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An Estimation of the Thermal Properties of Pu-Rich Metallic Fuel.

1. Introduction

Fast reactors can burn transuranic elements (TRUs; Pu, Np, Am, and Cm) effectively owing to their higher fission-to-neutron-capture ratio than light-water reactors (LWRs). LWRs will be the dominant nuclear power plants for at least the next few decades. To burn the TRUs produced from LWRs, it is necessary to improve the TRU burning capability of fast reactors. Because uranium TRU-fueled fast reactors also produce TRUs, the most effective approach is to use uranium-free TRU fuel because this does not produce additional TRUs. Such a system could reduce the capacity of the TRU burner units and the associated fuel cycle facilities to about 1/5 and 1/8, respectively. There have been many studies on uranium-free or fertile-free fuel systems [1-3]; however, difficulties remain, such as the requirement for new reprocessing technology. For example, reprocessing technology for producing TRU-burning oxide fuel is required to separate actinides and lanthanides, which have similar chemical behavior [4]. In addition, the remote control technology for reprocessing needs modifications because of high radioactivity of minor actinides. By contrast, uranium-free TRU metal could be reprocessed and fabricated based on pyroprocess and injection-casting technologies without substantial modification [5].

In the United States, many studies concerning uranium-free metal fuels have been carried out. Most notably, the US accelerator-driven transmutation of waste (ATW) program investigated an accelerator-driven transmutation system coupled with a subcritical fast reactor using uranium-free metal fuel [6-9]. In such systems, thermal properties, such as the heat capacity, thermal conductivity, and melting temperatures of the fuel, are important for the design of the core structure of the burning reactor.

In our previous study, we estimated the melting temperature of TRU-Zr alloys [10] and the thermal properties of Pu-rich alloys [11]. In the present study, we evaluate the thermal properties of Pu-40Zr (Pu-64at%Zr), a candidate material for TRU burners, and Pu-20U-20Zr (Pu-15at%U-40at%Zr) in a more relevant way.

2. Estimation of Thermal Properties

We calculated the heat capacity, thermal conductivity, and solidus and liquidus temperatures of the Pu-40Zr and the Pu-U-Zr alloys because experimental work with plutonium is difficult to obtain approval in Japan. The heat capacity of alloys was estimated using the Neumann-Kopp law, which is equivalent to an additive law. Although the heat capacity varied considerably with phase changes, the estimated values for Pu-40Zr and Pu-20U-20Zr alloys were similar if their phases were the same.

Generally, the thermal conductivity at high temperatures is calculated from the heat capacity, thermal diffusivity, and density. The heat capacity and density are often estimated from the Neumann-Kopp law and Vegard's law. However, the thermal diffusivity is comparatively difficult to estimate because it varies significantly with composition, phase, and temperature. Another common way to estimate the thermal conductivity of metallic materials is to use the Wiedemann-Franz law, which multiplies the electrical conductivity, absolute temperature, and Lorentz number [12]. Unfortunately, however, the electrical conductivity of Pu-Zr alloys had not been reported. Nordheim's rule is a common way to estimate the electrical conductivity of element although its use is limited to alloys that form a solid solution. Fortunately, Pu-Zr and Pu-U-Zr alloys are considered to form a body-centered cubic (bcc) solid solution from related binary systems and the U-Pu-Zr ternary system [13, 14]. Therefore, the thermal conductivity of Pu-40Zr and Pu-20U-20Zr alloys was estimated using both the Wiedemann-Franz law and Nordheim's rule with the Nordheim coefficients.

Finally, we calculated the solidus and liquidus temperatures using Thermo-Calc, which is based on the CALPHAD method. The phase diagrams of the U-Zr, Pu-Zr, and U-Pu systems are available in the literature; thus, we calculated the liquidus and solidus temperatures by creating a pseudobinary system of the Pu-(0-80U)-20Zr alloy.

