JPH0445796B2 - - Google Patents
Info
- Publication number
- JPH0445796B2 JPH0445796B2 JP58212098A JP21209883A JPH0445796B2 JP H0445796 B2 JPH0445796 B2 JP H0445796B2 JP 58212098 A JP58212098 A JP 58212098A JP 21209883 A JP21209883 A JP 21209883A JP H0445796 B2 JPH0445796 B2 JP H0445796B2
- Authority
- JP
- Japan
- Prior art keywords
- control rod
- core
- flow rate
- pattern
- control
- 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
-
- 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)
- Control Of Turbines (AREA)
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は沸騰水型原子炉(BWR)の起動法に
係り、特に制御棒の操作と炉心流量の調整とを併
用する出力上昇法における出力上昇時間を短縮す
るに適したBWRの起動法に関する。[Detailed Description of the Invention] [Field of Application of the Invention] The present invention relates to a method for starting up a boiling water reactor (BWR), and in particular to a method for increasing power in a power increasing method that combines control rod manipulation and core flow rate adjustment. Concerning a BWR startup method suitable for shortening time.
BWRの運転には、燃料健全性維持の観点か
ら、出力上昇時に燃料棒出力の急上昇を避け所謂
「ならし運転」を行うPCIOMR運転が実施されて
いる。PCIOMRは、出力の急上昇を避けるため、
制御棒操作による燃料線出力密度上昇のしきい値
(PCR)、およびそれに達した後の燃料線出力密度
の単位時間当りの変化率(P〓)を規定したもので
ある。
In BWR operation, from the perspective of maintaining fuel integrity, PCIOMR operation is carried out in which a so-called "breaking-in operation" is performed to avoid sudden increases in fuel rod output when output increases. PCIOMR is designed to avoid sudden spikes in output.
It stipulates the threshold value (P CR ) of increase in fuel line power density due to control rod operation and the rate of change in fuel line power density per unit time (P〓) after reaching this threshold.
ならし運転を行うPCIOMR運転は燃料健全性
維持には有効な運転法であるが、出力上昇にかな
り長時間を要し、原子炉の負荷率を若干低下させ
る嫌いがある。すなわち、BWRにおいてはボイ
ド分布が軸方向に生じるために出力分布が下方に
偏る傾向があり、その結果、原子炉起動時に燃料
線出力密度の上記しきい値PCRとなる炉心出力が
低い値に抑えられ、またそれからの出力上昇率P〓
も規定されていることから、出力上昇にかなり長
時間を要していた。 PCIOMR operation, which performs a break-in operation, is an effective operation method for maintaining fuel integrity, but it takes a considerable amount of time to increase output and has the disadvantage of slightly lowering the reactor load factor. In other words, in BWR, the void distribution occurs in the axial direction, so the power distribution tends to be biased downward, and as a result, the core power that reaches the above threshold P CR of the fuel line power density at reactor startup becomes a low value. The output increase rate P〓
Because of this, it took a considerable amount of time to increase the output.
近年このようなボイド分布特性を考慮して、燃
料集合体の上下領域に反応度の高低をつけて出力
分布を平坦化する改良燃料が提案された(特開昭
53−40188「燃料集合体」)。この改良燃料の採用に
より、通常出力運転時には浅挿入制御棒による出
力分布調整が不要になり、深挿入制御棒のみによ
り熱的に余裕のある運転が可能になつた。 In recent years, in consideration of such void distribution characteristics, improved fuels have been proposed that flatten the power distribution by creating high and low reactivity levels in the upper and lower regions of the fuel assembly (Japanese Patent Laid-Open Publication No.
53-40188 "Fuel assembly"). Adoption of this improved fuel eliminates the need for power distribution adjustment using shallowly inserted control rods during normal output operation, and allows operation with thermal margins using only deeply inserted control rods.
しかし、起動時の出力上昇中の低出力状態では
ゼノン(Xe)の蓄積量が十分でなく、また炉心
流量に対して炉心出力が相対的に高いためボイド
分布の影響で出力分布が下方に膨む効果が大きい
ので、従来、浅挿入制御棒を多く使つたり、又は
低出力において制御棒操作を中止し炉心流量の調
整のみで出力を上昇させてゼノンの蓄積を促進さ
せ、然る後再び制御棒を操作するという過程を何
回か繰返すこと(所謂ならし運転)を行なつて所
定出力に到達するという手順が採用されている。 However, in the low power state during the power increase at startup, the amount of xenon (Xe) accumulated is not sufficient, and the core power is relatively high compared to the core flow rate, so the power distribution expands downward due to the effect of the void distribution. Conventionally, the accumulation of Zenon is promoted by using many shallowly inserted control rods, or by stopping control rod operation at low power and increasing the power only by adjusting the core flow rate. A procedure is adopted in which the process of operating the control rods is repeated several times (so-called break-in operation) to reach a predetermined output.
