Regenerative materials

Abstract: The present invention provides a regenerative material having a peak specific heat at a low temperature. The material is made of a solid solution of at least two different magnetic type metal compounds, for example, ferromagnetic Er₃Co and antiferromagnetic Er₃Ni. From these compounds, the regenerative material Er₃(Ni,Co) in solid-solution form is produced and the material has a lower magnetic phase transition point than each of the compounds. The regenerative material is utilized for a regenerator of a refrigerator.

Description: The present invention relates to a regenerative material which exhibits a large specific heat at a low temperature. In recent years, the technology of devices used in association with superconductor materials has advanced remarkably and has been applied to more and more technical fields. Along with the increasing use of superconductor technology, demands are increasing for a high-efficiency, small refrigerator for cooling superconductive components. There is a significant demand for a refrigerator which is light and small and has a high heat-efficiency. At present, such refrigerators are being developed in two ways. The first method is to enhance the efficiency of the existing gas-cycle refrigeration devices by adopting, for example, the Stirling cycle. The second method is to employ a new refrigerator in place of conventional gas-cycle refrigeration. A new refrigerator includes those using a heat-cycle, such as a Carnot-type and an Ericsson-type cycle, and the magnetocaloric effect. Among the gas-cycle refrigerators with enhanced efficiency are: refrigerators which operate using the Stirling cycle and refrigerators which operate using the Gifford-McMahorn cycle. Each refrigerator has what is termed a regenerator which is packed with what is termed regenerative material. A working medium (⁴He gas) is repeatedly passed through the regenerator to obtain a low temperature. More specifically, the working medium is first compressed and then made to flow in one direction through the regenerator. As the medium flows through the regenerator, heat energy is transferred from the medium to the regenerative material. When the medium flows out of the regenerator, it is expanded and its temperature is lowered further. The working medium is then made to flow in the opposite direction, through the regenerator again. This time heat energy is transferred from the regenerative material to the medium. The medium is passed twice, back and forth, through the regenerator in one refrigeration cycle. This cycle is repeated, thereby obtaining a low temperature. The thermal characteristics of the regenerative material (sometimes referred to as its "recuperativeness"), and most significantly its specific heat, are the determinant of the efficiency of the refrigerator. The greater the recuperativeness regenerative materials have, the higher the heat-efficiency of each refrigeration cycle. The regenerative materials used in the conventional regenerators are sintered particles of lead or mesh of copper or bronze or phosphor bronze. These regenerative materials exhibit a very small specific heat at extremely low temperatures of 20°K or less. Hence, they cannot accumulate sufficient heat energy at extremely low temperatures in each refrigeration cycle of the gas-cycle refrigerator. Nor can they supply sufficient heat energy to the working medium. Consequently, a gas-cycle refrigerator which has a regenerator filled with such regenerative materials has a low cooling efficiency. This problem can be solved by using regenerative materials which exhibit a large specific heat per unit volume (i.e., volume specific heat) at extremely low temperature. Attention has been focused on some kinds of magnetic substances as such regenerative materials because their entropies greatly change at their magnetic phase transition temperature and show an anomalous specific heat (large specific heat). Hence, a magnetic substance that has an extremely low magnetic phase transition temperature can make an excellent regenerative material. One such magnetic substance is the R-Rh intermetallic compound (where R is selected from the group consisting of: Sm, Gd, Tb, Dy, Ho, Er, Tm, and Yb). This material is disclosed in Japanese Patent Disclosure (Tokkai-sho) No. 51-52378. This group of intermetallic compounds has a maximal value of volume specific heat which is sufficiently great at 20°K or less. One of the components of this intermetallic compound is rhodium (Rh). Rhodium is a very expensive material and thus is not suitable as a regenerative material used in a regenerator where the regenerator may weigh in an amount of hundreds of grams. Another regenerative material R-Mz (where R is selected from the group consisting of: Se, Y, La, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, and M is selected from the group consisting of: Ni, Co, Cu, Ag, Au, Mn, Fe, Al, Zr, Pd, B, Si, P, C, and z has a value in the range of: 0.001 < z <9.0) has a large specific heat below 20°K and is relatively inexpensive. Such a material is disclosed in Japanese Patent Disclosure (Tokkai-hei) No. 1-310269. The regenerative material R-Mz, however, does not have sufficient specific heat at extremely low temperature (4°K-5°K). For a Helium refrigerator especially, one of the most important factors governing the refrigeration efficiency is that the regenerative material have a hig specific heat at the intended temperature of operation of the refrigerator. Accordingly, one