2.1. Heat Capacity. Figure 1 shows the data available in the literature for the U-Zr alloy [15] and the constituents: uranium, zirconium, and plutonium [16, 17]. There are anomalous peaks for the heat capacities of all three elements, which are caused by their phase transitions. The heat capacity of a compound can be estimated using the Neumann-Kopp (additive) law [18, 19]. Specifically, if a solid compound, M, is formed from elements A, B, and C by a chemical reaction:

aA + bB + cC [right arrow] M, (1)

then the heat capacity of the compound CPM is expressed by the heat capacity of each element as follows:

[C.sub.PM] = [aC.sub.PA] + [bC.sub.PB] + [cC.sub.PC]. (2)

The heat capacity of the U-Zr alloy measured by Matsui et al. [20] was similar to that calculated using the Neumann-Kopp law. Therefore, it may be possible to use it to determine the heat capacities of Pu-Zr and Pu-U-Zr alloys. Plutonium has many phase transitions, at which its heat capacity changes. For the Pu-Zr system created by Kurata [21], the Pu-40Zr alloy had two phases from room temperature to melting point, and the phase-transition temperature was approximately 902 K (Figure 2).

The low-temperature phase is a face-centered cubic (fcc) structure, and the high-temperature phase is a bcc structure. Below 902 K, the heat capacity of plutonium in our calculation was determined by interpolation and/or extrapolation of the value for the [beta] and [delta] (fcc) phases. Above 902 K, the heat capacity was determined by extrapolation of the [epsilon] (bcc) phase. The heat capacity of zirconium was determined in a similar manner. Figure 3 shows the estimated heat capacity for Pu-40Zr and Pu-20U-20Zr alloys. For the Pu-20U-20Zr alloy, the phase-transition temperature was approximately 900 K, based on the available phase diagrams. The obtained fitting equations were as follows:

[mathematical expression not reproducible]. (3)

Although the phase transition temperature was different from the U-50Zr alloy, the value of Cp was not so different from it which has a similar ratio of zirconium with the Pu40Zr alloy.

2.2. Thermal Conductivity. Wiedemann-Franz law is known as a specific rule in metallic elements, which connect thermal conductivity with electrical conductivity [12]:

[kappa] = L[sigma]T = LT/[rho], (4)

where [kappa] is the thermal conductivity ([Wm.sup.-1] x [K.sup.-1]), a is the electrical conductivity ([[ohm].sup.-1] x [m.sup.-1]), [rho] is the electrical resistivity ([ohm]m), L is the Lorentz number, and T is the temperature (K). The Lorentz number is typically derived from the experimental measurement of thermal and electrical conductivity. However, it can also be derived from quantum mechanics, giving a value of L = 2.44 x [10.sup.-8] (W[ohm][K.sup.-2]), which is close to that of uranium, plutonium, and zirconium. Thus, we used this theoretical value of the Lorentz number in this study. For alloys form solid solution, Nordheim found that the electrical resistivity has a x(1 - x) dependence, as follows [23]:

[[rho].sub.m] = [[rho].sub.A] (1 - x)+ [[rho].sub.b]x + cx(1 - x), (5)

where [[rho].sub.m], [[rho].sub.A], and [[rho].sub.B] are the electrical resistivity of the mixture and elements A and B, x is the atomic fraction of element B, and c is the Nordheim coefficient, which is an element-dependent parameter. For example, for the Cu-Au alloy, the Nordheim coefficient of Cu-rich-Au alloys and Aurich-Cu alloys are different [24]. Thus, we treated the Nordheim coefficients of the U-rich-Zr alloy and Zr-rich-U alloy separately in this paper.

From the Wiedemann-Franz law and Nordheim's rule, the thermal conductivity is considered to have the same dependence as the electrical conductivity [25]:

[[kappa].sub.1] = 1/1 (1 - x)/[[kappa].sub.A] + x/[[kappa].sub.b] + [c.sub.1]x(1 - x)/(LT), (6)

where [[kappa].sub.1], [[kappa].sub.A], and [[kappa].sub.B] are the thermal conductivity ([Wm.sup.-1] x [K.sup.-1]) of the mixture and elements A and B, re spectively, x is the atomic fraction of element B, [c.sub.1] is the Nordheim coefficient, L is the Lorentz number, and T is the temperature. Because equation (5) only applies for binary alloys, we extended it to treat ternary alloys as a mixture of a binary alloy and third element as follows:

[[kappa].sub.2] = 1/1 (1 - x)/[[kappa].sub.1] + x/[[kappa].sub.C] + [c.sub.2]x(1 - x)/(LT) (7)

where [[kappa].sub.2], [[kappa].sub.1], and [[kappa].sub.C] are the thermal conductivity ([Wm.sup.-1]x [K.sup.-1]) of the ternary alloy, binary alloy, and third element C, respectively, and x is the atomic fraction of element C. In our estimation, elements A, B, and C were U, Zr, and Pu, respectively, to obtain the Nordheim coefficients. To obtain the thermal conductivity of Pu-Zr and Pu-U-Zr, elements A, B, and C were Pu, Zr, and U, respectively.