換言すれば、制御棒操作による燃料線出力密度
をしきい値PCR以下に抑えるための配慮から出力
上昇時の制御棒操作は強制循環による最低炉心流
量で行うのが通常であり、したがつて炉心流量に
対し炉心出力が相対的に高くなつて出力分布が下
方膨みとなる状態が生じているので、従来、これ
を吸収するために、定格到達目標制御棒パターン
を構成するに先立ち、所謂ならし運転を十分に行
う必要があつた。 In other words, in order to keep the fuel line power density due to control rod operation below the threshold P CR , control rod operation when power increases is usually performed at the lowest core flow rate due to forced circulation. Since the core power is relatively high compared to the core flow rate, resulting in a downward bulge in the power distribution, conventionally, in order to compensate for this, prior to configuring the target control rod pattern to achieve the rating, so-called It was necessary to perform a sufficient break-in operation.
このため操作が煩雑になると共に、起動時の出
力上昇にかなりの日数を要していた。 This made the operation complicated and required a considerable number of days to increase the output at startup.
〔発明の目的〕
本発明の目的は、上記従来の起動法の欠点に鑑
み、炉心流量に対して炉心出力が相対的に高い領
域で炉心出力分布の下方膨みを避け、出力上昇時
間を短縮し得るBWRの起動法を提供することに
ある。[Object of the Invention] In view of the above drawbacks of the conventional startup method, the object of the present invention is to avoid the downward expansion of the core power distribution in the region where the core power is relatively high relative to the core flow rate, and shorten the power rise time. The objective is to provide a method for starting BWR that can be used.
BWRの起動においては一般に核分裂生成物で
ある。ゼノン(Xe)がないので、これを炉心の
適所にできるだけ早く蓄積する必要があるゼノン
は第1図に示すように出力を高くするほど早く蓄
積する特性があるから、その蓄積を早めるには出
力をできるだけ早く高める必要がある。
Fission products are commonly used in BWR startups. Since there is no xeno (Xe), it is necessary to accumulate it in the appropriate place in the core as quickly as possible. need to be increased as soon as possible.
しかしBWRでは、一般に制御棒は炉心上方か
ら下方へ引抜かれるので、その引抜に伴つて出力
分布のピークも炉心下方へ移動する傾向があり、
しかも起動時には前述の如く一般に強制循環によ
る最低炉心流量状態で制御棒の引抜操作が行われ
るから、炉心流量に対して炉心出力が相対的に高
くなり、ボイド分布の影響で炉心出力分布はより
下方に膨むことになる。 However, in a BWR, the control rods are generally withdrawn from above the core to below, so the peak of the power distribution also tends to move downwards as the control rods are withdrawn.
Moreover, at startup, the control rod withdrawal operation is generally performed in the lowest core flow rate state due to forced circulation as described above, so the core power becomes relatively high relative to the core flow rate, and the core power distribution becomes more downward due to the effect of the void distribution. It will expand to.
上記の点に鑑み、本発明によるBWRの起動法
は、定格到達目標制御棒パターン中で全引抜であ
る最外周制御棒またはそれに隣接する制御棒のう
ち複数本は全挿入とし、且つ最外周およびそれに
隣接する制御棒以外の制御棒のうち定格到達目標
制御棒パターン中で全引抜でない制御棒は定格到
達目標制御棒パターンにおけるのと同じ又はその
近傍の引抜位置とした制御棒パターンを中間制御
棒パターンに採り、出力上昇時に、先ず、該中間
制御パターンを形成する制御棒操作により、強制
循環での最低炉心流量もしくはその近傍の炉心流
量にて、炉心出力を規定の燃料線出力密度のしき
い値に達する炉心出力まで上昇させて、該炉心出
力まで上昇した時点で上記中間制御棒パターンを
完成し、該中間制御棒パターンの完成以後は、制
御棒パターンを固定したままで炉心流量の増加操
作のみで炉心出力を更に上昇させる過程と、それ
に次いで炉心流量を固定したままで定格到達目標
制御棒パターンへ向けて制御棒引抜操作のみで規
定の燃料線出力密度変化率の制限値を遵守しなが
ら炉心出力を更に上昇させる過程とを経て、定格
到達目標制御パターンを完成することを特徴とす
るものである。 In view of the above points, the BWR startup method according to the present invention is to fully insert the outermost control rod or adjacent control rods that are fully withdrawn in the rated target control rod pattern, and to fully insert the outermost and adjacent control rods. Among the control rods other than the adjacent control rods, control rods that are not fully withdrawn in the rated target control rod pattern are set to intermediate control rod patterns with the same or nearby withdrawal position as in the rated target control rod pattern. When a pattern is adopted and the output is increased, first, by operating the control rods that form the intermediate control pattern, the core output is brought to the threshold of the specified fuel line power density at the minimum core flow rate in forced circulation or the core flow rate in the vicinity. The intermediate control rod pattern is completed at the point when the core output reaches the specified value, and after the completion of the intermediate control rod pattern, the core flow rate is increased while the control rod pattern remains fixed. Then, while keeping the core flow rate fixed, the control rod pattern is moved towards the target control rod pattern to reach the rating, while observing the specified fuel line power density change rate limit value only by withdrawing the control rods. This method is characterized in that the target control pattern for reaching the rated rating is completed through the process of further increasing the core power.
