CN1236096C - Rereearth-iron base compound magnetic refrigeration material with large magnetic entropy change and preparation process thereof - Google Patents

Rereearth-iron base compound magnetic refrigeration material with large magnetic entropy change and preparation process thereof Download PDF

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CN1236096C
CN1236096C CNB031210511A CN03121051A CN1236096C CN 1236096 C CN1236096 C CN 1236096C CN B031210511 A CNB031210511 A CN B031210511A CN 03121051 A CN03121051 A CN 03121051A CN 1236096 C CN1236096 C CN 1236096C
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magnetic entropy
lafe
temperature
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CN1450190A (en
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陈远富
沈保根
王芳
胡凤霞
王光军
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Institute of Physics of CAS
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Abstract

The present invention relates to a rare earth-iron base compound magnetic refrigeration material with large magnetic entropy changes and a preparation method thereof. The chemical general formula of the rare earth-iron base compound magnetic refrigeration material is La(1-x)Rx(Fe(1-y)My)(13-z)SizXalpha, wherein R represents more than one rare-earth element or a composition; M represents more than one of Al, Co, Ga, etc. or a composition; X represents more than one of C, H, N or a composition; x is from 0 to 0.4, y is from 0 to 0.3, z is from 0 to 3.0, and alpha is from 0 to 3.0. The preparation method of the present invention comprises the following steps: La(1-x)Rx(Fe(1-y)My)(13-z)Siz and interstitial compounds La(1-x)Rx(Fe(1-y)My)(13-z)SizCalpha with low C content can be prepared by directly melting and annealing; interstitial compounds La(1-x)Rx(Fe(1-y)My)(13-z)SizCalpha with high C content can be prepared by melting, rapid quenching and annealing; master alloy powder La(1-x)Rx(Fe(1-y)My)(13-z)Siz can be further deaired, and the N, the H, the C and the compounded interstitial compounds of the La(1-x)Rx(Fe(1-y)My)(13-z)Siz can be obtained. The Curie point of the rare earth-iron base compound of the present invention can be continuously adjusted in a large range; particularly, magnetic entropy changes which are more than two times larger than that of metal Gd can be obtained near the room temperature, so the present invention is an ideal magnetic refrigeration material at the room temperature. The method has the advantages of rich raw material, simple technology, etc. The method is suitable for industrial production.

Description

Has rare earth-iron base compound magnetic cooling material of great magnetic entropy variation and preparation method thereof
Technical field
The present invention relates to a kind of magneticsubstance, particularly relate to a kind of rare earth-iron base compound magnetic cooling material and preparation method thereof with great magnetic entropy variation.
Background technology
Tradition gas compression Refrigeration Technique is widely used in all trades and professions, has formed huge industry, but it exists that refrigerating efficiency is low, energy consumption big, destroy shortcomings such as atmospheric environment.
The magnetic refrigeration, be meant with the magneticsubstance to be a kind of novel Refrigeration Technique of refrigeration working medium, its ultimate principle is (or to claim magnetic refrigerating working medium by magnetic cooling material, magnetic working medium) magnetothermal effect, promptly under isothermal condition, when magneticstrength increased (magnetization), the magnetic moment of magnetic cooling material was tending towards ordered arrangement, magnetic entropy reduces, to extraneous heat extraction; When magneticstrength weakened (demagnetization), magnetic moment was tending towards lack of alignment, and magnetic entropy increases, and magnetic refrigerating working medium absorbs heat from the external world, just can reach the refrigerating purpose.
Compare with traditional gas compression Refrigeration Technique, that the magnetic Refrigeration Technique has is energy-efficient, the little significant advantage such as in light weight of environmental protection, stable, size, is described as high-new green refrigeration technology.Magnetic Refrigeration Technique, especially room temperature magnetic refrigerating technology are because of having the very big concern that huge potential application market is subjected to domestic and international research institution and branch of industry aspect the industries such as family expenses refrigerator, domestic air conditioning, central air-conditioning, supermarket food product refrigeration system.
The magnetic heating performance of magnetic refrigerating working medium mainly comprises magnetic entropy change, adiabatic temperature variation, specific heat, thermal conductivity or the like.Wherein, magnetic entropy becomes and adiabatic temperature to change be the sign of magnetic cooling material magnetothermal effect, be easy to accurate mensuration because of magnetic entropy becomes than the adiabatic temperature variation, thereby people more are accustomed to adopting magnetic entropy to become and characterize the magnetothermal effect of magnetic cooling material.The magnetothermal effect of magnetic cooling material (magnetic entropy change, adiabatic temperature change) is one of most critical factor of restriction magnetic refrigerator refrigerating efficiency, and therefore, seeking Curie temperature becomes the domestic and international research emphasis at the magnetic cooling material that the room temperature warm area has great magnetic entropy variation.
Before 1997, rare metal Gd is the magnetic refrigerating working medium of the best in room temperature interval always.1997, the Gschneidner of U.S.'s Ames Lab, Pecharsky found Gd 5(Si xGe 1-x) 4Alloy (US5743095) has huge magnetothermal effect, becomes about 2 times that reach Gd near the magnetic entropy room temperature, and the source of the great magnetic entropy variation of this material is a primary magnetic phase change.Compare with second-order phase transition, the magnetic entropy that the material of first-order phase transition takes place becomes and often concentrates near the narrower warm area transformation temperature, thereby presents higher magnetic entropy variate.Therefore, in the process of exploring novel magnetic cooling material, seeking the little first-order phase transition material with great magnetic entropy variation that lags behind has important practical sense.
Has NaZn 13Compound has the highest 3d metal content between the rare-earth transiting group metal of type cubic structure in known rare earth intermetallic compound, and the high symmetry of its structure makes it to have superior soft magnetic performance and high saturation and magnetic intensity in addition.For rare earth-iron base NaZn 13Type cubic structure compound, since positive formation heat between rare earth and the iron, RFe 13Do not exist, need to add elements reduction formation enthalpys such as Al, Si and obtain stable phase.
The basic NaZn of a kind of rare earth iron aluminium (R-Fe-Al) of CN1065294 patent disclosure 13Compound between shaped metal, this based compound have near Curie temperature advantage such as adjustable room temperature, but what take place because of this based compound is typical secondary magnetic phase transition, and it is less that magnetic entropy becomes, and under the changes of magnetic field of 0～1.4 tesla, its magnetic entropy becomes and only is 10～14J/m 3.K, for about half of Gd.
The applicant discloses a kind of NaZn in application number is 00107446.6 patent 13Type rare-earth-iron silicon (R-Fe-Si) base intermetallic compound can obtain great magnetic entropy variation when Si content drops to a certain degree, but Curie temperature (T C) far below room temperature and can only in very little temperature range, regulate, can improve Curie temperature though improve the content of Si, with the increase of Si content, the feature of first-order phase transition fades away, the second-order phase transition feature is more and more obvious, and magnetic entropy becomes and reduces.
In sum, current material all be difficult to satisfy Curie temperature by composition change adjustable on a large scale, keep big magnetic entropy to become the basic demand of this practicability magnetic cooling material simultaneously.