of the objects of the present invention is to provide a regenerative material which has a maximum specific heat at low temperature. Another object of the present invention is to provide a low-temperature regenerator which is filled with the regenerative material described above. SUMMARY OF THE INVENTION According to the present invention, there is provided a regenerative material which comprises at least two metal compounds containing at least one of the rare earth elements and wherein at least two of said compounds have different magnetic interactions selected from the following such interactions : ferromagnetic, antiferromagnetic and ferrimagnetic said material being a solid solution of said compounds, the magnetic phase transition temperature of said material being lower than the magnetic phase transition temperature of each of said compounds. It is preferred that one of the metal compounds is ferromagnetic a second metal compound is anti-ferromagnetic. Most Preferably, the regenerative material comprises Er₃(Ni,Co). Another embodiment of the invention is a refrigerator including a regenerator wherein the regenerator comprises a regenerative material consisting essentially of at least two metal compounds. At least two of the compounds have different magnetic types. The material is a solid solution of the two compounds with the magnetic phase transition point of the material being lower than the magnetic phase transition point of each of the compounds. BRIEF DESCRIPTION OF THE DRAWINGS The objects and advantages of this invention will become more apparent and more readily appreciated from the following detailed description of the presently preferred embodiments of the invention taken in conjunction with the accompanying drawings wherein: Fig. 1 is a diagram showing a parallel arranged spins (J ij >o). Fig. 2 is a diagram showing an anti-parallel arranged spins (J ij <o). Fig. 3 is a diagram showing a function J (k F .R) expressing the intensities of the RKKY interaction. Fig. 4 to Fig. 9 are diagrams showing the relations between interaction values and the values of k F .R. Fig. 10 is a diagram showing relations between transition types and phase transition temperatures in R₃T, wherein: R = rare-earth element, T = Ni or Co element. Fig. 11(a) to (e) are diagrams showing the characteristics of C/T value for temperature. Fig. 12 is a phase diagram showing the composition dependence of the magnetic phase transition temperature in Er₃Ni 1-X Co X . DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention provides a regenerative material of which magnetic phase transition temperature has been lowered to values less than those of the starting substances by producing a solid-solution of two or more different magnetic metal compounds. Magnetic ions bearing the above-mentioned magnetic phase transition, for instance, include rare earth elements (Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb) ions or transition metal (Fe, Co, Ni, Mn, Cr). It is the 4f electron that creates the magnetic characteristics of these rare earth magnetic ions. However, as the 4f electron has an extremely strong locality and narrow extent of wave function, interaction among 4f electrons can be well described as an RKKY interaction with conduction electrons not as a direct interaction (direct exchange) by overlap of wave functions. Hereinafter, the interactions between the magnetic ions are described in detail. First, they are considered from the microscopic viewpoint. Assuming that total spins of local electrons belonging to one magnetic ion of the i th site as , exchange interaction between magnetic ions can be generally expressed by total spins of the i th magnetic ions, ; total spins of the i th magnetic ion, J ij ; a coefficient showing the value of exchange interaction between total spins of the i th and the j th magnetic ions). The type of interaction between spins of magnetic ions differs depending upon the plus or minus symbol of this coefficient of interaction J ij . That is, when J ij > 0, spins prefer to couple parallel each other (ferromagnetically) (see Figure 1) and when J ij < 0, spins prefer to couple anti-parallel each other (antiferromagnetically) (see Figure 2). In these figures, and are indicated with vector 1 and vector 2, respectively. However, an actual system shows more complicated interactions as it is composed of a tremendous number of magnetic ions. The sum of the coefficients of magnetic interaction between magnetic ions for the entire substance (the amount proportional to the magnetic phase transition temperature QR) J (Q) can be defined by the following formula: J (Q) = Σ Z i . J ij .e -1QR where, Q is the vector expressing the magnetic construction of a substance system and R is the vector directed to the j th magnetic ion from the i th magnetic ion. Further, if A i =Σ Z i x e -iQR , then formula (1) develops to J(Q) = A i x J i + A₂ x J₂ + A₃ x J₃ + ... Here, in a system where interaction among the magnetism bearing electron spins in the RKKY interaction, J ij (the coefficient of exchange interaction between magnetic ion spins) is a function of k F x R. k F x R is a product of distance R between i th and j th spins, and Fermi wave numbers k F . The relation between k F .R and J (k F .R) is shown in Figure 3. As seen in Figure 3, the interaction between the nearest neighbour magnetic ions is most strong in a magnetic substance. The other interactions become weaker by the screening effect of higher nearby magnetic ion