〔発明の実施例〕
以下、本発明のBWR起動法の一実施例を説明
する。[Embodiment of the Invention] An embodiment of the BWR starting method of the present invention will be described below.
第2図aおよびbは本実施例における定格到達
目標制御棒パターンおよび中間制御棒パターンを
夫々示す。図中に記入された数字は、制御棒の全
ストロークを48としたとき、そこの制御棒がそ
の数字に相当するストロークだけ全挿入位置から
引抜かれていること、例えば数字10は全挿入から
10/48ストロークだけ引抜かれていることを表わ
しており、数字0は全挿入、ブランクは全引抜を
表わしている。全引抜は数字48で表わされるが、
図示の簡素化のためブランクで表わした。 FIGS. 2a and 2b show the rated target control rod pattern and intermediate control rod pattern, respectively, in this embodiment. The numbers written in the diagram indicate that when the total stroke of the control rod is 48, the control rod has been pulled out from the fully inserted position by the stroke corresponding to that number. For example, the number 10 indicates that the control rod has been pulled out from the fully inserted position by The number 0 represents full insertion and the blank represents full removal. Total withdrawal is represented by the number 48,
It is shown as a blank to simplify the illustration.
第2図aのように、定格到達目標制御棒パター
ンにおいては、最外周およびそれに隣接する制御
棒は全引抜であり、それ以外の制御棒のうち複数
本(対称的配置にある)が全引抜でなく他は全引
抜である。また、同図bのように、中間制御棒パ
ターンにおいては、最外周又はそれに隣接する制
御棒のうちの複数本(対称的配置にある)は全挿
入とされ、最外周およびそれに隣接する制御棒以
外の制御棒のうち定格到達目標パターン中で全引
抜でない前記の複数本は定格到達目標制御パター
ンにおけるその引抜位置と同じ引抜位置にあり、
他は定格到達目標制御棒パターンと同様に全引抜
である。 As shown in Figure 2a, in the rated target control rod pattern, the outermost control rods and adjacent control rods are fully withdrawn, and several other control rods (in a symmetrical arrangement) are fully withdrawn. However, the others are completely removed. In addition, as shown in Figure b, in the intermediate control rod pattern, multiple control rods (in a symmetrical arrangement) at or adjacent to the outermost periphery are fully inserted; Among the other control rods, the plurality of control rods that are not fully withdrawn in the rated target control pattern are at the same extraction position as in the rated target control pattern,
The other control rods are fully withdrawn, similar to the rated target control rod pattern.
比較のため、定格到達目標制御パターンを本実
施例のそれと同じくする従来例において採用され
る中間制御棒パターンを第3図に示す。本発明実
施例の中間制御棒パターン(第2図b)と従来例
のそれ(第3図)との本質的相違の一つは、前者
では最外周及びそれに隣接する制御棒以外の制御
棒のうちの複数本が定格到達目標制御棒パターン
と同じ引抜位置にあるのに対して、後者ではそれ
らが全挿入となつている点にある。 For comparison, FIG. 3 shows an intermediate control rod pattern employed in a conventional example in which the rated target control pattern is the same as that of this embodiment. One of the essential differences between the intermediate control rod pattern of the embodiment of the present invention (Fig. 2b) and that of the conventional example (Fig. 3) is that in the former, control rods other than the outermost control rod and adjacent control rods are The difference is that several of these control rods are in the same extraction position as the rated target control rod pattern, whereas in the latter they are fully inserted.