The thermal conductivity of U-Zr and U-Pu-Zr alloys were taken from the work of Takahashi et al. [26] and reports from the Argonne National Laboratory (ANL) [27, 28]. These values were fitted into the above equations to obtain the Nordheim coefficients c1 and c2 for U-Zr and U-Pu-Zr alloys as temperature-dependent linear functions. To derive these functions, we fitted the temperature dependences of the thermal conductivity of uranium, zirconium, and plutonium using the following equation from available data [29, 30]:

[kappa] = a + bT + [cT.sup.2] + [dT.sup.3]. (8)

Obtained fitting parameters are shown in Table 1. We obtained the thermal conductivity of Pu-Zr and Pu-U-Zr based on the assumption that their Nordheim coefficients were the same as those of U-Zr and U-Pu-Zr alloys. The Nordheim coefficients for U-Zr and U-Pu-Zr alloys are summarized in Table 2. In Figures 4 and 5, we compare the thermal conductivities obtained in the present study-using the obtained Nordheim coefficients with those of the available data [26-28]. These show relatively close to measured thermal conductivity for both U-Zr and U-Pu-Zr alloys. For the U-79Zr alloy, our correlation showed higher thermal conductivity than experimental data. However, if zirconium content is below 50 wt%, our correlation showed sufficiently agreed well. Obtained Nordheim coefficients were based on these experimental data. These experimental data were only available below 1173 K, and this is the temperature limitation in the present experiment. The Pu-40Zr alloy had a significantly lower thermal conductivity than plutonium because of the effect of zirconium addition. However, the thermal conductivity of the Pu-20U-20Zr alloy was improved and it was close to that of plutonium because of the presence of uranium (Figure 6).

2.3. Solidus and Liquidus Temperatures. Solidus and liquidus temperatures of the Pu-U-Zr alloy (Pu-(0-80U)-20Zr) were calculated by Thermo-Calc [22] by creating a pseudo-binary phase diagram. Thermo-Calc is the calculation code based on the CALPHAD method, which creates phase diagrams and phase equilibria. A description of the CALPHAD method is provided elsewhere [31]. We used the database for the calculation to create U-Zr, Pu-Zr, U-Pu, and U-Pu-Zr systems based on the most recent data of the Gibbs free energy reported by Kurata [13, 14] although the Pu-rich region is not well understood in the U-Pu-Zr system. Verification of the database provided by Kurata is performed by D. E. Janney et al. [32]. There is no experimental data of the melting points for the Pu-U-Zr alloys, and thus, experimental measurement will be mandatory. To judge whether Pu-rich metallic fuel can be used in fast reactors, the system should be evaluated. Our results are shown in Figure 7, and fitting was performed with uranium content as follows:

[T.sub.liq] (K) = 1530.5 + 385.07 x [W.sub.U] - 77.635 x [W.sup.2.sub.U], [T.sub.sol] (K) = 1321.1 + 38.449 x [W.sub.U] + 648.5 x [W.sup.2.sub.U], (9)

where [T.sub.liq] and [T.sub.sol] are the liquidus and solidus temperatures, respectively, and [W.sub.U] is the weight fraction of uranium. Accordingly, both [T.sub.liq] and [T.sub.sol] increase with increasing uranium content. We calculated [T.sub.liq] and [T.sub.sol] values of 1321.1 and 1530.5 K for the Pu-20Zr alloy which were agreed well with the Pu-Zr system [13]. We also calculated them of 1705.4 and 1788.9 K for the U-20Zr alloy. These values were slightly lower than those for the U-20Zr alloy calculated by the correlation produced by Ogata, as shown in Figure 7 [33, 34].

3. Conclusion

U-free metallic alloy fuel has important advantages for use in TRU burners. Most importantly, we showed theoretically that the thermal conductivity of the Pu-40Zr alloy was lower than that of the U-Zr alloys, which limits the core power. This addresses the metallic fuel has much lower durability in accidental situation than the U-Zr metallic fuel. To gain the safety margin, we also provided the estimation for the Purich metallic fuel with small amount of uranium addition. However, the addition of uranium to the Pu-Zr alloy increased its thermal conductivity and solidus temperature. Despite these advantages, it should be noted that uranium addition could lead to lower efficiency in TRU burners.

https://doi.org/10.1155/2019/7263721

Data Availability

No data were used to support this study.