Summary of the invention
The objective of the invention is to by to rare earth-iron base compound La 1-xR x(Fe 1-yM y) 13-zSi zMiddle interstitial atom or the substitute element introduced, solve that Curie temperature is continuously adjustable to keep big magnetic entropy to become this difficult problem simultaneously on a large scale, thereby it is adjustable on a large scale near room temperature to obtain a kind of Curie temperature, magnetic entropy become be better than Gd have rare earth-iron base compound magnetic cooling material of great magnetic entropy variation and preparation method thereof.
The objective of the invention is to realize by the following technical solutions:
Rare earth-iron base compound magnetic cooling material with great magnetic entropy variation provided by the invention, its chemical general formula is:
La 1-xR x(Fe 1-yM y) 13-zSi zC α
Wherein: R satisfies the arbitrary combination of the following rare earth element of x scope: Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, Y, Sc for one or more;
M satisfies the arbitrary combination of the following element of y scope: Al, Co, Be, Ga, B, Ti, V, Cr, Mn, Ni, Zr, Nb, Mo, Hf, Ta, W for one or more;
The scope of x is 0～0.4;
The scope of y is as follows:
When M was Co, Al, Ga, Be, B, Mn element, y was 0～0.3;
When M was Ti, V, Cr, Ni, Zr, Nb, Mo, Hf, Ta, W element, y was 0～0.1;
The scope of z is 0～3.0;
The scope of α is: when 0≤z≤1.5,0.2≤α≤2.8;
When 1.7≤z≤3.0,0.01≤α≤1.5.
Preparation method with gap rare earth-iron base compound magnetic cooling material of great magnetic entropy variation provided by the invention comprises the steps:
The present invention prepares La 1-xR x(Fe 1-yM y) 13-zSi zC α(α≤0.5) clearance C compound, concrete technology is:
I) press La 1-xR x(Fe 1-yM y) 13-zSi zC αThe chemical formula weighing mixes rare-earth metal La, R and Fe, Fe-C master alloy, M and Si raw material, and wherein, the excessive interpolation 1～15% of rare-earth metal La and R (atomic percent) compensates volatilization and the scaling loss in the fusion process;
Ii) with step I) raw material for preparing puts into electric arc furnace, is evacuated to 2 * 10 -5More than the torr, clean 1～2 time with common high-purity argon purging method after, adopt the usual method melting 3～6 times of under 1 atmospheric high-purity argon gas protection, overturning repeatedly, smelting temperature with fusing till;
Iii) through step I i) melted material handled 7～30 days 900～1100 ℃ of vacuum annealings, took out in quench fast liquid nitrogen or the water afterwards, can make rare earth-iron base compound La 1-xR x(Fe 1-yM y) 13-zSi zC α
When needs prepare the interstitial compound (α＞0.5) of higher C content, contain the second more phase (α-Fe) as stated above in (add Fe-C master alloy) interstitial compound that directly melting is prepared, therefore, except that by above-mentioned i)～iii) the step process, also comprise following two steps:
Iv) with above-mentioned i)～the iii) La of the high C content of step preparation 1-xR x(Fe 1-yM y) 13-zSi zC αAlloy (contains the higher second phase α-Fe), put into quick quenching furnace, is evacuated down to 2*10 -5After torr is above, charge into 1 atmospheric high-purity argon gas, under the high-purity argon gas protection, carry out routine and get rid of tape handling, the linear velocity of copper roller is 10～50m/s;
V) with step I v) the chilling fast quenching handle the strip obtain and be placed in the vacuum oven, be evacuated down to 2*10 -6More than the torr, or be extracted into 2*10 -5Charge into 1 atmospheric high-purity argon gas after the above high vacuum of torr, under 500～1200 ℃ of temperature, carry out 0.5～50 hour anneal, can obtain the interstitial compound La of the good high C content of single phase property 1-xR x(Fe 1-yM y) 13-zSi zC α
The invention has the advantages that:
The present invention has prepared a kind of rare earth-iron base compound magnetic cooling material with great magnetic entropy variation, i.e. La 1-xR x(Fe 1-yM y) 13-zSi zC αCompound, this compound Curie temperature changes adjustable continuously in 120K～360K interval on a large scale by composition, especially can obtain to be higher than the great magnetic entropy variation of Metal Gd more than 2 times near the room temperature, be a kind of very ideal room temperature magnetic refrigeration material, and its performance is as shown in table 1.
Preparation provided by the invention has the method for the rare earth-iron base compound magnetic cooling material of great magnetic entropy variation, because of employed raw material contains a large amount of relatively inexpensive Fe etc., have abundant raw materials, remarkable advantage such as with low cost, in addition, the present invention also have preparation technology simple, be suitable for advantage such as industrialized magnetic cooling material production.
Description of drawings
Fig. 1 is the LaFe of the embodiment of the invention 1 preparation 11.8Si 1.2Room temperature X-ray diffraction (XRD) spectral line;
The LaFe that Fig. 2 prepares for the embodiment of the invention of measuring on SQUID 1 13-zSi z(z=1.2,1.4,1.6) under 1.0 tesla magnetic fields pyromagnetic (curve of M～T), wherein:
"-" represents the LaFe of z=1.2 13-zSi zThermomagnetization curve;
" zero-" represents the LaFe of z=1.4 13-zSi zThermomagnetization curve;
Figure C0312105100081
Represent the LaFe of z=1.6 13-zSi zThermomagnetization curve;
Fig. 3 is the LaFe of embodiment 1 preparation 13-zSi zThe isothermal magnetization curve of (z=1.2,1.4,1.6), wherein:
Scheme a) to represent the LaFe of z=1.2 13-zSi zThe isothermal magnetization curve;
Figure b) represents the LaFe of z=1.4 13-zSi zThe isothermal magnetization curve;
Figure c) represents the LaFe of z=1.6 13-zSi zThe isothermal magnetization curve;
Fig. 4 is the LaFe of embodiment 1 preparation 13-zSi zThe isothermal magnetic entropy change～temperature of (z=1.2,1.4,1.6) (| the curve of Δ S|～T), wherein:
"-▲-" represent the LaFe of z=1.2 13-zSi zIsothermal magnetic entropy change～temperature curve;
" ■-" represents the LaFe of z=1.4 13-zSi zIsothermal magnetic entropy change～temperature curve;
"-●-" represent the LaFe of z=1.6 13-zSi zIsothermal magnetic entropy change～temperature curve;
Fig. 5 is the LaFe of embodiment 2 preparations 11.5Si 1.5H αThe room temperature XRD spectral line of (α=0,0.3,1.3,1.8), wherein:
Spectral line (a) is represented the LaFe of α=0 11.5Si 1.5H αThe XRD spectral line;
Spectral line (b) is represented the LaFe of α=0.3 11.5Si 1.5H αThe XRD spectral line;
Spectral line (c) is represented the LaFe of α=1.3 11.5Si 1.5H αThe XRD spectral line;
Spectral line (d) is represented the LaFe of α=1.8 11.5Si 1.5H αThe XRD spectral line;
Fig. 6 is the LaFe of embodiment 2 preparations 11.5Si 1.5H α(α=0,0.3,0.6,0.9,1.3,1.5,1.8) thermomagnetization curve under 100 gauss magnetic fields, wherein:
" ■-" represents the LaFe of α=0 11.5Si 1.5H αThe thermomagnetization curve of temperature-rise period;
"-●-" represent the LaFe of α=0.3 11.5Si 1.5H αThe thermomagnetization curve of temperature-rise period;
"-▲-" represent the LaFe of α=0.6 11.5Si 1.5H αThe thermomagnetization curve of temperature-rise period;
" -" represents the LaFe of α=0.9 11.5Si 1.5H αThe thermomagnetization curve of temperature-rise period;
"-◆-" represent the LaFe of α=1.3 11.5Si 1.5H αThe thermomagnetization curve of temperature-rise period;
Represent the LaFe of α=1.5 11.5Si 1.5H αThe thermomagnetization curve of temperature-rise period;
Represent the LaFe of α=1.8 11.5Si 1.5H αThe thermomagnetization curve of temperature-rise period;
Corresponding open symbols is represented the thermomagnetization curve of corresponding temperature-fall period among the figure;
Fig. 7 is the LaFe of embodiment 2 preparations 11.5Si 1.5H αNear (α=0,1.3,1.8) isothermal magnetization curve Curie temperature, wherein:
Scheme a) to represent the LaFe of α=0 11.5Si 1.5H αThe isothermal magnetization curve;
Figure b) represents the LaFe of α=1.3 11.5Si 1.5H αThe isothermal magnetization curve;
Figure c) represents the LaFe of α=1.8 11.5Si 1.5H αThe isothermal magnetization curve;
Fig. 8 is the LaFe of embodiment 2 preparations 11.5Si 1.5H αThe contrast of the isothermal magnetic entropy change～temperature curve of (α=0,0.3,0.6,0.9,1.3,1.5,1.8) and comparative example rare metal Gd, wherein:
Figure C0312105100091
Represent the LaFe of α=0 11.5Si 1.5H αIsothermal magnetic entropy change～temperature curve;
"-" represents the LaFe of α=0.3 11.5Si 1.5H αIsothermal magnetic entropy change～temperature curve;
" -" represents the LaFe of α=0.6 11.5Si 1.5H αIsothermal magnetic entropy change～temperature curve;
" zero-" represents the LaFe of α=0.9 11.5Si 1.5H αIsothermal magnetic entropy change～temperature curve;
"-◆-" represent the LaFe of α=1.3 11.5Si 1.5H αIsothermal magnetic entropy change～temperature curve;
" ◇-" represents the LaFe of α=1.5 11.5Si 1.5H αIsothermal magnetic entropy change～temperature curve;
" θ-" represents the LaFe of α=1.8 11.5Si 1.5H αIsothermal magnetic entropy change～temperature curve;
Figure C0312105100092
Represent the isothermal magnetic entropy change～temperature curve of comparative example rare metal Gd;
Fig. 9 is the La (Fe of embodiment 3 preparations 1-yMn y) 11.7Si 1.3The XRD spectral line of (y=0,0.01,0.02,0.03), wherein:
Spectral line a) is represented the La (Fe of y=0 1-yMn y) 11.7Si 1.3The XRD spectral line;
Spectral line b) represents the La (Fe of y=0.01 1-yMn y) 11.7Si 1.3The XRD spectral line;
Spectral line c) represents the La (Fe of y=0.02 1-yMn y) 11.7Si 1.3The XRD spectral line;
Spectral line d) represents the La (Fe of y=0.03 1-yMn y) 11.7Si 1.3The XRD spectral line;
Figure 10 is the La (Fe of embodiment 3 preparations 1-yMn y) 11.7Si 1.3H α(y=0,0.01,0.02,0.03, α=0 and 0.2) thermomagnetization curve under 100 gauss magnetic fields, wherein:
"-" represents y=0.03, the La (Fe of α=0 1-yMn y) 11.7Si 1.3H αThermomagnetization curve;
" ■-" represents y=0.02, the La (Fe of α=0 1-yMn y) 11.7Si 1.3H αThermomagnetization curve;
" zero-" represents y=0.01, the La (Fe of α=0 1-yMn y) 11.7Si 1.3H αThermomagnetization curve;
"-●-" represent y=0.00, the La (Fe of α=0 1-yMn y) 11.7Si 1.3H αThermomagnetization curve;
"-◆-" represent y=0.03, the La (Fe of α=2.0 1-yMn y) 11.7Si 1.3H αThermomagnetization curve;
" ◇-" represents y=0.02, the La (Fe of α=2.0 1-yMn y) 11.7Si 1.3H αThermomagnetization curve;
Figure C0312105100093
Represent y=0.01, the La (Fe of α=2.0 1-yMn y) 11.7Si 1.3H αThermomagnetization curve;
Figure 11 is the La (Fe of embodiment 3 preparations 1-yMn y) 11.7Si 1.3H αMagnetic entropy change～the temperature of (y=0,0.01,0.02,0.03, α=0 and 0.2) and comparative example rare metal Gd (| the Δ S|～T) contrast of curve, wherein:
"-" represents y=0.03, the La (Fe of α=0 1-yMn y) 11.7Si 1.3The isothermal magnetic entropy change～temperature curve of H α;
" zero-" represents y=0.02, the La (Fe of α=0 1-yMn y) 11.7Si 1.3H αIsothermal magnetic entropy change～temperature curve;
" Δ-" represents y=0.01, the La (Fe of α=0 1-yMn y) 11.7Si 1.3H αIsothermal magnetic entropy change～temperature curve;
" -" represents y=0.00, the La (Fe of α=0 1-yMn y) 11.7Si 1.3H αIsothermal magnetic entropy change～temperature curve;
Figure C0312105100101
Represent y=0.03, the La (Fe of α=2.0 1-yMn y) 11.7Si 1.3H αIsothermal magnetic entropy change～temperature curve;
Represent y=0.02, the La (Fe of α=2.0 1-yMn y) 11.7Si 1.3H αIsothermal magnetic entropy change～temperature curve;
" ◇-" represents y=0.01, the La (Fe of α=2.0 1-yMn y) 11.7Si 1.3H αIsothermal magnetic entropy change～temperature curve;
Represent the isothermal magnetic entropy change～temperature curve of comparative example rare metal Gd;
Figure 12 is the La (Fe of embodiment 4 preparations 1-yCo y) 11.9Si 1.1(y=0.04,0.06,0.08) thermomagnetization curve under 100 gauss magnetic fields, wherein:
A) represent the La (Fe of y=0.04 1-yCo y) 11.9Si 1.1Thermomagnetization curve;
