform low power control of a pressurized water reactor by fully inserting the control rod assembly group for power distribution control.In addition to controlling the power of only the control rods, the neutron absorption capacity is set to be small at the bottom and large at the top. By fully inserting all control rods, it is possible to respond to rapid output changes and control the output distribution, and it has a safe, highly efficient, and quick reactivity control function with little distortion of the output distribution. Its output control performance and reliability are significantly improved.
以下、本発明の実施例を図面参照により説明す
る。 Embodiments of the present invention will be described below with reference to the drawings.
熱出力270万KWクラス、標準3ループの加圧
水型軽水炉について説明すると、第4図に示すよ
うに、その炉心は157体の燃料集合体によつて構
成されているとともに、クラス型の制御棒集合体
を48体配置しさらに13体分の予備制御棒集合体を
取付可能にした出力制御装置が前記炉心に付設さ
れている。 To explain a pressurized water reactor with a thermal output class of 2.7 million KW and a standard 3-loop system, as shown in Figure 4, its core is composed of 157 fuel assemblies, as well as class-type control rod assemblies. A power control device is attached to the core, in which 48 control rod assemblies are arranged and 13 additional control rod assemblies can be attached.
前記の48体の制御棒集合体は、上下軸方向に中
性子吸収能力を均等に設定して上下方向移動操作
自在に配設され、かつ、同一使用態様即ち同じ任
務の6つの制御棒集合体群即ちバンクとし、停止
バンクSA,SBおよび制御バンクA,B,C,D
に分類されており、前記バンクはいずれも出力制
御用制御棒集合体群であつて、通常運転時には前
記制御バンクDが使用される。 The above-mentioned 48 control rod assemblies are arranged so that they can be freely moved in the vertical direction with equal neutron absorption capacity in the vertical axis direction, and are divided into six groups of control rod assemblies that are used in the same manner, that is, have the same mission. In other words, there are three banks, stop banks S A , S B and control banks A, B, C, D.
The banks are all control rod assembly groups for output control, and the control bank D is used during normal operation.
さらに、本実施例においては、前記制御バンク
のほかに、5つの制御棒集合体からなる出力分布
制御用制御棒集合体群即ち出力制御バンクPが設
けられている。前記出力制御バンクPの各制御棒
集合体は、その中性子吸収能力を下方が小さく上
方が大きく設定した構成になつており、該出力制
御バンクPは、出力低下に必要な負の反応度を与
えるとともに、出力低下による出力分布の歪を是
正することができるように前記のような構成に調
整され、低出力時には炉心の上下全長にわたつて
制御棒を挿入する全挿入、定格出力時には炉心外
に引抜いて配置する全引抜として使用され、出力
分布制御機能を有し、また通常の出力制御機能も
有しており、上下方向移動操作自在に構成されて
いる。 Furthermore, in this embodiment, in addition to the control bank, there is provided a control rod assembly group for power distribution control, ie, an output control bank P, consisting of five control rod assemblies. Each control rod assembly of the power control bank P has a configuration in which its neutron absorption capacity is set to be small at the bottom and large at the top, and the power control bank P provides negative reactivity necessary for power reduction. At the same time, the configuration described above has been adjusted to correct the distortion in the power distribution due to a decrease in power.At low power, the control rods are fully inserted across the entire length of the top and bottom of the reactor core, and at rated power, they are inserted outside the core. It is used as a full drawer that is pulled out and placed, has an output distribution control function, and also has a normal output control function, and is configured to be able to be moved vertically.
また、多少の反応度および出力分布の補正は、
従来通りに前記制御バンクDで補うことも可能で
ある。 In addition, some reactivity and output distribution corrections are
It is also possible to supplement with the control bank D in the conventional manner.
