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JPH047839B2 - - Google Patents
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JPH047839B2 - - Google Patents

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Publication number
JPH047839B2
JPH047839B2 JP59265372A JP26537284A JPH047839B2 JP H047839 B2 JPH047839 B2 JP H047839B2 JP 59265372 A JP59265372 A JP 59265372A JP 26537284 A JP26537284 A JP 26537284A JP H047839 B2 JPH047839 B2 JP H047839B2
Authority
JP
Japan
Prior art keywords
control rod
output
following operation
bank
weak absorption
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
Application number
JP59265372A
Other languages
Japanese (ja)
Other versions
JPS61144598A (en
Inventor
Hiroshi Tochihara
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.)
Mitsubishi Heavy Industries Ltd
Original Assignee
Mitsubishi Atomic Power Industries Inc
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 Mitsubishi Atomic Power Industries Inc filed Critical Mitsubishi Atomic Power Industries Inc
Priority to JP59265372A priority Critical patent/JPS61144598A/en
Publication of JPS61144598A publication Critical patent/JPS61144598A/en
Publication of JPH047839B2 publication Critical patent/JPH047839B2/ja
Granted legal-status Critical Current

Links

Classifications

    • 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

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  • Jet Pumps And Other Pumps (AREA)
  • Monitoring And Testing Of Nuclear Reactors (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は原子炉に関し、特に加圧水型原子炉の
負荷追従運転方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a nuclear reactor, and more particularly to a load following operation method for a pressurized water nuclear reactor.

[従来の技術] 例えば特開昭57−119297号公報及び特開昭57−
133395号公報等に記載されているように、従来、
加圧水型原子炉の反応度制御は制御棒の挿入、引
き抜き及びほう素濃度変化によつて行つている。
制御棒による制御は速い反応度変化を行わせるこ
とができるが、炉心上部から制御棒を挿入するの
で、挿入に従い軸方向出力分布が歪んでくるとい
う問題がある。一方、ほう素濃度変化系は一次冷
却材中のほう素濃度を増減させるもので、軸方向
出力分布の問題はないが、大量の水を取り扱わな
ければならないので、反応度変化が遅いという問
題点がある。
[Prior art] For example, JP-A-57-119297 and JP-A-57-
As stated in Publication No. 133395, etc., conventionally,
Reactivity control in pressurized water reactors is performed by inserting and withdrawing control rods and changing boron concentration.
Control using control rods can quickly change the reactivity, but since the control rods are inserted from the top of the core, there is a problem that the axial power distribution becomes distorted as they are inserted. On the other hand, the boron concentration variable system increases or decreases the boron concentration in the primary coolant, and there is no problem with the axial output distribution, but the problem is that the reactivity changes slowly because a large amount of water must be handled. There is.

負荷追従運転のように、炉心の出力変動がある
場合の反応度変化について見ると、第6A図に線
1で示すような出力レベル変化があつた場合、こ
の出力レベル変化に伴う反応度変化は、第6B図
に実線2で示すような反応度変化(これは出力欠
損分という)と、点線3で示すようなキセノン
(Xe)変化による反応度変化とから成り立つてい
る。そして出力欠損は第7図に典型例を示してい
るように、燃料温度変化によるドツプラー効果の
出力欠損分、即ち図に一点鎖線4で示すものと、
一次冷却材の炉心平均温度変化による図中点線5
で示す出力欠損分との合計であり、図中実線6で
示すようになる。
Looking at the change in reactivity when there is a fluctuation in the core output, such as during load following operation, if there is a change in the output level as shown by line 1 in Figure 6A, the change in reactivity due to this change in output level is , consists of a reactivity change as shown by the solid line 2 in FIG. 6B (this is called an output deficit) and a reactivity change due to a change in xenon (Xe) as shown by the dotted line 3. As shown in a typical example in Fig. 7, the output loss is the output loss due to the Doppler effect due to fuel temperature change, that is, the output loss shown by the dashed-dotted line 4 in the figure.
Dotted line 5 in the figure due to core average temperature change of primary coolant
This is the total of the output loss shown by , and is shown by the solid line 6 in the figure.

ドツプラー効果による出力欠損分は炉心の寿命
中余り変化しないが、温度変化による出力欠損分
の方は寿命末期に近付くに従つて大きくなるの
で、全体の出力欠損は第8図に実線7で典型例を
示すように、寿命末期で大きくなつてくる。
The power loss due to the Doppler effect does not change much during the life of the reactor core, but the power loss due to temperature changes increases as it approaches the end of the life, so the overall power loss is shown as a typical example by solid line 7 in Figure 8. As shown, it becomes larger at the end of life.