B) represent the La (Fe of y=0.06 1-yCo y) 11.9Si 1.1Thermomagnetization curve;
C) represent the La (Fe of y=0.08 1-yCo y) 11.9Si 1.1Thermomagnetization curve;
" ●-" represents the data point of temperature-rise period among the figure;
" zero-" represents the data point of temperature-fall period;
Figure 13 is the La (Fe of embodiment 4 preparations 1-yCo y) 11.9Si 1.1Magnetic entropy change～the temperature of (y=0.04,0.06,0.08) and comparative example rare metal Gd (| the Δ S|～T) contrast of curve, wherein:
" ■-" represents the La (Fe of y=0.04 1-yCo y) 11.9Si 1.1Isothermal magnetic entropy change～temperature curve;
"-●-" represent the La (Fe of y=0.06 1-yCo y) 11.9Si 1.1Isothermal magnetic entropy change～temperature curve;
"-▲-" represent the La (Fe of y=0.08 1-yCo y) 11.9Si 1.1Isothermal magnetic entropy change～temperature curve;
Represent the isothermal magnetic entropy change～temperature curve of comparative example rare metal Gd;
Figure 14 is the La (Fe of embodiment 5 preparations 1-yM y) 13-zSi zMagnetic entropy change～the temperature of (M is respectively Co, Al and combination) and comparative example rare metal Gd (| the Δ S|～T) contrast of curve, wherein:
"-" represents y=0, the La (Fe of z=1.17 1-yM y) 13-zSi zIsothermal magnetic entropy change～temperature curve;
" ■-" represents M is Al, y=0.0194, the La (Fe of z=0.936 1-yM y) 13-zSi zIsothermal magnetic entropy change～temperature curve;
" zero-" represents M is Co, y=0.0676, the La (Fe of z=1.17 1-yM y) 13-zSi zIsothermal magnetic entropy change～temperature curve;
"-●-" to represent M be Co: Al=3.42, y=0.0864, the La (Fe of z=0.936 1-yM y) 13-zSi zIsothermal magnetic entropy change～temperature curve;
" ◇-" represents M is Co: Al=1.71, y=0.1031, the La (Fe of z=0.702 1-yM y) 13-zSi zIsothermal magnetic entropy change～temperature curve;
"-◆-" to represent M be Co: Al=1.14, y=0.1199, the La (Fe of z=0.468 1-yM y) 13-zSi zIsothermal magnetic entropy change～temperature curve;
Representing M is Co: Al=0.72, y=0.172, the La (Fe of z=0 1-yM y) 13-zSi zIsothermal magnetic entropy change～temperature curve;
Figure C0312105100112
Represent the isothermal magnetic entropy change～temperature curve of comparative example rare metal Gd;
Figure 15 is the LaFe of embodiment 6 preparations 11.6Si 1.4C αThe room temperature XRD spectral line of (α=0,0.2,0.4,0.6), wherein:
Spectral line a) is represented the LaFe of α=0 11.6Si 1.4C αThe XRD spectral line;
Spectral line b) represents the LaFe of α=0.2 11.6Si 1.4C αThe XRD spectral line;
Spectral line c) represents the LaFe of α=0.4 11.6Si 1.4C αThe XRD spectral line;
Spectral line d) represents the LaFe of α=0.6 11.6Si 1.4C αThe XRD spectral line;
Figure 16 is the LaFe of embodiment 6 preparations 11.6Si 1.4C α(α=0,0.2,0.4,0.6) thermomagnetization curve under 100 gauss magnetic fields, wherein:
" ■-" represents the LaFe of α=0 11.6Si 1.4C αThermomagnetization curve;
"-" represents the LaFe of α=0.2 11.6Si 1.4C αThermomagnetization curve;
"-●-" represent the LaFe of α=0.4 11.6Si 1.4C αThermomagnetization curve;
" zero-" represents the LaFe of α=0.6 11.6Si 1.4C αThermomagnetization curve;
Figure 17 is the LaFe of embodiment 6 preparations 13-zSi zC αMagnetic entropy change～the temperature of (z=1.4 and 1.5, α=0～0.6) and comparative example rare metal Gd (| the Δ S|～T) contrast of curve, wherein:
"-" represents z=1.4, the LaFe of α=0 1.3-zSi zC αIsothermal magnetic entropy change～temperature curve;
" zero-" represents z=1.4, the LaFe of α=0.2 1.3-zSi zC αIsothermal magnetic entropy change～temperature curve;
" △-" represents z=1.4, the LaFe of α=0.4 1.3-zSi zC αIsothermal magnetic entropy change～temperature curve;
" -" represents z=1.4, the LaFe of α=0.6 1.3-zSi zC αIsothermal magnetic entropy change～temperature curve;
"-◆-" represent z=1.5, the LaFe of α=0 1.3-zSi zC αIsothermal magnetic entropy change～temperature curve;
" -" represents z=1.5, the LaFe of α=0.2 1.3-zSi zC αIsothermal magnetic entropy change～temperature curve;
" -" represents z=1.5, the LaFe of α=0.5 1.3-zSi zC αIsothermal magnetic entropy change～temperature curve;
Figure C0312105100113
Represent the isothermal magnetic entropy change～temperature curve of comparative example rare metal Gd;
Figure 18 is the LaFe of embodiment 7 preparations 11.7Si 1.3N 0.2The isothermal magnetic entropy change～temperature curve of interstitial compound, wherein:
"-●-" represent the LaFe of 0～1T 11.7Si 1.3N 0.2The isothermal magnetic entropy change～temperature curve of interstitial compound;
" zero-" represents the LaFe of 0～2T 11.7Si 1.3N 0.2The isothermal magnetic entropy change～temperature curve of interstitial compound;
"-▲-" represent the LaFe of 0～3T 11.7Si 1.3N 0.2The isothermal magnetic entropy change～temperature curve of interstitial compound;
" ■-" represents the LaFe of 0～4T 11.7Si 1.3N 0.2The isothermal magnetic entropy change～temperature curve of interstitial compound;
"-" represents the LaFe of 0～5T 11.7Si 1.3N 0.2The isothermal magnetic entropy change～temperature curve of interstitial compound.
Embodiment
Embodiment 1 preparation LaFe 13-zSi z(z=1.2,1.4,1.6)
Prepare LaFe by chemical formula 13-zSi z(z=1.2,1.4,1.6) compound, concrete technology is:
I) press LaFe 13-zSi z(z=1.2,1.4,1.6) chemical formula weighing is higher than 99.9% commercially available rare-earth metal La, R, Fe, M and the mixing of Si raw material, wherein La excessive 10% (atomic percent) compensation volatilization and scaling loss with purity;
Ii) with step I) raw material for preparing puts into electric arc furnace, is evacuated to 2 * 10 -5More than the torr, clean 1～2 time with common high-purity argon purging method after, adopt the usual method melting 3 times of under 1 atmospheric high-purity argon gas protection, overturning repeatedly, smelting temperature with fusing till;
Iii) cooling obtains cast alloy in copper crucible; Cast alloy is wrapped with molybdenum foil, be sealed in the vitreosil pipe, in 1050 ℃ of anneal are quenched liquid nitrogen after 2 weeks, obtain this based compound sample.