第4図は起動時の出力上昇の時間経過を示した
グラフ、第5図はこれを炉心流量と炉心出力との
関係で示したグラフ(炉心流量−炉心出力マツ
プ)である。第5図中、7は強制循環による最低
炉心流量(定格の約20%)ライン、8は強制循環
により炉心流量45%を与えるライン、9は
APRMロツドブロツクライン(制御棒の引抜禁
止限界ライン)、10は100%炉心流量制御ライ
ン、11は強制循環特性による最低出力ラインを
表わしている。 FIG. 4 is a graph showing the time course of the power increase at startup, and FIG. 5 is a graph showing this in terms of the relationship between core flow rate and core output (core flow rate - core output map). In Figure 5, 7 is the minimum core flow rate (approximately 20% of the rated value) line due to forced circulation, 8 is the line that provides 45% core flow rate due to forced circulation, and 9 is the line that provides the core flow rate of 45% due to forced circulation.
The APRM rod block line (control rod withdrawal prohibition limit line), 10 represents the 100% core flow control line, and 11 represents the minimum output line due to forced circulation characteristics.
第4図および第5図中、実線グラフは本実施例
の場合を、破線グラフは従来例の場合を示す。ま
たグラフに多数微小横線を付した部分は制御棒操
作を行う区間、付してない部分は炉心流量調整を
行う区間を表わしている。 In FIGS. 4 and 5, the solid line graph shows the case of this embodiment, and the broken line graph shows the case of the conventional example. In addition, the areas with many small horizontal lines on the graph represent the areas where control rod operations are performed, and the areas without lines represent areas where core flow rate adjustment is performed.
第4図中の水平区間2′,5′は制御棒操作又は
炉心流量調整による出力保持を示している。 Horizontal sections 2' and 5' in FIG. 4 indicate power maintenance by control rod operation or core flow rate adjustment.
さて、本実施例では、先ずa点から、強制循環
による最低炉心流量のもとで前記中間制御棒パタ
ーンを形成するように制御棒操作をすることによ
り、先述した規定の燃料線出力密度のしきい値
PCRとなる炉心出力に達するb点まで炉心出力を
上昇させ、b点で中間制御棒パターン完成とな
る。次いでb点から中間制御棒パターンを保つた
まま炉心流量を増加させることによりc点に達
し、c点から規定の燃料線出力密度変化率P〓を遵
守しながら中間制御棒パターン中の全挿入である
最外周又はその隣接の制御棒を引抜いて定格到達
目標制御棒パターンを形成するよう再び制御棒操
作をすることによつて、100%炉心流量制御ライ
ン10上のd点に達し、ここで定格到達目標制御
棒パターン完成となる。その後は定格到達目標制
御棒パターンを保つた状態で炉心流量のみを調整
することにより定格出力のe点に到達する。 In this example, first, from point a, the control rods are operated to form the intermediate control rod pattern under the minimum core flow rate due to forced circulation, thereby achieving the prescribed fuel line power density as described above. threshold
The core power is increased to point b, where the core power reaches P CR , and the intermediate control rod pattern is completed at point b. Next, from point b, by increasing the core flow rate while maintaining the intermediate control rod pattern, point c is reached, and from point c, the fuel line power density is fully inserted into the intermediate control rod pattern while observing the specified fuel line power density change rate P〓. By pulling out a certain outermost control rod or the adjacent control rod and operating the control rods again to form the target control rod pattern to reach the rating, point d on the 100% core flow control line 10 is reached, where the rated The target control rod pattern is completed. Thereafter, the rated output point e is reached by adjusting only the core flow rate while maintaining the rated target control rod pattern.
他方、従来例においては、その前記中間制御棒
パターン(第3図)を形成する制御棒操作により
強制循環の最低炉心流量にてa点から燃料線出力
密度しきい値PCRとなるb′点まで炉心出力を上昇
させ、そこから該中間制御棒パターンを保つたま
ま炉心流量の調整によりc′点まで出力上昇、次い
でd′点まで出力降下させてゼノン蓄積を促進し、
その後d′点から再び制御棒操作によりb″点(その
炉心出力レベルはやはり前記の燃料線出力密度し
きい値PCR以下になるようにする必要がある)ま
で炉心出力を上げ、ここで定格到達目標制御棒パ
ターン形成完了となり、その後は炉心流量調整の
みにより定格点e′に到達する。 On the other hand, in the conventional example, by operating the control rods that form the intermediate control rod pattern (Fig. 3), at the lowest core flow rate of forced circulation, from point a to point b' where the fuel line power density threshold value P CR is reached. The core power is increased to point C', and then the power is increased to point c' by adjusting the core flow rate while maintaining the intermediate control rod pattern, and then the power is decreased to point d' to promote Zenon accumulation.
Thereafter, the core power is increased from point d' to point b'' (the core power level must still be below the fuel line power density threshold P CR mentioned above) by operating the control rods again, and then the rated power is reached. The formation of the target control rod pattern is completed, and the rated point e' is then reached only by adjusting the core flow rate.