従つて、出力変動中の反応度変化のうち、出力
欠損分は制御棒の挿入、引き抜きで補償すれば速
い出力変化にも対応でき、Xe変化分はゆつくり
した変化であるので、ほう素濃度変化で対応すれ
ばよいことになる。
Therefore, among the reactivity changes during output fluctuations, if the output loss is compensated for by inserting and withdrawing control rods, fast output changes can be accommodated, and the Xe changes are slow changes, so the boron concentration We need to respond with change.

しかし、100%出力から50%出力への変化では、
出力欠損は約0.7%Δρであり、一方、制御に通常
使用されている制御棒バンク即ち組分けされた特
定の制御棒グループは全挿入で約1.0〜1.4%Δρの
制御棒価値があるので、制御棒だけでこの出力欠
損分を補償しようとすると、制御棒を炉心の軸方
向より下方へ深く挿入する必要がある。このよう
に制御棒を深く挿入すると、軸方向出力分布が大
きく歪んでくることは先にも記載した通りで、そ
の後Xeによる出力分布振動等も起こつてきて問
題となる。このような軸方向出力分布の歪みを避
けるため、最近では、制御棒を余り深く挿入しな
いで出力変動を行うことが、標準的運転方法とな
つている。
However, when changing from 100% output to 50% output,
The power loss is about 0.7% Δρ, while the control rod bank or grouped specific control rod group normally used for control has a control rod value of about 1.0-1.4% Δρ with total insertion. If an attempt is made to compensate for this power loss with only the control rods, it is necessary to insert the control rods deeper into the core than in the axial direction. As mentioned above, if the control rod is inserted deeply, the axial power distribution will be greatly distorted, and then the power distribution will oscillate due to Xe, which becomes a problem. In order to avoid such distortions in the axial power distribution, it has recently become a standard operating method to perform power fluctuations without inserting the control rods too deeply.

標準的な負荷追従運転中に第6A図に線1で示
すような出力レベル変化がある場合、制御棒は第
9A図に線8で示すようにその挿入度が変化し、
これに伴い、ほう素濃度は第9B図に曲線9で示
すように、出力欠損分とXe分とが混在した複雑
な変化をする。第9C図に、上述の場合の軸方向
出力分布歪みの指標であるアキシヤルオフセツト
変化を線24で示しているが、定常値を基準とし
てほぼ一定値で制御されていることが分かる。ま
た、この例ではほう素濃度変化幅は90ppm程度も
あり、毎日このような負荷追従運転を行うとする
と、1日当たり約90ppmのほう素希釈が必要にな
る。ほう素は一次冷却材中に混入されているの
で、ほう素希釈を行うためには一次冷却材を排出
し、代わりに純水を注入することが必要になる。
運転中のほう素濃度は、寿命初期の約1000ppmか
ら寿命末期の約100ppmまで炉心の燃焼と共に単
調に減少する。このため、寿命末期近くになり、
ほう素濃度が小さくなると、ほう素希釈のために
は大量の排出水を外に出して処理することが必要
になる。即ち、排出水及び排出放射性物質が増大
するという問題が生ずる。従つて、実際の負荷追
従運転では、この排出水の処理能力の点から、寿
命末期近くでの運転が制約を受けることになる。
また寿命末期近くでは、当然単位時間当たりのほ
う素濃度希釈速度にも制約が生じてくるので、こ
の点からも、第9B図の曲線9で示すような急激
なほう素濃度変化はできないようになる。
During standard load following operation, if there is a change in the output level as shown by line 1 in Figure 6A, the control rod will change its insertion degree as shown by line 8 in Figure 9A.
As a result, the boron concentration undergoes a complex change in which the output loss and the Xe component coexist, as shown by curve 9 in FIG. 9B. In FIG. 9C, the axial offset change, which is an index of the axial output distribution distortion in the above case, is shown by a line 24, and it can be seen that it is controlled to a substantially constant value with the steady value as a reference. Furthermore, in this example, the boron concentration variation range is about 90 ppm, and if such load following operation is performed every day, boron dilution of about 90 ppm per day is required. Since boron is mixed in the primary coolant, boron dilution requires draining the primary coolant and injecting pure water in its place.
The boron concentration during operation decreases monotonically as the reactor core burns, from about 1000 ppm at the beginning of life to about 100 ppm at the end of life. For this reason, near the end of its lifespan,
As the boron concentration decreases, a large amount of waste water must be discharged and treated to dilute the boron. That is, a problem arises in that the amount of discharged water and discharged radioactive materials increases. Therefore, in actual load following operation, operation near the end of life is restricted due to the processing capacity of this waste water.
In addition, near the end of life, there are naturally restrictions on the dilution rate of boron concentration per unit time, so from this point of view as well, it is important to avoid sudden changes in boron concentration as shown by curve 9 in Figure 9B. Become.