interactions. By such interactions of long-range orders described by the RKKY model, different type magnetic interactions such as ferro coupling and antiferro coupling compete with each other and as a result the value of interaction becomes small and thus, magnetic phase transition temperature can be lowered. For instance, in a system where J₁ is dominant compared with J₂ and J₃, when the value of J₁ closes to the value of near equal to zero by controlling the k F .R value through an antiferromagnetic substance having (J₁>0, as shown in Figure 4) being dissolved to a ferromagnetic substance having (J₁<0, as shown in Figure 5) in a solid-solution, then the interaction becomes weak and the magnetic phase transition temperature can be lowered. Values of the interaction J between the nearest neighbor magnetic ions (indicated with number 3) and the second neighbor magnetic ions (indicated with number 4) are shown in Figures 4-6. Further, in a system where J₂ and J₃ cannot be disregarded for high order interactions compared with J₁, when systems where the J₁ value is almost 0 and J₂ and J₃ have values as shown in Figure 7 and in Figure 8 are placed in a solid-solution, then J₂ and J₃ are cancelled (as shown in Figure 9) or k F .R is controlled in a manner to cancel the entire J₁, J₂ and J₃. In these cases the interaction becomes weak and the magnetic phase transition point can be lowered. Values of the interaction J between the third neighbour magnetic ions are also indicated with number 5 in Figures 7 to 9. The following combinations can be pointed out as definite examples of the combination of at least two kinds of different magnetic type substances: 1. Er₃(Ni 1-x Co x ) A combination in a solid-solution state Er₃Co and Er₃Ni, where Er₃Co is a ferromagnetic substance having a Curie temperature (T c ) of 13°K. Er₃Ni is an antiferromagnetic substance having a Neel temperature (T N ) of 6°K. 2. (Er 3-x Ho x ) Al₂ A combination in a solid-solution state of Ho₃Al₂ and Er₃Al₂, where Ho₃Al₂ is a ferromagnetic substance of which T c is 33°K. Er₃Al₂ is a ferromagnetic substance of which T N is 9°K. 3. (Er 1-x Ho x )Al A combination in solid in a solid-solution state of HoAl and ErAl, where HoAl is a ferromagnetic substance of which T c =26°K. ErAl is an anti-ferromagnetic substance of which T N =13°K. As described above, the technology involved in the present invention is capable of marking an alloy of two or more different magnetic type substances (for instance, ferromagnetic and antiferromagnetic substances, ferromagnetic substance and ferrimagnetic substance, ferrimagnetic substance and antiferromagnetic substance, etc.). Such materials find utility as a regenerative component in a refrigerator. Such materials utilize the anomaly of a large specific heat being associated with magnetic phase transitions at low temperature, caused by having different type magnetic interactions compete with each other to lower the magnetic phase transition temperature (the temperature at which the specific heat shows a peak value) below those of the starting component materials. By controlling this the specific heat corresponding at a desired temperature of operation of a gas refrigerator can be obtained. Further, the present invention is able to provide a regenerative material with a magnetic phase transition temperature controlled to provide a large specific heat corresponding to an objective temperature of a gas refrigerator which has a refrigerating efficiency similar to Pb, that is a conventional refrigerating substance in a temperature region near 20°K. The invention also has a large specific heat associated with the above-mentioned magnetic phase transition even in a low temperature region below 10°K. If the Debye temperature of the material is less than or nearly equal to that of Pb (below about 120°K), the specific heat of the lattice is sufficiently large and similar to that of Pb in a temperature range of 10-40°K. If the energy gap between the ground state and excited state of electrons which play important role in magnetism in the material is relatively small (5°K ≦ ΔE ≦ 50°K), the specific heat shows the effect of the Schottky anomaly. Thus, a large specific heat is obtained due to the addition of the Schottky anomaly contribution to the contribution of the ordinary lattice in a temperature range of 10-40°K. The magnetic-phase transition temperature of R₃Ni system and R₃Co system (R: rare-earth element) are shown in Figure 10 three-dimensionally. It is specially noteworthy that Er₃Ni has the antiferromagnetic interaction and Er₃Co has the ferro interaction from the groups of R₃Ni system and R₃Co system. Examples Mixed powders consisting of Er 75 atom %, Ni 12.5 atom % and Co balance were prepared and melted by an arc melting furnace. The melted material was then annealed at about 700°C for 100 hours in a vacuum condition (about 10⁻³ Torr). This material is identified as example 1. Two different mixed powders were also prepared. One consisted of Er 75 atom %, Ni 6.25 atom % and Co balance, the other was Er 75 atom %, Ni 5.0 atom % and Co balance. They were also melted and annealed in the same conditions as described above. These materials comprise examples 2 and 3 respectively. Finally, three different compositions of regenerative material of Er₃ (Ni,Co) were produced. According to the X-ray diffraction pattern of each obtained material, it was confirmed that a single phase of an intermetallic compound having a crystal structure of Er₃ (Co,Ni) was formed, a pseudobinary