本発明の実施例は、前記のような構成になつて
おり、前記の制御棒集合体群即ち制御バンクA、
B、C、Dと、前記の出力分布制御用制御棒集合
体群即ち出力制御バンクPとからなる出力制御装
置により、加圧水型原子炉の出力制御を行なう場
合の有効性、実用性、大型電子計算機によるシユ
ミレーシヨン結果を用いて説明すると、ある時刻
Tにおいて定格出力状態から急速に5%/分の割
合にて50%出力まで出力を低下し、その50%出力
状態を6時間目まで保持したのち、次に、同様に
5%/分の割合で定格出力まで上昇し、その状態
で24時間目まで保持する日負荷追従サイクル運転
を実施した際の主要パラメータを第1図、第2図
に示しており、第1図は、制御棒の中性子吸収能
力を上下軸方向均等に設定した制御棒集合体群つ
まり制御バンクA、B、C、Dの一部のみを使用
(停止バンクSA,SBおよびA、B、C、Dの一部
は全引抜)した場合であつて、曲線1は原子炉の
相対出力、曲線2は制御バンクA(またはB、C)
および曲線3は制御バンクDの炉心内相対位置で
あつて、1.0,0.0がそれらの全引抜と全挿入の位
置を示し、また、第2図は、制御棒の中性子吸収
能力を下方が小さく上方が大きく設定した出力分
布制御用制御棒集合体群即ち出力制御バンクPと
前記制御バンクDを使用した場合であつて、曲線
2′は出力制御バンクPを示しており、また、第
1,2図の曲線4,4′は、出力変化を実現する
ための操作を行なつた際のそれぞれの軸方向中性
子速偏差Δの変化を表わしており、前記偏差Δ
は、次式によるものである。 The embodiment of the present invention has the above-described configuration, and includes the control rod assembly group, that is, the control bank A,
Effectiveness, practicality, and large electronics when controlling the output of a pressurized water reactor using a power control device consisting of the control rods B, C, and D, and the power distribution control control rod assembly group, that is, the power control bank P. To explain using computer simulation results, at a certain time T, the output is rapidly reduced to 50% output at a rate of 5%/min from the rated output state, and after maintaining that 50% output state until the 6th hour. Next, Figures 1 and 2 show the main parameters when a daily load following cycle operation was carried out in which the output was increased to the rated output at a rate of 5%/min and maintained at that state until the 24th hour. Figure 1 shows that only part of the control rod assembly group A, B, C, and D is used (stop banks S A , S Curve 1 is the relative output of the reactor, and curve 2 is the control bank A (or B, C).
Curve 3 is the relative position of control bank D in the core, where 1.0 and 0.0 indicate the fully withdrawn and fully inserted positions. In this case, the control rod assembly group for power distribution control, that is, the power control bank P, and the control bank D are used, and the curve 2' shows the power control bank P, and the first and second Curves 4 and 4' in the figure represent changes in the axial neutron velocity deviation Δ when performing operations to realize output changes, and the deviation Δ
is based on the following equation.
Δ=PT−PB/PT+PB×P
PT:炉心上半分の出力
PB:炉心下半分の出力
P :炉心の相対出力(%)
また、同図の点線5は、軸方向中性子東一定値
運転において、その運転操作に柔軟性を持たせる
ための一定の許容幅即ち許容範囲を示すものであ
り、第1図の場合には、出力低下のために制御バ
ンクA(またはB,C)が全挿入され、反応度の
不足分を制御バンクDで補足するようになつてお
り、制御バンクDも挿入されて軸方向中性子束偏
差Δは許容範囲内に保たれる。しかし、この状
態のままでは核分裂生成物のうちキセノン(中性
子を吸収するが短かい半減期である)の濃度変化
により出力分布は前記偏差Δが負の方向、即
ち、炉心の下半分の出力が増大し、逆に上半分の
出力が減少し、炉心の上、下出力のアンバランス
が増大していく。よつて、それを補正するために
制御バンクDが少し引抜かれ、前記偏差Δは許
容範囲(点線5内)に制御される。 Δ=P T −P B /P T +P B ×P P T : Power of the upper half of the core P B : Power of the lower half of the core P : Relative power of the core (%) In addition, the dotted line 5 in the same figure indicates the axial direction. This indicates a certain tolerance range, that is, a tolerance range, to give flexibility to the operation in neutron east constant value operation.In the case of Fig. 1, control bank A (or B , C) are fully inserted, and the lack of reactivity is supplemented by the control bank D, and the control bank D is also inserted to keep the axial neutron flux deviation Δ within the permissible range. However, if this state continues, changes in the concentration of xenon (which absorbs neutrons but has a short half-life) among the fission products will cause the power distribution to shift in the direction where the deviation Δ is negative, that is, the power in the lower half of the core will decrease. On the other hand, the power output in the upper half of the reactor core decreases, and the imbalance between the upper and lower power outputs of the core increases. Therefore, in order to correct this, the control bank D is slightly withdrawn, and the deviation Δ is controlled within the permissible range (within the dotted line 5).