前述のように、軸方向出力分布歪みを避けるた
めに、最近では制御棒を余り深く挿入しないで出
力変動を行うことが標準的運転方法となつてい
る。この場合、制御棒だけでは出力欠損を補償で
きないので、残りの反応度はほう素濃度変化に依
存することになり、速い出力変動ができない。ま
た、低下した出力レベルから元の全出力レベルに
即時に復帰する即時復帰能力も、第9A図から諒
解されるように制御棒が出力欠損分だけ深く挿入
されていないので、当然不足することになる。
As mentioned above, in order to avoid distortion of the axial power distribution, it has recently become a standard operating method to perform power fluctuations without inserting the control rods too deeply. In this case, since the control rod alone cannot compensate for the power loss, the remaining reactivity depends on changes in boron concentration, and rapid power fluctuations are not possible. Furthermore, as can be seen from Figure 9A, the immediate recovery ability to immediately return to the original full output level from a reduced output level is naturally insufficient because the control rods are not inserted as deep as the output loss. Become.

[発明が解決しようとする問題点] 従つて、上述の記載から諒解されるように、従
来の技術には、次ぎのような問題点があつた。
[Problems to be Solved by the Invention] Therefore, as can be understood from the above description, the conventional technology has the following problems.

軸方向出力分布の歪みを避けるために制御棒
の炉心への深い挿入ができないので、低出力レ
ベルから全出力への即時復帰能力が不足する。
Because the control rods cannot be inserted deeply into the core to avoid distortion of the axial power distribution, the ability to quickly return to full power from low power levels is lacking.

臨界ほう素濃度変化が大幅に必要とされるた
めに、寿命未期近くの臨界ほう素濃度の低い時
期では臨界濃度希釈能力が制約され、負荷追従
運転能力が制約される。
Since a significant change in the critical boron concentration is required, the critical concentration dilution ability is restricted during the period when the critical boron concentration is low near the end of the life, and the load following operation ability is restricted.

上記項のように臨界ほう素濃度変化が大き
いので、寿命を通じて排出される一次冷却材排
出水が多量となり、水処理に高コストを要す
る。
As mentioned above, since the critical boron concentration changes greatly, a large amount of primary coolant discharge water is discharged throughout the life, and water treatment requires high cost.

上記〜項の問題点により例えばステツプ
状のような速い負荷追従運転はその実施が難し
い。
Due to the problems in items 1 to 1 above, it is difficult to perform fast load following operation such as step-like operation.

特開昭57−133395号公報に記載された負荷追
従運転方法では、即時全出力復帰能力が不足す
る。また、第10A図に線10で示すように低
出力レベルから全出力レベルに戻る場合に一度
に全出力に戻れず幾つかの部分出力レベルを経
て2〜3時間後に全出力に戻る。更に、第10
C図に線12で示すように臨界ほう素濃度変化
が第9B図の線9に比べて少なくなるとはい
え、完全にゼロにすることはできず、やはり寿
命末期にはほう素濃度希釈能力が不足する。こ
れ等のことは第10A図〜第10C図に記載さ
れた典型例から容易に諒解されよう。
The load following operation method described in Japanese Unexamined Patent Publication No. 57-133395 lacks the ability to immediately return to full output. Further, as shown by line 10 in FIG. 10A, when returning from a low output level to the full output level, the output cannot be returned to the full output at once, but returns to the full output after 2 to 3 hours through several partial output levels. Furthermore, the 10th
As shown by line 12 in Figure C, although the change in critical boron concentration is smaller than that shown by line 9 in Figure 9B, it cannot be completely reduced to zero, and the ability to dilute boron concentration still decreases at the end of life. Run short. These matters will be easily understood from the typical examples shown in FIGS. 10A to 10C.

従つて、本発明の目的は、これ等の問題点を解
決して、炉心の軸方向出力分布に大きな歪みを生
じさせることなく炉心の速い出力変化及び即時復
帰能力を容易に実現すると同時に、ほう素濃度変
化に伴うほう素希釈のための排出水量を少なくす
ることができる加圧水型原子炉の負荷追従運転方
法を提供するものである。
Therefore, an object of the present invention is to solve these problems and easily realize rapid power change and immediate return capability of the reactor core without causing large distortions in the axial power distribution of the reactor core. The present invention provides a load following operation method for a pressurized water reactor that can reduce the amount of water discharged for diluting boron as the element concentration changes.