本発明実施例によれば、前述したような中間制
御パターンを採用したことにより、従来例と比較
して、出力上昇途中の低出力状態において炉心上
方の出力を大きくして出力分布を平坦化すること
ができ、強制循環の最低炉心流量ライン7にて燃
料線出力密度しきい値PCRとなる炉心出力に達す
るb点の炉心出力レベルを比較的高くすることが
でき、その後さらに最終的に定格到達目標パター
ン完成に到る過程を短縮し単純化し得る。これに
対し、従来例では、強制循環の最低炉心流量ライ
ン7にて該しきい値PCRとなるb′点の炉心出力レ
ベルが比較的低く抑えられ、その後に最終的に定
格到達目標制御棒パターン完成となるb″点に到る
前に、炉心出力をc′点まで上昇、d′点まで下降さ
せる所謂ならし運転を予め行う必要があり、操作
複雑で長い時間を要する。 According to the embodiment of the present invention, by adopting the above-mentioned intermediate control pattern, the power above the core is increased and the power distribution is flattened in a low power state in the middle of power increase, compared to the conventional example. As a result, the core power level at point b can be made relatively high, reaching the core power that becomes the fuel line power density threshold P CR at the minimum core flow rate line 7 of forced circulation, and then the core power level at point b can be made relatively high. The process of completing the target pattern can be shortened and simplified. On the other hand, in the conventional example, the core power level at point b' where the threshold value P CR is reached in the forced circulation minimum core flow line 7 is kept relatively low, and then the target control rod finally reaches the rating. Before reaching point b'', where the pattern is completed, it is necessary to perform a so-called break-in operation in which the core power is increased to point c' and decreased to point d', which is complicated and takes a long time.
第6図は、本実施例の中間制御棒パターン(第
2図b)の完成となる制御棒操作区間1の終点
b、および従来例の中間制御棒パターン(第3
図)の完成となる制御棒操作区間1′の終点b′に
おける炉心軸方向平均相対出力分布を示し、併せ
て定格到達目標制御棒パターン完成時の出力分布
を示した図である。この図から、本発明実施例の
中間制御棒パターンによる出力分布平坦化の効果
が明らかにわかるであろう。 FIG. 6 shows the end point b of the control rod operation section 1, which is the completion of the intermediate control rod pattern of this embodiment (FIG. 2 b), and the intermediate control rod pattern of the conventional example (the third
Fig. 12 shows the average relative power distribution in the core axis direction at the end point b' of the control rod operation section 1' when the control rod operation section 1' is completed, and also shows the power distribution when the target control rod pattern to reach the rating is completed. From this figure, the effect of flattening the power distribution due to the intermediate control rod pattern of the embodiment of the present invention can be clearly seen.
本発明実施例においては、出力分布が下方膨み
となり易い従来のb″点を避けるよう、前述の如く
先ず制御棒操作でb点まで、次いで炉心流量制御
によりb点からc点まで、次いで制御棒操作によ
りc点からd点まで、さらに流量制御によりd点
から最終的にe点まで出力上昇することにより定
格出力に到達するのである。この場合、c→dの
制御棒操作は中間制御棒パターンから最外周又は
それに隣接する制御棒の引抜によるものであつ
て、規定の出力上昇率P〓lを遵守して出力上昇が可
能である。すなわち、最外周又はそれに隣接する
制御棒の引抜による制御棒隣接燃料の線出力密度
の上昇は、しきい出力PCR以下に抑えることがで
きるため、炉心全体の出力上昇をP〓l以下となるよ
う抑えて出力上昇を行えばよいことになる。 In the embodiment of the present invention, in order to avoid the conventional point b'' where the power distribution tends to swell downward, as described above, the control rods are first operated to reach point b, then the core flow rate is controlled from point b to point c, and then the control rods are operated to reach point b. The rated output is reached by increasing the output from point c to point d through rod operation and then from point d to finally point e through flow control.In this case, the control rod operation from c to d is performed by controlling the intermediate control rod. It is possible to increase the output by pulling out the outermost control rod from the pattern or the control rod adjacent to it, and it is possible to increase the output while complying with the specified output increase rate P〓 l.In other words, by pulling out the outermost control rod or the control rod adjacent to it Since the increase in the linear power density of the fuel adjacent to the control rods can be suppressed to below the threshold power P CR , it is sufficient to increase the power by suppressing the increase in the overall power of the core to below P〓l .