Measured room temperature X-ray diffraction (XRD) spectral line of all samples, the result shows and is NaZn 13Cubic crystal structure.Fig. 1 illustrates compound L aFe 11.8Si 1.2Room temperature XRD spectral line.
Go up the present embodiment compound L aFe that measures at superconducting quantum magnetometer (SQUID) 13-zSi zPyromagnetic (curve of M～T) as shown in Figure 2, can be determined Curie temperature T from M～T curve C, for z=1.2,1.4,1.6, T CBe respectively 190,200,206K.
Measuring near the isothermal magnetization curve of this interstitial compound Curie temperature as shown in Figure 3 on the SQUID.According to Maxwell relations: ( ∂ S ( T , H ) ∂ H ) T = ( ∂ M ( T , H ) ∂ T ) H , Can become from isothermal magnetization curve calculation magnetic entropy.
The compound L aFe of present embodiment preparation 13-zSi z(z=1.2,1.4,1.6) are at T separately CNear magnetic entropy change～temperature (| the curve of Δ S|～T) as shown in Figure 4, as we know from the figure: for z=1.2,1.4,1.6, at T separately CThe place very large magnetic entropy occurred and has become, and under 0～5T changes of magnetic field, maximum magnetic entropy variable is respectively 29.2,24.7,18.7J/kg.K.Can also see from Fig. 4: pass through the variation of z (Si content) merely, for T CThe amplitude of accommodation limited, and with the increase of z (Si content), magnetic entropy becomes and to reduce significantly.
The comparative example rare metal Gd
Select typical room temperature magnetic refrigeration material for use---99.9% rare metal Gd is as a comparative example.Recording its Curie temperature on SQUID is 293K, and under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 9.75J/kg.K.
Embodiment 2 preparation LaFe 11.5Si 1.5H α(α=0,0.3,0.6,0.9,1.3,1.5,1.8)
At first, press the prepared LaFe of embodiment 1 11.5Si 1.5Mother alloy further prepares its gap hydride then: the mother alloy fine grained chippings is put into autoclave, with the high-purity H of 5MPa 2Be enclosed in the autoclave.Keep inhaling H at 150 ℃ 2Time is 2 hours, obtains the saturated hydride LaFe of α=1.8 11.5Si 1.5H 1.8, under 250 ℃ of conditions, dehydrogenase 34 is 0,30,20,10 and 5 minutes in the vitreosil pipe, obtains α=0.3,0.6 respectively, 0.9,1.3,1.5 gap hydride then.
This embodiment compound L aFe 11.5Si 1.5H αThe room temperature XRD spectral line of (α=0,0.3,1.3,1.8) as shown in Figure 5.As seen from the figure: i) and LaFe 11.5Si 1.5H α(α=0) mother alloy is the same, gap hydride LaFe 11.5Si 1.5H α(α=0.3,1.3,1.8) all keep a cube NaZn 13The type structure, and single phase property is very good; Ii) the lattice parameter a of interstitial compound :～11.483 (α=0.3) ,～11.528 (α=1.3) and～11.602 (α=1.8), lattice parameter increases with the increase of α (H content) is dull, improve～0.07% than mother alloy (～11.475 ) respectively,～0.46% ,～1.11%.
This embodiment compound L aFe 11.5Si 1.5H αThe thermomagnetization curve of (α=0,0.3,0.6,0.9,1.3,1.5,1.8) as shown in Figure 6.As seen from the figure: with LaFe 11.5Si 1.5H α(α=0) mother alloy (T C=195K) compare, the Curie temperature of each gap hydride is respectively～224K (α=0.3) ,～257K (α=0.6) ,～272K (α=0.9) ,～288K (α=1.3) ,～312K (α=1.5) and～341K (α=1.8), obviously, T CThe dull rising with the increase of α (H content).
This embodiment compound L aFe 11.5Si 1.5H α(α=0,1.3,1.8) the isothermal magnetization curve as shown in Figure 7.As seen from the figure, compare with mother alloy, the magnetic field of gap hydrogen compound lags behind very little.Therefore can think LaFe basically 11.5Si 1.5H αInterstitial compound is a reversible to magnetic field, and this is extremely important for the magnetic cooling material as practicability.Concern according to Maxwell: ΔS ( T , H ) = - ∫ 0 H ( ∂ M / ∂ T ) H dH , The isothermal magnetic entropy that can calculate respectively separately becomes | Δ S|.Fig. 8 has provided LaFe 11.5Si 1.5H αCompound temperature magnetic entropy becomes a temperature curve and contrasts with Gd.As seen from the figure: under 0～5T magnetic field, LaFe 11.5Si 1.5H αBe respectively at the maximum magnetic entropy variable at Curie temperature place separately: 24.6J/kg.K (α=0), 17.4J/kg.K (α=0.3), 17.8J/kg.K (α=0.6), (16.9J/kg.K α=0.9), (17.0J/kg.K α=1.3), (16.5J/kg.K α=1.5), (20.5J/kg.K α=1.8), and rare metal Gd is 9.75J/kg.K at the maximum magnetic entropy variable of TC.Near room temperature, LaFe 11.5Si 1.5H αMagnetic entropy than Gd becomes raising 70～110%.
Embodiment 3 preparation La (Fe 1-yMn y) 11.7Si 1.3H α(y=0～0.03, α=0,2.0)
Press embodiment 2 preparation La (Fe 1-yMn y) 11.7Si 1.3H α(y=0～0.03, α=0,2.0) compound, wherein the excessive interpolation 10% of Mn (atomic percent) is with volatilization and scaling loss in the compensation fusion process.
Fig. 9 shows La (Fe 1-yMn y) 11.7Si 1.3The room temperature XRD spectral line of sample, as shown.As seen from the figure: i) and LaFe 11.7Si 1.3Mother alloy is the same, La (Fe 1-xMn x) 11.7Si 1.3(y=0.01,0.02,0.03) all is a cube NaZn 13The type structure for y=0.02 and 0.03, a spot of α-Fe occurred; Ii) micro-Mn substitutes Fe's, makes lattice parameter increase slightly, and this mainly is because the atomic radius of Mn is slightly higher than due to the atomic radius of Fe.
Figure 10 shows under 100 Gauss's conditions, compound L a (Fe 1-yMn y) 11.7Si 1.3H αThe thermomagnetization curve of (y=0～0.03, α=0,2.0).As seen from the figure: i) Mn substitutes the trace of Fe, causes T CReduce significantly, with mother alloy LaFe 11.7Si 1.3(T C=190K) compare La (Fe 0.99Mn 0.01) 11.7Si 1.3, La (Fe 0.98Mn 0.02) 11.7Si 1.3And La (Fe 0.97Mn 0.03) 11.7Si 1.3Curie temperature be respectively 166K, 151K and 127K, obviously, T CThe dull decline with the increase of Mn content; After ii) introducing the gap hydrogen atom, La (Fe 1-yMn y) 11.7Si 1.3H 2.0Curie's temperature of compound has obtained to increase significantly, and Curie reaches 331K (y=0.01), 316K (y=0.02), 295K (y=0.02) respectively, and amplification reaches 165K (y=0.01), 165 (y=0.02), 168K (y=0.03) respectively; Iii) the trace of Fe is substituted, and the introducing interstitial atom makes T by Mn CCan be adjustable on a large scale at bigger warm area (being higher than 200K).