[問題点を解決するための手段及び作用] この目的から、本発明による加圧水型原子炉の
負荷追従運転方法は、炉心への制御棒挿入により
出力低下を急速に行い、その後のキセノン増加に
よる反応度減少は制御棒を引き抜いて補償し、制
御棒が約20〜25%挿入程度に達し軸方向偏差が全
出力の定常値より約5〜10%負側に達した後は該
制御棒はその位置に保持し、弱吸収制御棒バンク
引き抜きにより制御を行い、その後の出力上昇に
あたつては制御棒引き抜き及び弱吸収制御棒バン
クの順次引き抜きによりステツプ状に全出力へ出
力上昇させ、出力上昇後のキセノン減少による反
応度増加を弱吸収制御棒バンクの再挿入により補
償することを特徴とするものである。
[Means and effects for solving the problem] For this purpose, the load following operation method of a pressurized water reactor according to the present invention rapidly reduces the output by inserting control rods into the reactor core, and then reduces the reaction due to the subsequent increase in xenon. The reduction in power is compensated for by withdrawing the control rod, and after the control rod has been inserted about 20 to 25% and the axial deviation has reached about 5 to 10% negative than the steady value of the full output, the control rod It is held in position and controlled by pulling out the weak absorption control rod bank, and after that, when increasing the output, the output is increased to full output in steps by pulling out the control rod and the weak absorption control rod bank sequentially, and the output is increased. This is characterized by compensating for the subsequent increase in reactivity due to the decrease in xenon by reinserting the weakly absorbing control rod bank.

加圧水型原子炉をこのように負荷追従運転する
ことにより、炉心の軸方向出力分布に大きな歪み
を生じさせることなく炉心の速い出力変化及び即
時復帰能力を容易に実現すると同時に、ほう素濃
度変化に伴うほう素希釈のための排出水量を少な
くすることができる。
Load-following operation of a pressurized water reactor in this way makes it possible to easily achieve rapid power changes and immediate recovery capabilities of the core without causing large distortions in the axial power distribution of the core, and at the same time, it is possible to easily realize rapid power changes and immediate recovery capabilities of the core without causing large distortions in the axial power distribution of the core. The amount of water discharged for boron dilution can be reduced.

[実施例] 次に、本発明の好適な実施例について添付図面
を参照して詳細に説明するが、図中、同一符号は
同一又は対応部分を示すものとする。
[Embodiments] Next, preferred embodiments of the present invention will be described in detail with reference to the accompanying drawings, in which the same reference numerals indicate the same or corresponding parts.

本発明は、特開昭57−133395号公報記載の負荷
追従運転方法に加えて、中性子の弱吸収材からな
る制御棒を使用することにより、寿命初期から寿
命末期までの全期間を通じて低出力レベルから全
出力への即時復帰能力があると共に、水排出量の
大幅な低減を可能にする理想的な負荷追従運転方
法を提供するものである。
In addition to the load following operation method described in JP-A-57-133395, the present invention uses control rods made of a weak neutron absorber to achieve low output levels throughout the entire period from the beginning of life to the end of life. This provides an ideal load-following operation method that has the ability to immediately return to full output from 100 to 100 kW, and enables a significant reduction in water discharge.

前記特開昭57−133395号公報記載の方法では、
出力低下は制御棒挿入で即時に行うが、出力低下
後のキセノン濃度変化分を制御棒引き抜きで補償
するために、制御棒は次第に引き抜かれて行き、
全出力に復帰しようとして制御棒を全引き抜きに
しても、反応度的に不足することになり、完全な
即時全出力復帰能力がない。
In the method described in JP-A-57-133395,
The power reduction occurs immediately by inserting the control rod, but in order to compensate for the change in xenon concentration after the power reduction by withdrawing the control rod, the control rod is gradually withdrawn.
Even if the control rods were fully withdrawn in an attempt to return to full power, the reactivity would be insufficient, and there would be no ability to immediately return to full power.

これを解決するためには、予め全出力レベルに
おいて出力欠損分に相当するだけの反応度効果を
有する特別の制御棒を炉心に挿入しておき、全出
力レベルへの復帰の場合には、この制御棒を引き
抜くという方法が考えられる。ただし、全出力レ
ベルで炉心に全挿入するわけであるから、制御棒
反応度価値の余り大きいものは挿入とともに半径
方向及び軸方向出力分布が大きく歪むために採用
が難しい。従つて、このような目的に使用する制
御棒としては、中性子の弱吸収材棒(例えば、ス
テンレス鋼、インコネル等)で構成された制御棒
クラスタ集合体が望まれる。
To solve this problem, special control rods with reactivity effects equivalent to the power loss at full power level are inserted into the core in advance, and when returning to full power level, these control rods are inserted into the reactor core. One possible method is to pull out the control rod. However, since the control rods are fully inserted into the core at full power level, control rods with extremely high reactivity values are difficult to employ because the radial and axial power distributions will be greatly distorted as they are inserted. Therefore, as a control rod used for such a purpose, a control rod cluster assembly composed of rods of a weak neutron absorber (for example, stainless steel, Inconel, etc.) is desired.