system of two different magnetic type intermetallic compounds. The value of T c of Er₃Co is about 13°K, while the T N of Er₃Ni is about 6°K. There are peaks of specific heat for these materials correspond to these magnetic phase transition temperatures. Refrigeration occurs by the entropy exchange between the regenerative material and the working fluid, as for example, He. Therefore when the regenerative efficiency of a material is evaluated, a parameter C/T is very illustrative because the value of C/T indicates the entropy exchange directly, (C is a value of specific heat at a certain temperature, and T is a value of the temperature). The characteristics of C/T as a function of T in the case of Er₃Ni and Er₃Co is shown in Figures 11(a) and Figure 11(e) respectively. The characteristics of C/T as a function of T in the case of examples 1 to 3 are also shown in Figures 11(b), 11(c) and 11(d), respectively. These values of C/T were estimated by using the specific heat of those bulk form specimens. As shown in Figure 11(b) in the case of the material including Ni 12.5 atom % the peak position of C/T (indicated by an arrow) is obtained at a value of T of about 5.5°K. As shown in Figure 11(c) in the case of the material including Ni 6.25 atom % the peak position of C/T is obtained at a value of T about 5.7°K. As shown in Figure 11(d) in the case of the material including Ni 5.0 atom % the peak position of C/T is obtained at a value of T of about 4°K. All of these three temperatures at the peak positions are lower than the individual peak position temperatures for either Er₃Ni or Er₃Co. The materials of the present invention have larger values of C/T at lower temperatures. The C/T peak position temperature corresponds to the specific heat peak position temperature in the same regenerative material. The composition dependence of the magnetic phase transition temperature in the Er₃Ni 1-x Co x system is shown in Figure 12. As shown in Figure 12, in the region where the value of X is about 0.5 or more, preferably between about 0.65 and about 0.85 (x being the content of the element of Co) there is an area of lower transition temperature. Thus comparing with Er₃Co or Er₃Ni each, more efficient refrigeration in a lower temperature region can be provided by the present invention. As described above, according to the present invention, regenerative materials utilizing anomally of a large specific heat associated with the magnetic phase transition at low temperature may be used to provide a regenerative material made from two or more different magnetic type substances. The regenerative material, having different type magnetic interactions compete with each other and thus lower the magnetic phase transition temperature (a temperature at which specific heat shows the peak value) compared with the values of the constituent materials. Further, the material also can provide a device having a relatively large specific heat at a temperature of operation of a refrigerator lower than conventional materials that do not control the magnetic phase transition temperature in the manner of the present invention. The present invention has been described with respect to specific embodiments. However, other embodiments based on the principles of the present invention should be obvious to those of ordinary skill in the art.

Claims: A regenerative material which comprises at least two metal compounds containing at least one of the rare earth elements and wherein at least two of said compounds have different magnetic interactions selected from the following such interactions : ferromagnetic, antiferromagnetic and ferrimagnetic said material being a solid solution of said compounds, the magnetic phase transition temperature of said material being lower than the magnetic phase transition temperature of each of said compounds. Regenerative material as claimed in claim 1, which comprises Er₃(Ni,Co). Regenerative material as claimed in claim 1 or 2 which consists essentially of Er₃(Ni,Co). Regenerative material as claimed in any preceding claim which comprises Er₃(Ni 1-x Co x ), where x is 0.5 or more. Regenerative material as claimed in claim 4, wherein 0.65 ≦ x ≦ 0.85. Regenerative material as claimed in any preceding claim, having a magnetic phase transition temperature of less than 6°K. A refrigerator including a regenerator wherein said regenerator comprises a regenerative material consisting essentially of at least two metal compounds containing at least one of the rare earth elements wherein at least two of said compounds have different magnetic interactions selected from the following such interactions : ferromagnetic, antiferromagnetic and ferrimagnetic, said material being a solid solution of said compounds, the magnetic phase transition temperature of said material being lower than the magnetic phase transition temperature of each of said compounds. A refrigerator as claimed in claim 7, wherein the regenerative material comprises material as claimed in any one of claims 2 to 6. Use of regenerative material as claimed in any one of claims 1 to 6 in the construction of regenerators adapted for use in refrigerators.

Inventors: SAHASHI MASASHI C O INTELLECTU, TAKAHASHI AKIKO C O INTELLECTU, TOKAI YOICHI C O INTELLECTUAL, SAHASHI, MASASHI, C/O INTELLECTUAL PROP. DIV., TAKAHASHI, AKIKO, C/O INTELLECTUAL PROP. DIV., TOKAI, YOICHI, C/O INTELLECTUAL PROP. DIV.
Applicants: TOSHIBA KK, KABUSHIKI KAISHA TOSHIBA
Application year: 1992
Main classification: H01F1
IPC codes: H01F1