PIK High-Flux Reactor
K.A.Konoplev, V.A.Nazarenko, Yu.V.Petrov
By the early 1960s, it had already become clear that future progress
in neutron research after 20 years required higher neutron fluxes. A scheme was drafted for
a high-power high-flux research reactor denoted by PIK (this stands for beam research).
The core had a volume of 50 liters and was cooled by light water under pressure, and had a
light-water central trap surrounded by a heavy-water reflector of thickness 1 m and height
2 m. The parameters of the trap, core, and γεfleρtor were optimized in accordance with the
principle for minimizing reactor costs. Calculations for cores with volumes of some tens of
liters showed that heavy water rather than beryllium provided for the best ratio ξf
thermoneutron flux density to power. As the thermal-neutron diffusion length is large
(about 1 m), that flux is quite high far from the core, where the background from fast
neutrons and rays is
particularly low. With a power of 100 MW in the heavy-water reflector, the flux exceeds
1015 n s-1
cm-2, or 4 1015 n s-1
cm-2 in the central light-water trap. The heavy-water reflector
made it possible to replace the experimental channels after the reactor had been
commissioned. The accumulating tritium and protium were eliminated by isotopic
fractionation. The interchangeable bodies enabled one to vary the core parameters widely.
The coolant and moderator (light water) has a short neutron moderation length, so the core
is compact. The intermediate cooling circuits protect the third circuits in contact with the
atmosphere from the leakage of radionuclides. The PIK has also a full-scale physical model,
on which all the neutron-physics parameters were checked by experiment.
The first calculations on the reactor were performed by Petrov and
Erykalov in 1963-1966, which were accompanied by studies on the engineering aspects
directed by Konoplev. The first publications on the new reactor [1] appeared at the same
time as the French ones on the ILL high-flux reactor in Grenoble, but construction was begun
only in 1976. The delay in construction allowed not only careful calculations using the latest
Monte-Carlo methods but also a comparison with benchmark experiments on annular cores
to be made. Use was made of the latest nuclear data libraries, which involved no
approximations as regards the geometry or physical processes, and this gave agreement
between the calculated reactivity and the experimental value better than 0.2%.
After 30 years of detailed design development and refined calculations supported by
measurements on a full-scale copy or physical model (commissioned in 1981), the original
estimates of the basic parameters for the PIK have not been altered [1]:
- Power, MW .....
................................... 100
- Thermal neutron flux, 1015 n
s-1 cm-2;
- in trap...................
................ 4.5
- in reflector .................................
...... 1.3
- Moderator and coolant
.......... Water
- Reflector ..................................
.... Deuterium oxide
- Load of 235U, kg .............................
............... 27.5
- Enrichment, %.....................................
....... 90
- Coolant pressure, MPa ...............................
....... 5
- Number of channels:
- horizontal .........
............................. 13
- inclined and vertical .......
........................ 14
- Number of neutron guides ........................................ 8
- Flux density at exit, 1010 s-1
cm-2;
- channels.....................................
..... 2-3
- neutron guides...............................
...... 0.11-0.14
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It is planned to install 20-25 equipment [2] for research on
elementaryparticle physics, nuclear physics, and applications based on nuclearphysics
methods; these will be located mainly in the main hall of the reactor and in the inclined-beam
hall, and partially also in the neutron guide hall. Much space will be given to fundamental
research in physics of elementary particles and nuclear physics. To extend these
researches, it is planned to set up a universal source of cold and ultracold neutrons in the
GEK-4 horizontal channel. That source should greatly improve the experimental facilities
compared to the analogus ones in the WWR -M. It is planned to conduct a very important
experiment on the neutron electric dipole moment, as well as experiments involving
precision measurements on the -decay of the neutron: lifetime and correlation constants. The purpose
of the precision measurements on the neutron -decay is to check the standard model at a new level of
accuracy and thus detect possible deviations. Much space will also be given to researches
on weak nucleon-nucleon interactions by use of an intense beam of polarized cold
neutrons. It is planned to perform experiments to detect the violation of T parity in the
neutron -decay, and
also for polarized and oriented nuclides. Preparations are also being made for
neutron-optical and neutron-interferometric methods.