即ち、使用しうる弱吸収制御棒クラスタは第1
図に示した通りであり、第1図の線A−Aに沿つ
た断面を第2図に示すように、弱吸収制御棒クラ
スタ13を構成する複数の弱吸収制御棒ピン材と
しては、ステンレス鋼中実棒13aを使用するこ
とができる。また、第2A図に示すように、ステ
ンレス鋼中実棒13aと、中性子吸収の強いAg
−In−Cd棒13bとを混在させた弱吸収制御棒
クラスタ13を使用してもよい。更に、第2図及
び第2A図のステンレス鋼中実棒13aに代え
て、第2B図に示すような、内側にアルミナ、ジ
ルコニア等のような中性子弱吸収材13cを充填
した中空のステンレス鋼管13dを使用すること
もできる。また、第2図のステンレス鋼棒13a
の代わりにインコネル棒を使用したり、第2A図
に示すAg−In−Cd棒13bの代わりにHf棒、
B4C棒等を用いることも可能である。
In other words, the weakly absorbing control rod cluster that can be used is the first one.
As shown in the figure, and as shown in FIG. 2, a cross section taken along the line A-A in FIG. A solid steel rod 13a can be used. In addition, as shown in FIG. 2A, a stainless steel solid rod 13a and Ag with strong neutron absorption are used.
A weak absorption control rod cluster 13 in which -In-Cd rods 13b are mixed may also be used. Furthermore, instead of the solid stainless steel rod 13a shown in FIGS. 2 and 2A, a hollow stainless steel tube 13d filled with a weak neutron absorber 13c such as alumina or zirconia inside is used as shown in FIG. 2B. You can also use In addition, the stainless steel rod 13a in FIG.
An Inconel rod may be used instead of , or an Hf rod may be used instead of the Ag-In-Cd rod 13b shown in Fig. 2A.
It is also possible to use a B 4 C rod or the like.

第3図は弱吸収制御棒の配置例を示す炉心平面
図で、図中、例えば符号Gで示す位置に配置され
た弱吸収制御棒13は20体設けられている。組分
けされた特定の制御棒グループは一般にバンクと
呼ばれているが、第3図の配置例では、各バンク
4体の弱吸収制御棒クラスタからなるG1〜G5
5バンクに分けられている。尚、A,BC及びD
は制御バンク、Sa,Sb,Se及びSdは停止バンク
である。
FIG. 3 is a core plan view showing an example of the arrangement of weak absorption control rods. In the figure, for example, 20 weak absorption control rods 13 are arranged at positions indicated by the symbol G. A specific group of control rods is generally called a bank, but in the arrangement example shown in Figure 3, each bank is divided into five banks, G1 to G5 , each consisting of four weakly absorbing control rod clusters. ing. Furthermore, A, BC and D
is the control bank, and Sa, Sb, Se and Sd are the stop banks.

第1図に示すようなステンレス鋼等からなる弱
吸収制御棒クラスタ13を全出力レベルにおいて
出力変動が予定される出力欠損分に相当する体数
だけ臨界ほう素濃度希釈により全挿入しておけ
ば、低出力レベルから即時全出力に復帰するため
には、これ等の弱吸収制御棒クラスタを全引き抜
きすることにより、臨界ほう素濃度変化なしに即
時に対応することができる。必要な出力欠損分の
反応度は、第7図の線6及び第8図の線7で示す
ように100%→50%の出力変化では約0.7%Δρ〜
1.0%Δρであるが、特開昭57−133395号公報に開
示された方法では、制御棒が低出力レベルで完全
に引き抜けるわけではなく、少なくとも約20〜50
%は炉心に挿入されているために、この制御棒引
き抜きによる出力上昇分を利用できることを考え
ると、弱吸収制御棒の反応度は約0.5%Δρ〜1.0%
Δρが望ましいことになる。その理由は、0.5%Δρ
より小さい反応度価値であると、補償すべき出力
欠損分に不足することが問題となり、1.0%Δρよ
り大きい反応度価値であると、多数の弱吸収制御
棒バンクが必要となり、その駆動装置も含めて建
設コスト的に不利になるからである。これだけの
反応度効果を有する弱吸収制御棒が一度に挿入さ
れると出力分布の歪みが生ずるので、通常は4〜
5バンクに分けて各バンク当たりの反応度効果を
薄めるということにしている。また、多数のバン
クに分けると臨界ほう素濃度の微調整用に利用す
る上でも有利である。
If the number of weak absorption control rod clusters 13 made of stainless steel or the like shown in Fig. 1 is fully inserted by diluting the critical boron concentration at all output levels, the number corresponds to the expected output deficit due to output fluctuation. In order to immediately return to full power from a low power level, it is possible to respond immediately without changing the critical boron concentration by fully withdrawing these weakly absorbing control rod clusters. The reactivity for the necessary output loss is approximately 0.7% Δρ for a change in output from 100% to 50%, as shown by line 6 in Figure 7 and line 7 in Figure 8.
However, in the method disclosed in Japanese Patent Application Laid-Open No. 57-133395, the control rod cannot be completely withdrawn at a low output level, and at least about 20 to 50%
% is inserted into the reactor core, and considering that the power increase due to control rod withdrawal can be utilized, the reactivity of the weakly absorbing control rods is approximately 0.5% Δρ ~ 1.0%
It follows that Δρ is desirable. The reason is 0.5%Δρ
If the reactivity value is smaller, there will be a problem of insufficient power loss to compensate, and if the reactivity value is larger than 1.0%Δρ, a large number of weak absorption control rod banks will be required, and their drive equipment will also be required. This is because it would be disadvantageous in terms of construction costs. If weak absorption control rods with such a reactivity effect are inserted all at once, the output distribution will be distorted, so normally 4~
We decided to divide it into 5 banks and dilute the reactivity effect for each bank. Furthermore, dividing into a large number of banks is advantageous for use in finely adjusting the critical boron concentration.