中間制御棒パターン中の最外周又はそれに隣接
する制御棒のうち全挿入とする制御棒の本数は、
対象とする原子炉の炉心特性によつて定められる
が、一般的には20本挿入で約20%定格出力となる
ので、これを目安にその挿入本数を定めることが
できる。これは一般には4本以上であることが望
ましく、且つ炉心に対し対称配置に選ぶのが望ま
しい。 The number of control rods to be fully inserted among the outermost control rods in the intermediate control rod pattern or adjacent to it is:
It is determined by the core characteristics of the target reactor, but generally speaking, inserting 20 tubes will give about 20% of the rated output, so the number of tubes to be inserted can be determined using this as a guide. It is generally desirable that there be four or more, and that they are arranged symmetrically with respect to the reactor core.
中間制御棒パターンの最外周またはそれに隣接
する全挿入の制御棒を定格到達目標制御棒パター
ンへ向けて引抜く(第4図、第5図のc点からd
点への移行)には、好ましくはノツチ引抜を用い
る。ノツチ引抜においては、それらを4本程度づ
つ組にして全挿入から全引抜まで引抜いてもよい
し、又はそれらの全数を引抜位置が揃うようにし
て引抜いてもよい。 Pull out all the inserted control rods at or adjacent to the outermost circumference of the intermediate control rod pattern toward the target control rod pattern to achieve the rating (from point c to d in Figures 4 and 5).
(transition to a point) preferably using notch withdrawal. In the notch extraction, they may be pulled out in sets of about four, from full insertion to full withdrawal, or all of them may be pulled out so that the extraction positions are aligned.
また、b点からc点への移行のための炉心流量
の増加幅は定格炉心流量の約10%以上とするのが
好ましく、この炉心流量10%増加により軸方向出
力ピーキングで約3%改善される。 In addition, it is preferable that the range of increase in core flow rate for the transition from point b to point c be approximately 10% or more of the rated core flow rate, and this 10% increase in core flow rate will improve the axial power peaking by approximately 3%. Ru.
第7図は本発明の他の実施例による出力上昇を
炉心流量−炉心出力マツプで示したものである。
この実施例では、強制循環による最低炉心流量ラ
イン7での出力上昇から100%炉心流量制御ライ
ン10上での定格到達目標制御棒パターン完成に
至る出力上昇は、中間制御棒パターンからの最外
周又はそれに隣接する全挿入の制御棒の引抜操作
と炉心流量増加との交互実施により多段階的に行
われる。図中、12は30%炉心流量ラインを示
す。各段階での炉心流量の増加幅は、定格流量の
約10%以上であることが好ましい。本実施例は、
不安定になる恐のある強制循環による最低炉心流
量ライン7と100%炉心流量制御ライン10との
交る付近の領域をできるだけ避けると共に、制御
棒操作によるステツプ的な出力上昇を緩和する出
力上昇法である。 FIG. 7 shows the power increase according to another embodiment of the present invention as a core flow rate-core power map.
In this embodiment, the power increase from the power increase at the lowest core flow rate line 7 due to forced circulation to the completion of the rated target control rod pattern on the 100% core flow rate control line 10 is determined from the outermost or This is performed in multiple stages by alternately performing the withdrawal operation of the adjacent fully inserted control rods and increasing the core flow rate. In the figure, 12 indicates the 30% core flow line. The amount of increase in core flow rate at each stage is preferably about 10% or more of the rated flow rate. In this example,
A power increase method that avoids as much as possible the area near the intersection of the minimum core flow rate line 7 due to forced circulation and the 100% core flow rate control line 10, which may become unstable, and also alleviates the stepwise increase in power due to control rod operation. It is.
第8a図は、先記の実施例の中間制御パターン
において、最外周およびそれに隣接する制御棒以
外の制御棒のうち、定格到達目標制御パターン中
で全引抜でない制御棒は定格到達目標制御棒パタ
ーンでの引抜位置と同じ又はその近傍の引抜位置
とし、また定格到達目標制御棒パターン中で全引
抜である制御棒は全ストロークの75%以上炉外に
引抜いた位置とした制御棒パターンを中間制御棒
パターンとして採用する本発明の他の実施例に関
して、低流量、低出力時の炉心軸方向出力分布を
示したものである。同図の左半部はこれら制御棒
の位置を模式的に表わしている。本実施によれば
上記出力分布をより平坦化し得る。 Figure 8a shows that in the intermediate control pattern of the above embodiment, among the control rods other than the outermost and adjacent control rods, the control rods that are not fully drawn out in the rated target control pattern are in the rated target control rod pattern. Intermediate control is a control rod pattern in which the withdrawal position is the same as or near the withdrawal position in Regarding another embodiment of the present invention adopted as a bar pattern, the power distribution in the core axial direction at low flow rate and low power is shown. The left half of the figure schematically represents the positions of these control rods. According to this embodiment, the output distribution can be made even more flat.