Figure 11 has provided La (Fe 1-yMn y) 11.7Si 1.3H αThe isothermal magnetic entropy of (y=0～0.03, α=0,2.0) becomes the contrast with Gd.As seen from the figure: at～120K in～330K warm area scope, La (Fe 1-yMn y) 11.7Si 1.3H αMagnetic entropy become and all to reach or be higher than 2 times of Gd.
Embodiment 4 preparation La (Fe 1-yCo y) 11.9Si 1.1(y=0.04,0.06,0.08)
Press the prepared compound L a (Fe of embodiment 1 1-yCo y) 11.9Si 1.1(y=0.04,0.06,0.08).
Under 100 gauss magnetic fields, measured thermomagnetization curve, as shown in figure 12.As seen from the figure: Curie temperature is respectively 243 (y=0.04), 274 (y=0.06), and 301K (y=0.08), promptly along with the increase of Co content, Curie temperature increases considerably.
Figure 13 has provided under 0～5 tesla's changes of magnetic field, La (Fe 1-yCo y) 11.9Si 1.1The isothermal magnetic entropy of (y=0.04,0.06,0.08) becomes the contrast with Gd.As seen from the figure: near room temperature, the magnetic entropy of this based compound becomes and all to reach or be higher than 2 times of Gd.
Embodiment 5 preparation La (Fe 1-yM y) 13-zSi z(M is respectively Co, Al and combination, y=0.0676～0.194, z=0～1.17)
Prepared compound L a (Fe by embodiment 1 1-yM y) 13-zSi z(M is respectively Co, Al and combination, y=0.0676～0.194, z=0～1.17).Under 0～5 tesla's changes of magnetic field, its isothermal magnetic entropy become with Gd more as shown in figure 14.As seen from the figure: by Al, Co and combination thereof, we can be easily be adjusted to Curie temperature more than the room temperature from～190K, and magnetic entropy becomes and all reaches or be higher than more than 2 times of Gd.
Embodiment 6 preparation LaFe 13-zSi zC α(z=1.4,1.5, α=0～0.6)
Adopt adding direct melting of Fe-C master alloy and anneal to get final product, concrete technology is with embodiment 1.
Figure 15 has provided compound L aFe 11.6Si 1.4C αThe room temperature XRD spectral line of (α=0,0.2,0.4,0.6).As seen from the figure: i) crystalline structure of interstitial carbon compound is consistent with the crystalline structure of mother alloy, is a cube NaZn 13The type structure, but with the increase of C content, a spot of second phase α-Fe has appearred; Ii) along with the increase of C content, corresponding diffraction peak is obviously to the skew of low angular region, and promptly dullness increases lattice parameter with the increase of C content.
Measuring compound L aFe under 100 gauss magnetic fields on the SQUID 11.6Si 1.4C αThe thermomagnetization curve of (α=0,0.2,0.4,0.6), as shown in figure 17.From scheming as seen:, make the crossover of Fe-3d wave function reduce, thereby caused the rising of Curie temperature, with mother alloy LaFe because the introducing of clearance C atom has caused tangible lattice dilatation 11.6Si 1.4(T C=195K) compare LaFe 11.6Si 1.4C αCurie temperature is respectively 218.6K (α=0.2), 237K (α=0.4) and 248K (α=0.6), obviously, and T CThe dull rising with the increase of C content.
Figure 18 has provided under 0～5 tesla's changes of magnetic field, LaFe 13-zSi zC αThe isothermal magnetic entropy of (z=1.4,1.5, α=0～0.6) becomes the contrast with the comparative example rare metal Gd.As seen from the figure: the magnetic entropy of this based compound becomes and all reaches or be higher than 2 times of Gd.
Embodiment 7 preparation LaFe 11.7Si 1.3N 0.2
The LaFe that melts out by the technology of embodiment 1 11.7Si 1.3Alloy is worn into the following powder of 30 μ m; Place common high pressure vessel; At room temperature, in high pressure vessel, feed 0.15MPa mobile high-purity N 2, flow is 0.2 liter of per second, keeping inhaling the nitrogen time at 650 ℃ is 15 minutes, obtains LaFe 11.7Si 1.3N 0.2Interstitial compound.
The LaFe of embodiment 7 preparations 11.7Si 1.3N 0.2Near Curie temperature isothermal magnetization curve as shown in figure 18.
The LaFe of Figure 19 for calculating according to Figure 18 11.7Si 1.3N 0.2The isothermal magnetic entropy change～temperature curve of interstitial compound.From scheming as seen: LaFe 11.7Si 1.3N 0.2Interstitial compound Curie temperature T CBe 208K, than the LaFe of embodiment 3 11.7Si 1.3Mother alloy (T CBe 190K) raising 18K; Under 0～5T foreign field changed, the magnetic entropy change at the Curie temperature place reached 15.47J/kg.K, is 1.587 times of Gd (9.75J/kg.K).
Embodiment 8 preparation La 0.9Gd 0.1(Fe 0.7Co 0.2Mn 0.1) 11.6Si 1.4H 0.8
Press the prepared La of embodiment 2 0.9Gd 0.1(Fe 0.7Co 0.2Mn 0.1) 11.6Si 1.4H 0.8, wherein, H in the high pressure vessel 2Pressure is 5.5MPa, and inhaling the hydrogen time is 1.5 hours.
The La of present embodiment preparation 0.9Gd 0.1(Fe 0.7Co 0.2Mn 0.1) 11.6Si 1.4H 0.8Curie temperature be 290K, under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 18.5J/kg.K.
Embodiment 9 preparation La 0.9Ce 0.1(Fe 0.9Nb 0.1) 11.6Si 1.4H 0.5N 0.5
Press the prepared La of embodiment 7 0.9Ce 0.1(Fe 0.9Nb 0.1) 11.6Si 1.4H 0.5N 0.5Interstitial compound feeds high-purity H 2, N 2Mixed flow atmosphere, H 2, N 2Volume ratio is 1: 1, and pressure 0.20MPa, flow are 0.2 liter of per second, 250 ℃ air-breathing 1 hour, obtain La 0.9Ce 0.1(Fe 0.9Nb 0.1) 11.6Si 1.4H 0.5N 0.5Interstitial compound.
The La of present embodiment preparation 0.9Ce 0.1(Fe 0.9Nb 0.1) 11.6Si 1.4H 0.5N 0.5Curie temperature be 277K, under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 17.8J/kg.K.