しかし、定格出力への復帰のために前記制御バ
ンクを引抜くと、出力分布は前記偏差Δが負側
の許容範囲外に出て、制御棒操作で前記偏差Δ
を制御できないようになり、即ち、この状態で制
御棒を挿入しても、出力分布はさらに炉心の下半
分の出力が増大され、上半分の出力が減少し、前
記偏差Δがさらに負側に移行する。軸方向中性
子束一定値運転が不可能となる。前記運転が可能
であるためには前記偏差Δの許容範囲内で全て
の運転が可能である必要がある。 However, when the control bank is pulled out to return to the rated output, the output distribution goes out of the tolerance range on the negative side of the deviation Δ, and when the control rods are operated, the deviation Δ
In other words, even if a control rod is inserted in this state, the power distribution will further increase the power in the lower half of the core, decrease the power in the upper half, and the deviation Δ will become even more negative. Transition. Operation with constant axial neutron flux becomes impossible. In order for the above operation to be possible, all operations must be possible within the allowable range of the deviation Δ.
また、第2図においては、前記出力バンクPを
使用しているため、低出力時の出力分布変化が著
しく少なくなつて、定格出力復帰後においても前
記偏差Δを許容範囲に制御できる。前記時刻T
から17時間目で前記偏差Δが正側に逸脱するの
を防ぐために制御バンクが少し挿入され、また、
2時間後に前記偏差Δが負側に逸脱するのを防
ぐため元の位置まで引抜かれるが、前記偏差Δ
は十分に制御される。 Further, in FIG. 2, since the output bank P is used, the change in the output distribution at low output is significantly reduced, and the deviation Δ can be controlled within the allowable range even after the rated output is restored. Said time T
A control bank is inserted a little to prevent the deviation Δ from deviating to the positive side at the 17th hour, and
After 2 hours, it is pulled out to the original position to prevent the deviation Δ from deviating to the negative side, but the deviation Δ
is well controlled.
なお、第1図および第2図において、制御バン
クDが全引抜されていないのは、運転上の必要性
から定められた要求に従つたものである。 Note that in FIGS. 1 and 2, the control bank D is not fully withdrawn in accordance with a request determined from operational necessity.
さらに、第3図に出力制御バンクPの軸方向中
性子吸収能力を示し、曲線6は、制御バンクDを
基準にとり、その吸収能力を1.0として表わした
ものであつて、また、曲線7は、第2図のシユミ
レーシヨンに使用した出力制御バンクPのもので
ある。即ち、同図から明らかなように、制御棒の
みの使用と前記出力制御バンクPの全挿入によ
り、早い出力変化に対応できかつ出力分布制御が
可能であつて、安全、高効率で出力分布の歪の少
ない素早い反応度制御機能を有し、加圧水型原子
炉の出力制御性能、その信頼性が著しく向上され
る。このように本発明によるときは多数の核燃料
集合体によつて形成された炉心内に挿入される複
数の制御棒集合体を、出力制御用制御棒集合体群
と、出力分布制御用集合体群とから構成し、その
出力制御用制御棒集合体群の制御棒を炉心の全高
にわたつて挿脱自在とすると共に、その全長にわ
たつて中性子吸収能力を一様とし、一方その出力
分布制御用集合体群の制御棒を部分出力運転時の
み炉心に全挿入され、同部分出力運転時外では全
引抜きとすると共にその中性子吸収能力の分布を
前記出力制御用制御棒集合体群の制御棒より小さ
い上半部と同上半部より更に低い下半部とに分け
たものであるから出力分布制御用制御棒集合体群
は迅速に封入されて出力制御用と併用されて部分
出力運転を可能とすると共に部分出力運転時の軽
水の温度低下(炉心上部で生ずる)による出力分
布の偏りを防止でき更にこれを引抜いて全出力
(定格)運転に戻したとき出力分布の変動を少く
することができる等の効果を有する。 Further, FIG. 3 shows the axial neutron absorption capacity of the output control bank P, where the curve 6 is based on the control bank D and expresses its absorption capacity as 1.0, and the curve 7 is the axial neutron absorption capacity of the output control bank P. This is for the output control bank P used in the simulation of FIG. That is, as is clear from the figure, by using only the control rods and fully inserting the output control bank P, it is possible to respond to rapid output changes and control the output distribution, and the output distribution can be controlled safely and efficiently. It has a quick reactivity control function with little distortion and significantly improves the power control performance and reliability of pressurized water reactors. In this way, according to the present invention, a plurality of control rod assemblies inserted into a reactor core formed by a large number of nuclear fuel assemblies are divided into a control rod assembly group for power control and a control rod assembly group for power distribution control. The control rods of the control rod assembly group for power control can be freely inserted and removed over the entire height of the reactor core, and the neutron absorption capacity is uniform over the entire length, while the control rods for power distribution control The control rods of the control rod assembly group are fully inserted into the reactor core only during partial power operation, and are fully withdrawn outside of the same partial power operation, and the distribution of their neutron absorption capacity is determined from the control rods of the control rod assembly group for power control. Since it is divided into a small upper half and a lower half that is even lower than the upper half, the control rod assembly group for power distribution control can be quickly enclosed and used together with the power control rod to enable partial power operation. At the same time, it is possible to prevent bias in the power distribution due to the temperature drop of light water (occurring in the upper part of the core) during partial power operation, and furthermore, it is possible to reduce fluctuations in the power distribution when this is withdrawn and return to full power (rated) operation. It has the following effects.
