Nanostructure Evolution as Cause of the RPV Steel Non-Monotonic Radiation Embrittlement
Evgeny
Krasikov*
*Corresponding author: Evgeny Krasikov, Research Assistant, National Research Centre, Kurchatov Institute, Kurchatov Sq 1, Moscow 123182, Russia. Tel: +74991969233; Email: ekrasikov@mail.ru
Received Date: 28 August, 2017; Accepted Date: 06 September, 2017; Published Date: 13 September, 2017
Citation: Krasikov E (2017) Nanostructure Evolution as Cause of the RPV Steel Non-Monotonic Radiation Embrittlement. J Nanomed Nanosci: JNAN-123. DOI: 10.29011/JNAN-123. 100023
1. Abstract
Influence of neutron irradiation on Reactor Pressure Vessel (RPV) steel degradation are examined with reference to the possible reasons of the substantial experimental data scatter and furthermore nonstandard (non-monotonous) and oscillatory embrittlement behavior. In our glance this phenomenon may be explained by presence of the wavelike recovering component in the embrittlement kinetics.
We suppose that the main factor affecting steel anomalous embrittlement is fast neutron intensity (dose rate or flux), flux effect manifestation depends on state-of-the-art fluence level. At low fluencies radiation degradation has to exceed normative value, then approaches to normative meaning and finally became sub normative. In our opinion controversy in the estimation on neutron flux on radiation degradation impact may be explained by presence of the wavelike component in the embrittlement kinetics. Therefore, flux effect manifestation depends on fluence level. At low fluencies radiation degradation has to exceed normative value, then approaches to normative meaning and finally became sub normative. As a result of dose rate effect manifestation peripheral RPV’s zones in some range of fluencies have to be damaged to a large extent than situated closely to core.
Moreover, as a hypothesis we suppose that at some stages of irradiation damaged metal have to be partially restored by irradiation i.e. neutron bombardment. Nascent during irradiation nanostructure undergo occurring once or periodically evolution in a direction both degradation and recovery of the initial properties. According to our hypothesis at some stages of metal nanostructure degradation neutron bombardment became recovering factor. As a result, oscillation arise that in turn lead to enhanced data scatter. In this case we have to consider irradiation as a recovery factor.
2.
Keywords: Embrittlement Kinetics; Material
Intelligent Behavior; Reactor Pressure Vessel; Self-Recovering
Section; Steel
1. Introduction
Operating PWR’s reactor pressure vessels are subject to multi-factor influence. It is practically impossible to reproduce some of this factor (long-time bias, e.g.) in the framework of experimental investigations including RPV surveillance specimen’s tests. Detailed information that can be obtained by means of taking through RPV wall samples immediate from the decommissioned RPVs is more representative than received by any another way and therefore has a highest value.
Testing of the specimens presented a unique opportunity for qualifying consequences of long-term irradiation, multi-factor influence and dose rate (flux) effect on actual RPV properties. Data on radiation damage change through the ex-service RPV walls taking into account chemical factor and neutron flux were obtained. Controversy in the opinions on neutron flux on radiation degradation impact may be explained by presence of the wavelike component in the embrittlement kinetics that in turn is an indication of material intelligent behavior at some sections of RPV steel radiation embrittlement kinetics.
2. Experimental Procedures
Along with routine investigations in Russia systematic research on actual radiation embrittlement of the decommissioned PWR pressure vessel via through samples (trepans) has been carried out.
The
earliest commercial PWR prototype unit Novovoronezh-1 (NV1) RPV after 20 years
of operation was trepanned in 1987. Then Novovoronezh-2 (NV2), the oldest PWR
type experimental reactor-prototype ERP and, finely, nuclear icebreaker NIB)
Lenin RPVs also were trepanned. The most interesting and
unexpected data were
discovered during trepans of the first nuclear ship -
icebreaker Lenin investigation. Chemical analyses of the icebreaker RPV
material were carried out with FSQ Baird optical emission spectrometer. Results
can be seen in (Table 1).