Embodiment 10 preparation La 0.9Dy 0.067Nd 0.033(Fe 0.85Al 0.15) 13.0C 0.5
Press the prepared La of embodiment 6 0.9Dy 0.067Nd 0.033(Fe 0.85Al 0.15) 13.0C 0.5Interstitial compound feeds high-purity CH 4The atmosphere that flows, pressure 0.18MPa, flow are 0.8 liter of per second, 450 ℃ air-breathing 1 hour, obtain La 0.9Dy 0.067Nd 0.033(Fe 0.85Al 0.15) 13.0C 0.5Interstitial compound.
The La of present embodiment preparation 0.9Dy 0.067Nd 0.033(Fe 0.85Al 0.15) 13.0C 0.5The Curie temperature of interstitial compound is 248K, and under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 9.9J/kg.K.
Embodiment 11 preparation La 0.95Yb 0.025Lu 0.025(Fe 0.90Ga 0.02Co 0.08) 11.9Si 1.1H 3.0
Press the prepared La of embodiment 2 0.95Gd 0.05(Fe 0.90Ga 0.02Co 0.08) 11.9Si 1.1H 3.0, wherein, H in the autoclave 2Pressure be 4.8MPa, inhaling the hydrogen temperature is 100 ℃, inhaling the hydrogen time is 5 hours.
The La of present embodiment preparation 0.95Gd 0.05(Fe 0.90Ga 0.02Co 0.08) 11.9Si 1.1H 3.0Curie temperature be 350K, under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 14.8J/kg.K.
Embodiment 12 preparation La (Fe 0.95Co 0.05) 10.0Si 3.0C 0.01
Press the prepared La (Fe of embodiment 6 0.95Co 0.05) 10.0Si 3.0C 0.01Interstitial compound.
La (the Fe of present embodiment preparation 0.95Co 0.05) 10.0Si 3.0C 0.01Curie temperature be 267K, under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 10.7J/kg.K.
Embodiment 13 preparation LaFe 11.6Si 1.4N 0.60C 0.2
Press the prepared LaFe of embodiment 1 11.6Si 1.4Mother alloy is made the following powder of 30 μ m then, places autoclave; Under 680 ℃ of conditions, with 1MPa, N 2: CH 4=3: 1 high-purity gas is enclosed in the autoclave, air-breathing 30 minutes, obtains LaFe 11.6Si 1.4N 0.60C 0.2Interstitial compound.
The gap N of present embodiment preparation, the Curie temperature of Cization thing are 268K, and under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 13.5J/kg.K.
Embodiment 14 preparation La (Fe 0.7Al 0.3) 13
Melting technology by embodiment 1 is carried out melting, and annealing conditions is: quench after 950 ℃ of 2 weeks of insulation in the liquid nitrogen, can obtain the present embodiment sample.Its Curie temperature is 235K, and under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 7.8J/kg.K.
Embodiment 15 preparation La 0.9Sm 0.1(Fe 0.93Be 0.07) 11.2Si 1.8N 0.8
Press the prepared La of embodiment 1 0.9Sm 0.1(Fe 0.93Be 0.07) 11.2Si 1.8Mother alloy.
Under 680 ℃ condition, the high purity nitrogen of 1MPa is enclosed in the autoclave, inhaled nitrogen 50 minutes at 680 ℃, obtain La 0.9Sm 0.1(Fe 0.93Be 0.07) 11.2Si 1.8N 0.8Interstitial compound.
The La of present embodiment preparation 0.9Sm 0.1(Fe 0.93Be 0.07) 11.2Si 1.8N 0.8Curie temperature be 265K, under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 10.3J/kg.K.
Embodiment 16 preparation La 0.9Tb 0.067Sc 0.033(Fe 0.95Ti 0.05) 11.7Si 2.0H 0.75C 0.25
Press embodiment 1 preparation La 0.9Tb 0.067Sc 0.033(Fe 0.95Ti 0.05) 11.7Si 2.0Mother alloy is made the following powder of 30 μ m then, places autoclave; Under 280 ℃ of conditions, with 1.5MPa, H 2: CH 4=3: 1 high-purity gas is enclosed in the autoclave, air-breathing 35 minutes, obtains La 0.9Tb 0.067Sc 0.033(Fe 0.95Ti 0.05) 11.7Si 2.0H 0.75C 0.25Interstitial compound.
The La of present embodiment preparation 0.9Tb 0.067Sc 0.033(Fe 0.95Ti 0.05) 11.7Si 2.0H 0.75C 0.25Curie temperature be 269K, under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 12.7J/kg.K.
Embodiment 17 preparation La 0.6Pr 0.4(Fe 0.94B 0.04V 0.02) 10.9Si 2.1H 1.2
Press embodiment 2 preparation La 0.6Pr 0.4(Fe 0.94B 0.04V 0.02) 10.9Si 2.1H 1.2, wherein inhaling the hydrogen time is 50 minutes.
The La of present embodiment preparation 0.6Pr 0.4(Fe 0.94B 0.04V 0.02) 10.9Si 2.1H 1.2Curie temperature be 285K, under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 10.40J/kg.K.
Embodiment 18 preparation La 0.9Y 0.1(Fe 0.9Cr 0.1) 11.7Si 1.3N 1.5
Press embodiment 7 preparation La 0.9Y 0.1(Fe 0.9Cr 0.1) 11.7Si 1.3N 1.5, wherein inhaling the nitrogen temperature is 700 ℃, inhaling the nitrogen time is 1.5 hours.
The Curie temperature of the compound of present embodiment preparation is 250K, and under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 12.1J/kg.K.
Embodiment 19 preparation La (Fe 0.7Al 0.3) 13H 3.0
Press the prepared present embodiment sample of embodiment 2.Its Curie temperature is 360K, and under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 8.0J/kg.K.
Embodiment 20 preparation La 0.9Er 0.1Fe 11.7Si 1.3C 2.8
Press the prepared La of embodiment 1 0.9Pr 0.1Fe 11.7Si 1.3C 2.8Mother alloy.Because of this mother alloy contains more α-Fe phase, therefore, must carry out fast quenching and handle: this mother alloy be put into quick quenching furnace, be evacuated down to 2*10 -5After torr is above, charge into 1 atmospheric high-purity argon gas, carry out routine and get rid of tape handling, the linear velocity of copper roller is 50m/s; The strip that gets rid of the band preparation is placed in the vacuum oven, is evacuated down to 2*10 -6Torr carries out 10 hours anneal under 1050 ℃ of temperature, can obtain the good La of single phase property 0.9Pr 0.1Fe 11.7Si 1.3C 2.8Interstitial compound.
The La of present embodiment preparation 0.9Pr 0.1Fe 11.7Si 1.3C 2.8Curie temperature be 350K, under 0～5T changes of magnetic field, the magnetic entropy at the Curie temperature place becomes 9.9J/kg.K.
The present invention has prepared a series of rare earth-iron base compound magnetic cooling materials with great magnetic entropy variation, and its composition, technology and performance are listed in table 1.