以上本発明を実施例について説明したが、勿論
本発明はこのような実施例にだけ局限されるもの
ではなく、本発明の精神を逸脱しない範囲内で
種々の設計の改変を施しうるものである。 Although the present invention has been described above with reference to embodiments, it goes without saying that the present invention is not limited to such embodiments, and that various design modifications can be made without departing from the spirit of the present invention. .
第1図は制御棒の中性子吸収能力を上下軸方向
均等に設定した制御棒集合体群のみによる加圧水
型原子炉の出力制御における主要パラメータ図、
第2図は出力分布制御用制御棒集合体群を用いた
同出力制御における主要パラメータ図、第3図は
出力分布制御用制御棒集合体群の中性子吸収能力
図、第4図は加圧水型原子炉の炉心および制御棒
の構造配置図である。
A,B,C,D:制御棒集合体群(制御バン
ク)、SA,SB:制御棒集合体群(停止バンク)、
P:出力分布制御用制御棒集合体群(出力制御バ
ンク)。
Figure 1 is a diagram of the main parameters in power control of a pressurized water reactor using only a group of control rod assemblies in which the neutron absorption capacity of the control rods is set equally in the upper and lower axial directions.
Figure 2 is a diagram of the main parameters in power control using a control rod assembly group for power distribution control, Figure 3 is a neutron absorption capacity diagram of the control rod assembly group for power distribution control, and Figure 4 is a pressurized water type atom FIG. 2 is a structural layout diagram of a reactor core and control rods. A, B, C, D: Control rod assembly group (control bank), SA, SB: Control rod assembly group (stop bank),
P: Control rod assembly group for power distribution control (power control bank).
Claims (1)
内に挿入される複数の制御棒集合体を、出力制御
用制御棒集合体群と、出力分布制御用集合体群と
から構成し、前記出力制御用制御棒集合体群の制
御棒を前記炉心の全高にわたつて挿脱自在とする
と共に、その全長にわたつて中性子吸収能力を一
様とし、一方前記出力分布用制御棒集合体群の制
御棒を部分出力運転時にのみ前記炉心に全挿入さ
れ、同部分出力運転時外では全引抜とすると共に
その中性子吸収能力の分布を前記出力制御用制御
棒集合体群の制御棒より小さい上半部と同上半部
より更に低い下半部とに分けてなることを特徴と
する加圧水型原子炉。1 A plurality of control rod assemblies inserted into a reactor core formed by a large number of nuclear fuel assemblies are composed of a group of control rod assemblies for power control and a group of assemblies for power distribution control, and The control rods of the control rod assembly group for control are freely inserted and removed over the entire height of the reactor core, and the neutron absorption capacity is made uniform over the entire length, while the control rods of the control rod assembly group for power distribution are controlled. The rods are fully inserted into the core only during partial power operation, and are fully withdrawn outside of the same partial power operation, and the distribution of their neutron absorption capacity is changed to the upper half of the control rods smaller than the control rods of the control rod assembly group for power control. A pressurized water reactor characterized by being divided into a lower half that is lower than the upper half.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58070090A JPS59196497A (en) | 1983-04-22 | 1983-04-22 | pressurized water reactor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58070090A JPS59196497A (en) | 1983-04-22 | 1983-04-22 | pressurized water reactor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59196497A JPS59196497A (en) | 1984-11-07 |
| JPH0249678B2 true JPH0249678B2 (en) | 1990-10-30 |
Family
ID=13421489
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58070090A Granted JPS59196497A (en) | 1983-04-22 | 1983-04-22 | pressurized water reactor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59196497A (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE2337354C3 (en) * | 1973-07-23 | 1981-06-25 | Siemens AG, 1000 Berlin und 8000 München | Device for regulating a pressurized water reactor with adjustable control rods |
| ES449946A1 (en) * | 1975-08-14 | 1977-12-01 | Combustion Eng | Control rod and reactor |
| JPS56110092A (en) * | 1980-02-04 | 1981-09-01 | Mitsubishi Atomic Power Ind | Method of operating nuclear reactor |
-
1983
- 1983-04-22 JP JP58070090A patent/JPS59196497A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59196497A (en) | 1984-11-07 |
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