Disclosure

Our previous work was presented in NuMat2018 at Seattle, entitled "An estimation of the thermal properties of Pu-rich metallic fuel," P1.008. This research was conducted as the Nuclear System Research and Development program under a contract with the Ministry of Education, Culture, Sports, Science and Technology (MEXT) in Japan during the fiscal year of 2014 to 2017. The title was "Innovative metallic fuel design and development of the production technology for TRU burning."

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this study.

Acknowledgments

We thank Adam Brotchie, PhD, from Edanz Group (http:// www.edanzediting.com/ac)for editing a draft of this manuscript.

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Naoya Odaira and Yuji Arita

University of Fukui, 1-3-33 Kanawa-cho, Tsuruga, Fukui 914-0055, Japan

Correspondence should be addressed to Yuji Arita; arita@u-fukui.ac.jp

Received 31 March 2019; Revised 25 July 2019; Accepted 2 August 2019; Published 4 September 2019 Guest Editor: Pradip Basnet

Caption: Figure 1: Literature data of the heat capacity of U-Zr and U, Zr, and Pu elements [15-17].

Caption: Figure 2: Phase diagram of the Pu-Zr system [21, 22].

Caption: Figure 3: Estimated heat capacity of Pu-40Zr and Pu-20U-20Zr alloys.

Caption: Figure 4: Comparison between the obtained thermal conductivity-temperature correlations (broken line) (present work) for (a) U-rich and (b) Zr-rich U-Zr alloys and the results of Takahashi et al. [26] (each point).

Caption: Figure 5: Comparison between the obtained thermal conductivity-temperature correlations (broken line) (present work) for the U-Pu-Zr alloy and data from (a) ANL-7230 (U-16.2Pu-6.2Zr, U-14.7Pu-9.7Zr, and U-18.4Pu-11.5Zr alloys (in wt%) and (b) ANL-7155 (U-15Pu-10Zr, U-18.4Pu-14.1Zr, and U-17.1Pu-3.4Zr [wt%] alloys (in wt%) [27, 28] (each point).

Caption: Figure 6: Estimated thermal conductivity of Pu-Zr and Pu-U-Zr alloys [29, 30].

Caption: Figure 7: Estimated solidus and liquidus temperatures for the PuU-20Zr alloy [33, 34].
Table 1: Fitted parameters for each element [29, 30].

      [kappa] = a + bT + c[T.sup.2] + d[T.sup.3]

               a                        b

U      3.739 x [10.sup.-6]            0.01837
Zr     2.090 x [10.sup.-5]           -0.02515
Pu    -5.288 x [10.sup.-8]     6.439 x [10.sup.-5]

          [kappa] = a + bT + c[T.sup.2]
                  + d[T.sup.3]

               c               d

U           -21.69             --
Zr           27.48             --
Pu    9.278 x [10.sup.-3]    -1.534

Table 2: Obtained Nordheim coefficients for U-Zr and U-Pu-Zr alloys.

               c = a + bT (Nordheim coefficient)

For published data                     For estimation

Zr-rich (U-Zr alloy)                Pu-40Zr (Pu-64at%Zr)
U-rich (U-Zr alloy)                          --
U-Zr-rich (U-Pu-Zr alloy)      Pu-20U-20Zr (Pu-15at%U-40at%Zr)

               c = a + bT (Nordheim coefficient)

For published data                      a

Zr-rich (U-Zr alloy)           7.985 x [10.sup.-6]
U-rich (U-Zr alloy)            1.581 x [10.sup.-6]
U-Zr-rich (U-Pu-Zr alloy)      2.747 x [10.sup.-6]

               c = a + bT (Nordheim coefficient)

For published data                      b

Zr-rich (U-Zr alloy)           -7.436 x [10.sup.-9]
U-rich (U-Zr alloy)            -1.619 x [10.sup.-9]
U-Zr-rich (U-Pu-Zr alloy)      -1.847 x [10.sup.-9]
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Title Annotation:Research Article
Author:Odaira, Naoya; Arita, Yuji
Publication:Advances in Materials Science and Engineering
Geographic Code:9JAPA
Date:Sep 30, 2019
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