Table 1 La 1-xR x(Fe 1-yM y) 13-zSi zX αThe composition of compound and fundamental property are relatively
Embodiment is numbered R x M y z X α T C K 0～5T magnetic entropy becomes | Δ S| J/kg.K
Comparative example Gd - - - - - - 293 9.75
1 - - - 0 0 0 - - - 0 0 0 1.6 1.4 1.2 - - - 0 0 0 190 200 206 29.2 24.7 18.7
2 - - - - - - - 0 0 0 0 0 0 0 - - - - - - - 0 0 0 0 0 0 0 0 1.5 1.5 1.5 1.5 1.5 1.5 - - - H 2Provide H--- 0 0.3 0.6 0.9 1.2 1.5 1.8 195 224 257 272 288 312 341 24.6 17.4 17.8 16.9 17.0 16.5 20.5
3 - - - - - - - 0 0 0 0 0 0 0 Mn Mn Mn Mn Mn Mn 0 0.01 0.02 0.03 0.01 0.02 0.03 1.3 1.3 1.3 1.3 1.3 1.3 1.3 - - - - H 2H is provided H 2H is provided H 2H is provided 0 0 0 0 2.0 2.0 2.0 193 166 151 127 336 312 287 26.0 25.7 20.8 17.1 23.4 17.7 15.8
4 - - - 0 0 0 Co Co Co 0.04 0.06 0.08 1.1 1.1 1.1 - - - 0 0 0 243 274 301 23.0 19.7 15.6
5 - - - - - - - 0 0 0 0 0 0 0 Al Co Co∶Al＝3.42 Co∶Al＝1.71 Co∶Al＝1.14 Co∶Al＝0.72 0 0.0194 0.0676 0.0864 0.1031 0.1199 0.172 1.17 0.936 1.17 0.936 0.702 0.468 0 - - - - - - - 0 0 0 0 0 0 0 175 170 276 278 280 290 307.5 35(18 *) 23(17.5 *) 18.5 16.5 14.5 9.0 8.5
6 - - - - - 0 0 0 0 0 - - - - - 0 0 0 0 0 1.4 1.4 1.4 1.5 1.5 Fe-C provides C Fe-C to provide C Fe-C to provide C Fe-C to provide C Fe-C that C is provided 0.2 0.4 0.6 0.2 0.5 218 238 250 229 251 24.2 18.8 12.1 22.9 12.7
7 - 0 - 0 1.3 N 2N is provided 0.2 208 15.5
8 Gd 0.1 Co∶Mn＝2 0.30 1.4 H 2H is provided 0.8 290 18.5
9 Ce 0.1 Nb 0.1 1.4 H 2∶N 2=1: 1 provides HN 1.0 277 17.8
10 Dy∶Nd＝2 0.1 Al 0.15 0 CH 4C is provided 0.5 248 9.9
11 Yb∶Lu＝1 0.05 Ga∶Co＝0.25 0.10 1.1 H 2H is provided 3.0 350 14.8
12 - 0 Co 0.05 3.0 Fe-C provides C 0.01 267 10.7
13 - 0 - 0 1.4 N 2∶CH 4Provide N, C at=3: 1 0.8 268 13.5
14 - 0 Al 0.30 0 - 0 235 7.8
15 Sm 0.1 Be 0.07 1.8 N 2N is provided 0.8 265 10.3
16 Tb∶Sc＝2 0.1 Ti 0.05 2.0 H 2∶CH 4Provide H, C at=3: 1 1.0 269 12.7
17 Pr 0.4 B∶V＝2 0.06 2.1 H 2H is provided 1.2 285 10.4
18 Y 0.1 Cr 0.1 1.7 N 2N is provided 1.5 250 12.1
19 - 0 Al 0.3 0 H 2H is provided 3.0 360 8.0
20 Er 0.1 - 0 1.3 Fe-C provides C 2.8 350 9.9
Annotate: *Corresponding data is the data (seeing for details among the figure) of approximate platform

Claims (3)

1. the rare earth-iron base compound magnetic cooling material with great magnetic entropy variation is characterized in that its chemical general formula is: La 1-xR x(Fe 1-yM y) 13-zSi zC α
Wherein: R satisfies the arbitrary combination of the following rare earth element of x scope: Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, Y, Sc for one or more;
M satisfies the arbitrary combination of the following element of y scope: Al, Co, Be, Ga, B, Ti, V, Cr, Mn, Ni, Zr, Nb, Mo, Hf, Ta, W for one or more;
The scope of x is 0～0.4;
The scope of y is as follows:
When M was Co, Al, Ga, Be, B, Mn element, y was 0～0.3;
When M was Ti, V, Cr, Ni, Zr, Nb, Mo, Hf, Ta, W element, y was 0～0.1;
The scope of z is 0～3.0;
The scope of α is: when 0≤z≤1.5,0.2≤α≤2.8;
When 1.7≤z≤3.0,0.01≤α≤1.5.
2. the described preparation method with rare earth-iron base compound magnetic cooling material of great magnetic entropy variation of claim 1 is characterized in that comprising the steps:
I) press La 1-xR x(Fe 1-yM y) 13-zSi zC αThe chemical formula weighing mixes rare-earth metal La, R and Fe, Fe-C master alloy, M and Si raw material; Wherein, excessive interpolation 1～15% atomic percent of rare-earth metal La and R;
Ii) with step I) raw material for preparing puts into electric arc furnace, is evacuated to 2 * 10 -5More than the torr, clean 1～2 time with common high-purity argon purging method after, adopt the usual method melting 3～6 times of under 1 atmospheric high-purity argon gas protection, overturning repeatedly, smelting temperature with fusing till;
Iii) through step I i) melted material handled 7～30 days 900～1100 ℃ of vacuum annealings, took out in quench fast liquid nitrogen or the water afterwards, prepared the La of rare earth-iron base compound C content α≤0.5 1-xR x(Fe 1-yM y) 13-zSi zC αInterstitial compound.
3. by the described preparation method of claim 2, it is characterized in that also comprising the steps: with rare earth-iron base compound magnetic cooling material of great magnetic entropy variation
1) with the i in the claim 2)～the iii) La of the high C content of step preparation 1-xR x(Fe 1-yM y) 13-zSi zC αAlloy is put into quick quenching furnace, in quick quenching furnace, carries out common chilling fast quenching and handles under the high-purity argon gas protection;
2) with above-mentioned steps 1) the chilling fast quenching handles the strip obtain and is placed in the vacuum annealing furnace, is evacuated down to 2*10 -6More than the torr, or be evacuated down to 2*10 -5Charge in the 1 atmospheric high-purity argon atmosphere after torr is above, under 500～1150 ℃ of temperature, carry out 0.5～50 hour anneal, obtain the La of the good high C content of single phase property 1-xR x(Fe 1-yM y) 13-zSi zC αInterstitial compound.
CNB031210511A 2002-03-26 2003-03-21 Rereearth-iron base compound magnetic refrigeration material with large magnetic entropy change and preparation process thereof Expired - Fee Related CN1236096C (en)

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CN102093850B (en) * 2009-12-11 2015-03-25 中国科学院物理研究所 High-temperature-stable La(Fe,Si)13-based multi-interstitial-atom hydride magnetic refrigeration material with large magnetic entropy change and preparation method thereof
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