制御棒バンク及び弱吸収制御棒バンクの引き抜
きにより低出力レベルから全出力に復帰した後
は、キセノン濃度の減少分の反応度は弱吸収制御
棒バンクを順次挿入して行くことによつて補償す
ることができる。50%出力レベルから100%出力
レベルへの復帰後のキセノン濃度変化の反応度は
0.8%Δρ程度であるので、弱吸収制御棒を全数全
挿入することによつて補償することができる。こ
のように負荷追従運転中の全反応変化は制御棒バ
ンクと弱吸収制御棒バンクとで殆ど賄うことがで
きるので臨界ほう素濃度変化を殆ど必要とせずに
各種の負荷追従運転を行うことができる。
After returning from a low power level to full power by withdrawing the control rod bank and the weak absorption control rod bank, the reactivity due to the decrease in xenon concentration is compensated for by sequentially inserting the weak absorption control rod banks. be able to. The reactivity of xenon concentration change after returning from 50% output level to 100% output level is
Since it is about 0.8%Δρ, it can be compensated by fully inserting all weak absorption control rods. In this way, most of the total reaction changes during load following operation can be covered by the control rod bank and the weak absorption control rod bank, so various load following operations can be performed with little need for changes in critical boron concentration. .

第4図は制御棒挿入による出力分布の軸方向偏
差の変化例を示す図であり、それぞれ線14は全
5バンクの弱吸収制御棒、線15は弱吸収制御棒
1バンク、線23はバンク間にオーバーラツプが
ある従来の全長制御棒の挿入例を示している。弱
吸収制御棒バンクは、各バンク間のオーバーラツ
プなしに単独で炉心に挿入されるので、全バンク
を一括して挿入しても、線14に示すように全挿
入後は軸方向出力分布は歪まない。歪みの指標で
ある軸方向偏差AOは、qT,qBをそれぞれ炉心
上半分及び下半分の出力とすると、 AO=qT−qB/qT+qB×100% で定義される。
FIG. 4 is a diagram showing an example of a change in the axial deviation of the power distribution due to control rod insertion, in which line 14 represents all five banks of weak absorption control rods, line 15 represents one bank of weak absorption control rods, and line 23 represents a bank of weak absorption control rods. An example of conventional full-length control rod insertion with overlap in between is shown. The weakly absorbing control rod banks are inserted into the core individually without overlap between each bank, so even if all banks are inserted at once, the axial power distribution will be distorted after all insertions, as shown by line 14. do not have. The axial deviation AO, which is an index of strain, is defined as AO = qT - qB / qT + qB x 100%, where qT and qB are the outputs of the upper and lower half of the core, respectively.

この軸方向偏差AOは、弱吸収制御棒挿入後は
殆ど変化しないこと及び実際は1バンクずつ順次
挿入して行くため線15で示すように挿入中の
AO変化も小さいので、弱吸収制御棒挿入による
出力分布の変動は殆ど問題にならない。従つて、
出力分布歪みを気にせずに必要に応じて弱吸収制
御棒バンクを挿入、引き抜きして反応度を微調整
することができる。
This axial deviation AO hardly changes after the weak absorption control rod is inserted, and in reality, it is inserted one bank at a time, so the deviation AO during insertion is as shown by line 15.
Since the AO change is also small, fluctuations in the power distribution due to the insertion of weak absorption control rods are hardly a problem. Therefore,
The reactivity can be finely adjusted by inserting and withdrawing the weak absorption control rod bank as needed without worrying about power distribution distortion.