Fast (E≥0,5MeV) neutron fluence evaluation was based on the specific Mn-54 and Nb-93m activities of the vessels steel and on the Nb-93m activity of the cladding.
The RPV materials radiation degradation (embrittlement) was determined by finding the ductile-to-brittle Transition Temperature Shift (TTS). RKP-300 impact pendulum test machine for standard Charpy specimens testing was used.
The general dependence of the TTS on radiation
embrittlement coefficient (REC) AF is
as follows: TTS=AF×Fn,
where AF is the radiation embrittlement coefficient and F is the fast (E≥0,5MeV) neutron fluence in units of 1018sm-2(fluence factor), n - coefficient (~1/3).
For Russian RPV Cr-Mo-V base steel AF=A×(P+0,07Cu), where A - coefficient (800 at
270°C), P and Cu - are the weight
concentrations of these elements.
3. Test Results
The unexpected results of the icebreaker RPV weld
and base metal studying are given in (Figure 1).
where one can recognize that the actual (measured) radiation embrittlement coefficients of the trepan materials for the periphery (remote) zone of the vessel are significantly higher that for the inner part. One can see also that hardness measurement and Charpy impact testing results agree.
Note: HB=252|189kgf/mm2 - hardness values at as-received condition after annealing 650°C/2h.
4. Data Analysis and Discussion
First impression from foregoing decommissioned PWR pressure vessel material properties study - enhanced degradation rate at low neutron fluxes. Registered facts denote that known as flux effect factor was in action. Unexpected circumstance however is reduced embrittlement zone appearance that follows after of previous part of enhanced embrittlement.
In support of the unusual materials gained, we started flux effect purposeful study using surveillance specimens from WWER-440/213 RPV. Taking into account the flux level that is the irradiation position of the selected standard Charpy-type surveillance specimens additional sub size specimens were manufactured and tested. Analysis shows that 3-fold difference in flux level may lead to evident distinction in terms of TTS: ≈60°С at neutron fluence of 4×1019cm-2 and copper concentration as low as ~0,1% mass [1].
Search
of similar far from trivial effect brings to example where it characterized by
authors as quite atypical for Doel I, II weld metal SS data (Figure 2) [2].
One can
recognize that relatively to
Regulatory Guide 1.99 curves zones with opposite effects take place, enlarged shift
changes by depressed one. For the sake of correctness, it is necessary to
underline that the first mention concerning distinction between test reactors and
low-lead-factor (surveillance) data had appeared as early as 1980 [3]. Summing the previously mentioned on the subject
discussed one might conclude, that depending of the fluence level reached
manifestation of the flux effect in reference to Guide pattern may be quite
different, namely: negative, positive and two zeros as represented in (Figure 3).
Situation looks like famous parable blind men and an elephant, where a group of blind men (or men in the dark) touch an elephant to learn what it is like. The story is used to indicate that reality may be viewed differently depending upon one's perspective, suggesting that what seems an absolute truth may be relative due to the deceptive nature of half-truths.
Regulatory Guide dependence (formula) has appeared as a result of forced irradiation in test reactors. One can recognize however that specific properties of metal and actual reactor environment may deform this ideal trajectory to the extent that curve monotony character damage. The very wonderful fact is the enhanced degradation aftereffect of the temporary weakening of the embrittlement appearance. Possible comprehensible explanation is as follows: the radiation-induced copper-rich precipitates nature (dimensions and concentration) alteration. Evidently, we have fixed phenomenon similar to observed in [4] where neutron irradiation in some range of doses improves the mechanical properties of the unirradiated mild steel (Figure 4).
It is seen that irradiation of
unirradiated (initial condition) steel up to dose of ~2,0×1018cm-2 along
with strengthening lead to more than 2-fold ductility increase.
