Control rod for nuclear reactor

Induced nuclear reactions: processes – systems – and elements – Control component for a fission reactor

Reexamination Certificate

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C376S219000, C376S333000

Reexamination Certificate

active

06285728

ABSTRACT:

The present invention relates to a control rod for a nuclear reactor, and more particularly, to a control rod for a nuclear reactor of the long-life type having an improved mechanical soundness in a boiling water reactor.
A control rod for a boiling water reactor (BWR) has usually four wings formed by housing neutron absorber plates in a plurality of long sheaths having a deep U-shaped cross-section. A leading end structural member is provided at an insertion leading end portion of each of the wings, or a terminal end structural member, at an insertion terminal end portion thereof, and the U-shaped openings of the sheaths in each of four wings are secured to an integral type center structural member (known also as a tie rod) having a cruciform cross-section to provide a cruciform sectional configuration or arrangement.
In a conventional control rod, the sheath is made of stainless steel (S.S such as SUS, hereinafter abbreviated as “SUS”), and a SUS tube having a diameter of 5 mm filled with boron carbide (B
4
C) powder has been employed as a neutron absorbing rod.
Boron (B) has however a short nuclear life because it reacts with neutron to generate helium (He) and lithium (Li), resulting in a degraded neutron absorbing ability, and helium causes an increase in internal pressure, leading to a decrease in soundness of the SUS tube and hence to a shorter mechanical and physical service life.
In order to provide a control rod having a long service life, there has been used a long-life type control rod manufactured by replacing a conventional neutron absorbing rod partially or totally by hafnium (hereinafter abbreviated as “Hf”) which is a long-life type neutron absorber.
Since Hf has a large specific gravity (density) as about 13, an Hf rod having the same cross-section as a conventional neutron absorbing rod using boron carbide results in a weight about 1.5 times as large as the control rod as a whole, although the neutron absorbing ability (reactivity value) is substantially the same, making it impossible to back-fit it into a nuclear reactor in operation.
As a counter-measure, Japanese Patent Laid-open (KOKAI) Publication No. HEI 1-34358 “Control Rod for Nuclear Reactor” proposes an Hf control rod of the type known as a trap type in which Hf is formed into a plate shape, and two Hf plates are arranged opposite to each other with a gap for introduction of water.
Further, in view of the fact that in about the terminal end side half of a control rod for the BWR, upon insertion thereof into the reactor core, a decreased neutron absorbing ability would cause no inconvenience in the control of the BWR, a control rod configured so as to use a smaller Hf content in the portion on the insertion terminal end side than in the portion on the insertion leading end side is proposed in Japanese Patent Laid-open Publication No. HEI 7-3468 “Control Rod for Nuclear Reactor”.
Regarding the long-life control rod having the trap structure using the Hf plate, excellent results have already been achieved in many BWRs, and it is the usual practice to set aL short service life for maintenance purposes.
When setting a longer service life, it becomes now clearer than ever that it is effective to improve mechanical strength of SUS structural members such as a sheath in the control rod.
FIGS. 19
to
21
illustrate an outline of an Hf trap type control rod, in which
FIG. 19A
is a partially cutaway perspective view,
FIG. 19B
is a sectional view of a wing and
FIG. 19C
is a perspective view of a load supporting member (also referred to as a “load supporting spacer” of “top spacer”).
FIG. 20A
is a partially cutaway front view of a sheath shown in
FIG. 19A
, and
FIG. 20B
illustrates an example of thickness of an Hf plate which is a neutron absorber plate of a neutron absorbing material attached in the interior of a sheath, as illustrated in a distribution diagram in the control rod insertion/withdrawal direction which is the sheath longitudinal direction.
FIG. 21A
is a partially enlarged front view of
FIG. 20A
,
FIG. 21B
is an enlarged front view of a pair of Hf plates shown in
FIG. 21A
, and
FIG. 21C
is a sectional view of
FIG. 21C
taken along the line XXIC—XXIC of FIG.
21
B.
Referring to these figures, a long-life type control rod
1
has a cruciform section with four wings
2
, and a leading end structural member
4
integral with a handle
3
is secured to the insertion leading end portion into the reactor core, and a terminal end structural member
5
i s secured to an insertion terminal end portion.
Further, a cruciform integral type center structural member made of SUS is provided a t an axial center of the control rod
1
(central tie rod), and an opening portion of a sheath
7
made of SUS having a deep U-shaped cross-section forming an outer periphery of the wing
2
is secured by welding to each projection of this integral type center structural member
6
.
A plurality of sheath holes
8
and water holes
9
are pierced in the sheath
7
, in which two Hf plates
10
which are neutron absorber plates are supported by a load supporting member
12
also serving as a gap (interval) maintaining space, and a water gap
11
(gap through which cooling water flows during use in the reactor) is formed between the two Hf plates
10
.
The load supporting member
12
has a top-like shape, and the thickness of a gap maintaining portion
12
a
at the center thereof has a function of spacer. The Hf plates
10
are supported by attaching the Hf plates
10
from both the sides to a support shaft
12
b
through an attachment hole
13
and causing engagement of the support shaft
12
b
with a sheath hole (bore)
8
, which are secured together by means of welding.
When inserting or withdrawing the control rod
1
into or from the reactor core, a percussive force is applied to the sheath
7
upon intermittent driving, or particularly, upon starting driving or decelerating during scram of the reactor.
In a long-life type control rod
1
, the sheath
7
and the load supporting member
12
made of SUS forming the wing
2
have a thermal expansion coefficient about three times as high as that of the Hf plate
10
, which is the neutron absorber formed of a material different from those of the sheath
7
and the load supporting member
12
. For example, while SUS has a thermal expansion coefficient of 17.8×10
−6
/deg-C, that of Hf is 5.9×10
−6
/deg-C (“Nuclear Reactor Materials Handbook” published by Nikkan Kogyo Shinbun-sha).
To avoid inconveniences resulting therefrom, the attachment hole
13
of the Hf plate
10
to be attached to the support shaft
12
b
of the load supporting member
12
has a diameter larger than that of the support shaft
12
b
to provide a margin, thereby permitting avoidance of their mutual interference through expansion and contraction in heat cycles during operation of the reactor.
In the example shown in
FIG. 20
, the Hf plate
10
of the control rod
1
having a length L in the inserting direction into the reactor core or the sheath longitudinal direction is longitudinally and equally divided into eight sections. The length
1
of a single Hf plate
10
is therefore about L/8.
FIGS. 20 and 21A
are described with a scale compressed in the axial direction for convenience of illustration, and
FIG. 21B
represents the Hf plate substantially similarly to the actual one.
Within the wing
2
, two Hf plates
10
which are neutron absorber plates arranged opposite to each other form an Hf plate pair
14
which is held by the sheath
7
through four (or three, five or six) load supporting members
12
.
The attachment hole
13
of the Hf plate and the sheath hole
8
of the sheath
7
have the same pitch
15
size in the sheath longitudinal direction.
During inserting or withdrawing operation of the control rod
1
, the sheath
7
is subjected, not only to a static load caused by the weight of the Hf plate pair
14
applied through the load supporting member
12
in the stationary state, but also to a dynamic load caused by the relative displacement to the Hf pl

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