第8b図は、比較のため、中間制御棒パターン
として、最外周およびそれに隣接る以外の制御に
ついてその若干本は全挿入、その余のものは全引
抜とした制御棒パターン(第3図のようなパター
ン)を採用する従来例の場合の炉心軸方向出力分
布を示す。同図左半部はこれら制御棒を模式的に
示す。 For comparison, Figure 8b shows an intermediate control rod pattern in which some of the controls other than the outermost and adjacent ones are fully inserted and the remaining ones are fully withdrawn (as shown in Figure 3). The figure shows the power distribution in the axial direction of the reactor core in the case of a conventional example that adopts a similar pattern. The left half of the figure schematically shows these control rods.
第8a図を第8b図と比べると、本実施例では
出力上昇途中の低炉心流量、低炉心出力時の炉心
出力分布が著しく平坦化されることが明らかであ
る。 Comparing FIG. 8a with FIG. 8b, it is clear that in this example, the core power distribution at low core flow rate and low core power during power increase is significantly flattened.
本発明のBWR起動法によれば、従来の起動法
に比べて、出力上昇途中において、炉心出力が下
方膨みとなる領域を回避し、且つ、強制循環での
最低炉心流量近傍の炉心流量にて燃料線出溶密度
しきい値に達する時点の炉心出力レベルを比較的
高くすることが可能で、しかも、不安定を招く恐
れのある強制循環による最低炉心流量ラインと
100%炉心流量制御ラインとの交る付近の領域を
避けながら、出力上昇の所要時間を短縮すること
ができ、起動日数は発電機併入から定格出力到達
までに約3日の短縮が可能である。しかも本発明
のBWR起動法は、従来と同じ燃料線出力密度し
きい値PCRおよびその後の燃料線出力密度変化率
P〓の規定を遵守しながら上記の効果を収めること
ができるものである。
According to the BWR startup method of the present invention, compared to conventional startup methods, it is possible to avoid the region where the core power swells downward during the power increase, and to maintain the core flow rate close to the minimum core flow rate in forced circulation. It is possible to make the core power level relatively high at the point when the fuel line melt density threshold is reached, and also to avoid the minimum core flow rate line due to forced circulation, which may lead to instability.
While avoiding the area near the intersection with the 100% core flow control line, it is possible to shorten the time required to increase the output, and it is possible to shorten the start-up time by approximately 3 days from the time the generator is installed to reaching the rated output. be. Moreover, the BWR startup method of the present invention uses the same fuel line power density threshold P CR and subsequent fuel line power density change rate as in the past.
It is possible to achieve the above effects while complying with the provisions of P〓.
第1図は到達出力パラメータとしたゼノンの蓄
積特性を示す図、第2図aおよびbは夫々本発明
の一実施例における定格到達目標制御棒パターン
および中間制御棒パターンを示す図、第3図は従
来例の中間制御棒パターンを示す図、第4図は本
発明の一実施例および従来例による炉心出力の時
間的経過を示すグラフ、第5図は第4図を炉心流
量と炉心出力との関係で示したグラフ、第6図は
本発明実施例の炉心出力分布の平坦化効果を従来
例との比較で示した図、第7図は本発明の他の実
施例による出力上昇を示す炉心流量−炉心出力マ
ツプ、第8a図および第8b図は夫々本発明の他
の実施例および従来例での炉心出力分布を示した
図である。
FIG. 1 is a diagram showing the accumulation characteristics of Zenon as the ultimate output parameter, FIGS. 2 a and b are diagrams showing the rated target control rod pattern and intermediate control rod pattern, respectively, in an embodiment of the present invention. FIG. 3 is a diagram showing the intermediate control rod pattern of the conventional example, FIG. 4 is a graph showing the time course of the core power according to an embodiment of the present invention and the conventional example, and FIG. FIG. 6 is a graph showing the flattening effect of the core power distribution of the embodiment of the present invention in comparison with the conventional example, and FIG. 7 is a graph showing the power increase due to another embodiment of the present invention. The core flow rate-core power map, FIGS. 8a and 8b, is a diagram showing the core power distribution in another embodiment of the present invention and a conventional example, respectively.