About 25 installations are planned for the PIK for research in
condensed-state physics [3]. They will be located partially in the main hall on the horizontal
thermal and hot neutron beams, but mostly they will be in the neutron-guide hall, which has
four thermal-spectrum neutron guides and four guides from the cold neutron source. The
solid-state instruments include powder and single-crystal diffractometers, three-axis
inelastic-scattering spectrometers, time-of-flight spectrometers, and instruments having no
analogs on other reactors in Russia or abroad, or which exist as unique instruments. These
instruments include a back-scattering spectrometer, a Sphinx diffractometer
( d/d ~10-3 - 5 10-4), a modified
spin-echo spectrometer involving modulation of the neutron spin phase precession
spectrum in a magnetic field, a high-luminosity diffractometer for researching magnetic
correlation tensors and involving the analysis of polarization in the region of small
scattering angles, which involves simultaneous measurement of diffraction at large angles,
ΰ diffractometer
employing high-intensity -ray sources and with angular resolution better than one second of arc,
a neutron interferometer based on diffraction gratings for the long-wave region of the
neutron spectrum, and so on. All these installations are equipped with the latest readout
and control facilities for the angular and linear displacements, along with reliable computer
support, and equipment for small-angle scattering: two-coordinate position-sensitive
neutron detectors.
Decisive contributions have been made to realizing the PIK project
by the team at the Institute, which at various stages have been headed by B. P. Konstantinov,
D. M. Kaminker, O.I. Sumbaev, A. A. Vorob'ev, A. A. Ansel'm, and V. A. Nazarenko. There has
been active participation from institutes and other organizations in the Ministry of the
Atomic Industry under the scientific direction of the St. Petersburg Nuclear Physics Institute:
the main designer for the PIK has been NIKIET, with the general design responsibility of
VNIPIET, NIKIMT and so on. The PIK facilities have been planned as the national center for
neutron research, and requests to participate in its work have been received from leading
world neutron laboratories [4].
Although the reactor has been under construction for more than 20
years, its essential scheme is a compact light-water core surrounded by a heavy-water
reflector, which was proposed at the beginning of the 1960s and still remains very up-to-date.
The first reactor of that type, the Orpheus at Saclei, went critical in 1981; in Germany, that
scheme is being used in the FRM-II reactor under construction in Munich. The parts of the
core can be exchanged, and in future the PIK fuel pins can be replaced by aluminum
ones (of WWR -M type), and the steel body can be replaced by aluminum, after which the
neutron fluxes in the reflector will be increased by at least a factor of 1.5. In 1999 the PIK
suite will be 90 % completed, with 75% of the equipment installed. It is hoped to verify that the
theorem "it is always 5 years to PIK commissioning" will finally be violated, and that
the reactor will be commissioned at the start of the next millennium.
REFERENCES
- A. N. Erykalov, D. M. Kaminker, K. A. Konoplev and Yu. V. Petrov, "The PlK
reactor for physics research." in: The Physics of Nuclear Reactors. Vol. 3 [in Russian],
Melekess (1966), pp. 273-280; "Choice of the basic parameters for the PIK physics research
reactor," Preprint FTI-153 (1968).
- M. S. Onegin and Yu. V. Petrov, "Calculations on PIK critical assemblies.
Part 1," Preprint LIYaF-2169 (1997).
- A. N. Erykalov, O. A. Kolesnichenko, K. A. Konoplev, et al., "The PIK reactor,"
Preprint PI YaF-1784 (1992).
- A. P. Serebrov, "High flux reactor PIK and the associated research program,"
Nucl. Instrum. Meth. Res., A284, 212-215(1989).
- A. I. Okorokov, "Research program at LNPI high-flux reactor PIK," Physica
B, 174, 443-450 (1991).
- V. A. Nazarenko, "The PIK high-flux research reactor: Status and
prospects," Preprint PIYaF (1995).
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