弱吸収制御棒を第3図のように配置した場合の
負荷追従運転方法においては、第5A図〜第5D
図に例示するように、第5A図に線16で示す非
常に早い負荷変化(5%出力/分)且つ第5C図
の線17で示すように殆どゼロの臨界ほう素濃度
変化で、負荷追従運転を行うことができる。第5
B図では、点線18は弱吸収制御棒バンクの挿入
度を、実線19は制御棒バンクの挿入度を示して
いる。また、制御棒バンク及び弱吸収制御棒バン
クの引き抜きによつて、第5B図の区間20で示
す低出力レベルからの即時全出力復帰能力も完全
にあることが分かる。更に、全出力状態で若干の
制御棒バンク挿入を行えば、完全に第5C図の線
17の臨界ほう素濃度変化をゼロとすることも可
能である。また、第5D図に線25で示すアキシ
ヤルオフセツト変化は、出力低下時の制御棒挿入
及びその後の引き抜きにより定常値より約5〜10
%負側に維持されており、その後出力上昇した後
のアキシヤルオフセツトはほぼ一定値に制御され
ることが分かる。
In the load following operation method when the weak absorption control rods are arranged as shown in Fig. 3, Figs. 5A to 5D
As illustrated in the figure, load tracking is achieved with very fast load changes (5% output/min) as shown by line 16 in Fig. 5A and with almost zero critical boron concentration changes as shown by line 17 in Fig. 5C. Able to drive. Fifth
In Figure B, the dotted line 18 indicates the degree of insertion of the weakly absorbing control rod bank, and the solid line 19 indicates the degree of insertion of the control rod bank. It can also be seen that by withdrawal of the control rod bank and the weak absorbing control rod bank, there is complete ability to immediately return to full power from the low power level shown in section 20 of FIG. 5B. Furthermore, by slightly inserting a control rod bank under full power conditions, it is possible to completely reduce the critical boron concentration change shown by line 17 in FIG. 5C to zero. In addition, the axial offset change shown by line 25 in Figure 5D is about 5 to 10% lower than the steady value due to control rod insertion and subsequent withdrawal during power reduction.
It can be seen that the axial offset is maintained on the negative side, and after the output increases thereafter, the axial offset is controlled to a substantially constant value.

[発明の効果] 以上のように、本発明によれば、弱吸収制御棒
バンクを使用するので、特開昭57−133395号公報
記載の方法に比べて、下記のように優れた理想的
な負荷追従運転を行うことが可能である。
[Effects of the Invention] As described above, according to the present invention, since a weak absorption control rod bank is used, compared to the method described in JP-A-57-133395, it is possible to achieve the ideal ideal It is possible to perform load following operation.

5%出力/分程度の速い負荷変化からもつと
ゆつくりした負荷変化まで各種の負荷変化パタ
ーンに対応できる。
It can handle various load change patterns, from fast load changes of about 5% output/minute to slow load changes.

ほぼ寿命末期まで完全な即時全出力復帰能力
のある負荷追従運転ができる。
Capable of load following operation with complete instantaneous full output return capability until almost the end of life.

ほぼ寿命末期まで臨界ほう素濃度変化がほぼ
ゼロとなる負荷追従運転ができるので、排出水
量はその処理が殆んど問題にならない程激減す
る。
Since it is possible to perform load-following operation in which the change in critical boron concentration is almost zero until almost the end of its life, the amount of discharged water is reduced so drastically that its treatment becomes almost no problem.