In accordance with sketch of (Figure 3) flux effects manifestation depends on fluence level. At low fluencies radiation degradation has to exceed normative value, then approaches to normative meaning and finally became sub normative. As a result of dose rate effect manifestation peripheral RPV’s zones in some range of fluencies have to be damaged to a large extent than situated closely to core.
5.
Conclusion
Influence of neutron irradiation on Reactor Pressure Vessel (RPV) steel degradation are examined with reference to the possible reasons of the substantial experimental data scatter and furthermore - nonstandard (non-monotonous) and oscillatory embrittlement behavior. In our glance this phenomenon may be explained by presence of the wavelike recovering component in the embrittlement kinetics.
We suppose that the main factor affecting steel anomalous embrittlement is fast neutron intensity (dose rate or flux), flux effect manifestation depends on state-of-the-art fluence level. At low fluencies radiation degradation has to exceed normative value, then approaches to normative meaning and finally became sub normative. Data on radiation damage change including through the ex-service RPVs taking into account chemical factor, fast neutron fluence and neutron flux were obtained and analyzed.
In our opinion controversy in the estimation on neutron flux on radiation degradation impact may be explained by presence of the wavelike component in the embrittlement kinetics. Therefore, flux effect manifestation depends on fluence level. At low fluencies radiation degradation has to exceed normative value, then approaches to normative meaning and finally became sub normative. As a result of dose rate effect manifestation peripheral RPV’s zones in some range of fluencies have to be damaged to a large extent than situated closely to core. This finding recently was confirmed by German scientists [5].
Moreover, as a hypothesis we suppose that at some stages of irradiation damaged metal have to be partially restored by irradiation i.e. neutron bombardment. Nascent during irradiation structure undergo occurring once or periodically transformation in a direction both degradation and recovery of the initial properties. According to our hypothesis at some stages of metal structure degradation neutron bombardment became recovering factor. Self-recovering section of RPV steel radiation embrittlement kinetics as indication of material intelligent behavior. As a result, oscillation arise that in turn lead to enhanced data scatter. In this case we have to consider irradiation as a recovery factor.
Foregoing
hypothetical assumptions on “Low-dose effects” in terms “Radiation embrittlement
contains oscillatory component” and “Radiation annealing of the radiation
embrittlement” is questionable and needs additional experimental verification
and profound scientific study. The information gained would be relevant to the
RPV degradation mechanisms consideration and understanding, also to possible
current PWR generation lifetime extension evaluation.
Figure 1: Radiation Embrittlement Coefficient AF and Hardness Value HB Through the Icebreaker RPV Wall Distribution. TT-Transition
Temperature, TT0 - Transition
Temperature in Initial State.
Figure 2: Doel I, II Weld -
Surveillance Results.
Figure 4: Stress-Strain Curves of Steel as a Function of
Neutron Fluence.
Material |
C |
Mn |
Si |
P |
Cu |
Mo |
Ni |
Cr |
V |
Weld |
0,05 |
1,03 |
0,41 |
0,035 |
0,15 |
0,49 |
0,17 |
1,39 |
0,15 |
Base |
0,17 |
0,45 |
0,28 |
0,018 |
0,09 |
0,67 |
0,35 |
2,75 |
0,09 |
Material |
C |
Mn |
Si |
P |
Cu |
Mo |
Ni |
Cr |
V |
Weld |
0,05 |
1,03 |
0,41 |
0,035 |
0,15 |
0,49 |
0,17 |
1,39 |
0,15 |
Base |
0,17 |
0,45 |
0,28 |
0,018 |
0,09 |
0,67 |
0,35 |
2,75 |
0,09 |
Table 1: Chemical Composition of the Icebreaker RPV Materials Under Study [%%Wt.]
1.
Nikolaenko VA and Krasikov EA (2004) Dose
rate effect on WWER-440/213 RPV materials embrittlement, Atomic energy: 177-182.