Abstract:Dilatometry tests were performed to study the phase transformation kinetic of nuclear fuel claddings made of Zircaloy-4 upon fast heating rates (up to 2000 • C/s). These tests highlighted that from equilibrium to 500 • C/s the temperature at which the transformation starts shifts towards higher temperatures with increasing heating rates. Above 500 • C/s, no impact of the heating rate was observed. The temperature at which the transformation ends remains close to 960 • C with no clear dependence on heating rate… Show more
“…More recent investigations of phase transformation kinetics include Nguyen et al’s 22 , 23 in-situ synchrotron X-ray diffraction (SXRD) measurements of cold-worked (CW) Zircaloy-4L subjected to heating rates in the range of 10 to 100 K/s, and electrical resistivity measurements of CW Zircaloy-4L and RX Zircaloy-4L at 100 K/s 22 , 24 , supporting their SXRD measurements. In a new study, Jailin et al 25 using dilatometric technique measured the phase transformation kinetics of SRA Zircaloy-4L subjected to very high heating rates, i.e. from 50 to 2000 K/s.…”
We present a kinetic model for solid state phase transformation ($$\alpha \rightleftharpoons \beta$$
α
⇌
β
) of common zirconium alloys used as fuel cladding material in light water reactors. The model computes the relative amounts of $$\beta$$
β
or $$\alpha$$
α
phase fraction as a function of time or temperature in the alloys. The model accounts for the influence of excess oxygen (due to oxidation) and hydrogen concentration (due to hydrogen pickup) on phase transformation kinetics. Two variants of the model denoted by A and B are presented. Model A is suitable for simulation of laboratory experiments in which the heating/cooling rate is constant and is prescribed. Model B is more generic. We compare the results of our model computations, for both A and B variants, with accessible experimental data reported in the literature covering heating/cooling rates of up to 100 K/s. The results of our comparison are satisfactory, especially for model A. Our model B is intended for implementation in fuel rod behavior computer programs, applicable to a reactor accident situation, in which the Zr-based fuel cladding may go through $$\alpha \rightleftharpoons \beta$$
α
⇌
β
phase transformation.
“…More recent investigations of phase transformation kinetics include Nguyen et al’s 22 , 23 in-situ synchrotron X-ray diffraction (SXRD) measurements of cold-worked (CW) Zircaloy-4L subjected to heating rates in the range of 10 to 100 K/s, and electrical resistivity measurements of CW Zircaloy-4L and RX Zircaloy-4L at 100 K/s 22 , 24 , supporting their SXRD measurements. In a new study, Jailin et al 25 using dilatometric technique measured the phase transformation kinetics of SRA Zircaloy-4L subjected to very high heating rates, i.e. from 50 to 2000 K/s.…”
We present a kinetic model for solid state phase transformation ($$\alpha \rightleftharpoons \beta$$
α
⇌
β
) of common zirconium alloys used as fuel cladding material in light water reactors. The model computes the relative amounts of $$\beta$$
β
or $$\alpha$$
α
phase fraction as a function of time or temperature in the alloys. The model accounts for the influence of excess oxygen (due to oxidation) and hydrogen concentration (due to hydrogen pickup) on phase transformation kinetics. Two variants of the model denoted by A and B are presented. Model A is suitable for simulation of laboratory experiments in which the heating/cooling rate is constant and is prescribed. Model B is more generic. We compare the results of our model computations, for both A and B variants, with accessible experimental data reported in the literature covering heating/cooling rates of up to 100 K/s. The results of our comparison are satisfactory, especially for model A. Our model B is intended for implementation in fuel rod behavior computer programs, applicable to a reactor accident situation, in which the Zr-based fuel cladding may go through $$\alpha \rightleftharpoons \beta$$
α
⇌
β
phase transformation.
“…The equilibrium data can be found in [4]. The 1200 • C/s curve was obtained by a stress-free dilatometry experiment performed at an imposed heating rate of 1200 • C/s on a GLEEBLE-3500 device [31]. The 230 phase fraction accuracy is estimated to be 5% of the phase fraction between 10 and 90% of β content.…”
The thermo-mechanical behavior of Zircaloy-4 claddings under simulated post-DNB RIA conditions was investigated. Around twenty experiments were performed in simulated post-DNB conditions, i.e. creep ballooning tests with heating rates greater than 1000 • C/s. Two different levels of pressure of 7 and 11 bar were tested for temperatures of interest ranging from 840 • C to 1020 • C. A complex creep behavior was highlighted in this range of temperature. It appears very well correlated to the phase content present within the material during fast thermal transients. Tests with low thermal transients were also performed and evidence a strong impact of the heating rate on the thermo-mechanical properties of the claddings.
“…From this, it follows that it is sometimes necessary to work directly on structural samples, in order to take into account the effects of geometry and fabrication process of the specimen on its thermomechanical behavior. On another hand, the loading conditions example, the heating rate may affect the phase transformation of the material [2,3,4] and thus may affect its mechanical properties [3,5,6]. Therefore, the identification of a constitutive model must be done in conditions as close as possible to real life conditions in order to avoid extrapolations that may lead to 30 uncontrolled discrepancies.…”
Section: Introductionmentioning
confidence: 99%
“…The ballooning deformation and the temperature at the sample surface were measured by stereo-correlation and near infrared thermography, respectively. The sample, made of Zircaloy-4 alloy, shows a (α → β) phase 50 transformation at high temperature from around 800 to 1000 °C [3, 9,10,4]. This transformation, studied and modeled in [4] from equilibrium to 2000 °C/s, shows a strong dependence to the heating rate.…”
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