出力分布歪みの少ない安定した負荷追従運転
が可能である。
Stable load following operation with little output distribution distortion is possible.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明の負荷追従運転方法において使
用しうる弱吸収制御棒クラスタの構造例を示す側
面図、第2図は第1図のA−A線断面図、第2A
図は別の弱吸収制御棒クラスタの第2図に相当す
る断面図、第2B図は弱吸収制御棒の変形例を示
す断面図、第3図は原子炉炉心におけ弱吸収制御
棒クラスタの配置例を示す平面図、第4図は制御
棒挿入による軸方向偏差の変形例を示す図、第5
A図は本発明の負荷追従運転例における出力レベ
ルの変化を示す図、第5B図は本発明の負荷追従
運転例における制御棒挿入度の変化を示す図、第
5C図は本発明の負荷追従運転例におけるほう素
濃度変化を示す図、第5D図は本発明の負荷追従
運転例におけるアキシヤルオフセツト変化を示す
図、第6A図は従来の負荷追従運転における出力
レベルの時間に伴う変化例を示す図、第6B図は
第6A図の出力レベル変化に伴う反応度変化を示
す図、第7図は出力レベルに対する出力欠損の関
係を示す図、第8図は炉心寿命に対する出力欠損
の関係を示す図、第9A図は従来の負荷追従運転
中の時間対制御棒挿入度の関係を示す図、第9B
図は従来の負荷追従運転中の時間対ほう素濃度変
化の関係を示す図、第9C図は従来の負荷追従運
転中の時間対アキシヤルオフセツト変化の関係を
示す図、第10A図、第10B図及び第10C図
は従来の負荷追従運転方法による場合の出力レベ
ル、制御棒挿入度及びほう素濃度変化をそれぞれ
示す図である。 13…弱吸収制御棒クラスタ、13a,13b
及び13c…弱吸収制御棒。
Fig. 1 is a side view showing a structural example of a weak absorption control rod cluster that can be used in the load following operation method of the present invention, Fig. 2 is a sectional view taken along line A-A in Fig. 1,
The figure is a cross-sectional view corresponding to FIG. 2 of another weak-absorbing control rod cluster, FIG. 2B is a cross-sectional view showing a modification of the weak-absorbing control rod, and FIG. Fig. 4 is a plan view showing an example of arrangement; Fig. 4 is a drawing showing a modification of axial deviation due to control rod insertion;
Figure A is a diagram showing changes in the output level in an example of load following operation of the present invention, Figure 5B is a diagram showing changes in control rod insertion degree in an example of load following operation of the present invention, and Figure 5C is a diagram showing changes in the degree of control rod insertion in an example of load following operation of the present invention. FIG. 5D is a diagram showing changes in boron concentration in an example of operation, FIG. 5D is a diagram showing changes in axial offset in an example of load following operation of the present invention, and FIG. 6A is an example of change in output level over time in conventional load following operation. Figure 6B is a diagram showing the change in reactivity due to the change in power level in Figure 6A, Figure 7 is a diagram showing the relationship of power loss to power level, and Figure 8 is a diagram showing the relationship of power loss to core life. Figure 9A is a diagram showing the relationship between time and control rod insertion degree during conventional load following operation, Figure 9B
9C is a diagram showing the relationship between time and axial offset change during conventional load following operation. FIG. 9C is a diagram showing the relationship between time and axial offset change during conventional load following operation. Figures 10B and 10C are diagrams showing the output level, control rod insertion degree, and boron concentration changes, respectively, when using the conventional load following operation method. 13... Weak absorption control rod cluster, 13a, 13b
and 13c...weak absorption control rod.

Claims (1)

【特許請求の範囲】 1 炉心への制御棒挿入により出力低下を急速に
行い、その後のキセノン増加による反応度減少は
制御棒を引き抜いて補償し、制御棒が約20〜25%
挿入程度に達し軸方向偏差が全出力の定常値より
約5〜10%負側に達した後は該制御棒はその位置
に保持し、弱吸収制御棒バンク引き抜きにより制
御を行い、その後の出力上昇にあたつては制御棒
引き抜き及び弱吸収制御棒バンクの順次引き抜き
によりステツプ状に全出力へ出力上昇させ、出力
上昇後のキセノン減少による反応度増加を弱吸収
制御棒バンクの再挿入により補償することを特徴
とする加圧水型原子炉の負荷追従運転方法。 2 前記弱吸収制御棒クラスタ全バンクの反応度
価値は0.5%Δρ〜1.0%Δρであることを特徴とす
る特許請求の範囲第1項記載の加圧水型原子炉の
負荷追従運転方法。
[Claims] 1. The power is rapidly reduced by inserting the control rods into the reactor core, and the subsequent decrease in reactivity due to the increase in xenon is compensated for by withdrawing the control rods.
After the control rod reaches the insertion level and the axial deviation reaches about 5 to 10% negative than the steady value of the full output, the control rod is held in that position and control is performed by withdrawing the weak absorption control rod bank, and the subsequent output is During the ascent, the output is increased to full output in steps by withdrawing the control rods and the weak absorption control rod bank in sequence, and the increase in reactivity due to the decrease in xenon after the increase in output is compensated for by reinserting the weak absorption control rod bank. A load following operation method for a pressurized water reactor, characterized by: 2. The load following operation method for a pressurized water reactor according to claim 1, wherein the reactivity value of all banks of the weak absorption control rod cluster is 0.5% Δρ to 1.0% Δρ.
JP59265372A 1984-12-18 1984-12-18 Load follow-up operation method of pressurized water type reactor Granted JPS61144598A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59265372A JPS61144598A (en) 1984-12-18 1984-12-18 Load follow-up operation method of pressurized water type reactor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59265372A JPS61144598A (en) 1984-12-18 1984-12-18 Load follow-up operation method of pressurized water type reactor

Publications (2)

Publication Number Publication Date
JPS61144598A JPS61144598A (en) 1986-07-02
JPH047839B2 true JPH047839B2 (en) 1992-02-13

Family

ID=17416262

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59265372A Granted JPS61144598A (en) 1984-12-18 1984-12-18 Load follow-up operation method of pressurized water type reactor

Country Status (1)

Country Link
JP (1) JPS61144598A (en)

Also Published As

Publication number Publication date
JPS61144598A (en) 1986-07-02

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