Claims (1)
る最外周制御棒またはそれに隣接する制御棒のう
ち複数本は全挿入とし、且つ最外周およびそれに
隣接する制御棒以外の制御棒のうち定格到達目標
制御棒パターン中で全引抜でない制御棒は定格到
達目標制御棒パターンにおけるのと同じ又はその
近傍の引抜位置とした制御棒パターンを中間制御
棒パターンに採り、出力上昇時に、先ず、該中間
制御パターンを形成する制御棒操作により、強制
循環での最低炉心流量もしくはその近傍の炉心流
量にて、炉心出力を規定の燃料線出力密度のしき
い値に達する炉心出力まで上昇させて、該炉心出
力まで上昇した時点で上記中間制御棒パターンを
完成し、該中間制御棒パターンの完成以後は、制
御棒パターンを固定したままで炉心流量の増加操
作のみで炉心出力を更に上昇させる過程と、それ
に次いで炉心流量を固定したままで定格到達目標
制御棒パターンへ向けての制御棒引抜操作のみで
規定の燃料線出力密度変化率の制限値を遵守しな
がら炉心出力を更に上昇させる過程とを経て、定
格到達目標制御パターンを完成することを特徴と
する沸騰水型原子炉の起動法。 2 前記中間制御棒パターン中で、最外周および
それに隣接する制御棒以外の制御棒のうち前記の
特定された引抜位置とされた制御棒でない制御棒
は制御棒ストロークの75%以上引抜かれた引抜位
置にある特許請求の範囲第1項記載の沸騰水型原
子炉の起動法。 3 中間制御棒パターンの完成後から定格到達目
標制御棒パターンの完成までの制御棒の前記引抜
操作を炉心流量の前記増加操作と交互に多段階で
行う特許請求の範囲第1項又は第2項記載の沸騰
水型原子炉の起動法。 4 前記炉心流量の増加操作での炉心流量増加の
幅は定格炉心流量の10%以上とする特許請求の範
囲第1項、第2項又は第3項記載の沸騰水型原子
炉の起動法。[Scope of Claims] 1. In the rated target control rod pattern, the outermost control rod or the adjacent control rods that are fully withdrawn are fully inserted, and the control rods other than the outermost control rod and the adjacent control rods are fully inserted. For the control rods that are not fully withdrawn in the rated target control rod pattern, the intermediate control rod pattern is set to the same or nearby withdrawal position as in the rated target control rod pattern, and when the output increases, First, by operating the control rods that form the intermediate control pattern, the core power is increased to the core power that reaches the specified fuel line power density threshold at the minimum core flow rate in forced circulation or a core flow rate close to it. The intermediate control rod pattern is completed when the core output reaches the core output, and after the intermediate control rod pattern is completed, the core output is further increased only by increasing the core flow rate while keeping the control rod pattern fixed. process, and then a process in which the core power is further increased while observing the specified fuel line power density change rate limit value by simply withdrawing the control rods toward the target control rod pattern to achieve the rating while keeping the core flow rate fixed. A method for starting a boiling water reactor characterized by completing a rated target control pattern through the following steps. 2. In the intermediate control rod pattern, among the control rods other than the outermost control rods and adjacent control rods, the control rods that are not in the specified extraction position are extracted by more than 75% of the control rod stroke. A method for starting a boiling water nuclear reactor as claimed in claim 1 in a position. 3. Claims 1 or 2, wherein the withdrawal operation of the control rods from the completion of the intermediate control rod pattern to the completion of the rated target control rod pattern is performed in multiple stages alternately with the increase operation of the core flow rate. The described method for starting a boiling water reactor. 4. The method for starting a boiling water reactor according to claim 1, 2, or 3, wherein the range of increase in core flow rate in the core flow rate increase operation is 10% or more of the rated core flow rate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58212098A JPS60104295A (en) | 1983-11-11 | 1983-11-11 | How to start a boiling water reactor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58212098A JPS60104295A (en) | 1983-11-11 | 1983-11-11 | How to start a boiling water reactor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60104295A JPS60104295A (en) | 1985-06-08 |
| JPH0445796B2 true JPH0445796B2 (en) | 1992-07-27 |
Family
ID=16616842
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58212098A Granted JPS60104295A (en) | 1983-11-11 | 1983-11-11 | How to start a boiling water reactor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60104295A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7267093B2 (en) * | 2019-05-16 | 2023-05-01 | 三菱重工業株式会社 | NUCLEAR POWER PLANT CONTROL DEVICE, NUCLEAR POWER PLANT AND NUCLEAR POWER PLANT CONTROL METHOD |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS54129290A (en) * | 1978-03-29 | 1979-10-06 | Hitachi Ltd | Operation method of boiling water reactor |
| JPS56124087A (en) * | 1980-03-05 | 1981-09-29 | Hitachi Ltd | Operating method of bwr type reactor |
-
1983
- 1983-11-11 JP JP58212098A patent/JPS60104295A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60104295A (en) | 1985-06-08 |
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