CN101105996A - High temperature low magnetic field large magnetic material and its preparation method thereof - Google Patents
High temperature low magnetic field large magnetic material and its preparation method thereof Download PDFInfo
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- CN101105996A CN101105996A CNA2007100993777A CN200710099377A CN101105996A CN 101105996 A CN101105996 A CN 101105996A CN A2007100993777 A CNA2007100993777 A CN A2007100993777A CN 200710099377 A CN200710099377 A CN 200710099377A CN 101105996 A CN101105996 A CN 101105996A
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Abstract
A high-temperature low-magnetic field big-magnetic entropy compound and the preparation method thereof and belongs to the technical field of magnetic cold material. The chemical composition of the compound is La (FeyCo1-y) 13-xAlx, 1.50>=x>=1.2, and the value of y is ranged from 0.075 to 0.15. The curve of the material's M2 changing with Mu0H/M is linear in magnetic inversion temperature, and under the condition of magnetic inversion temperature above 305k and magnetic field change equal to 2T, the absolute value of the maximum changing value of magnetic entropy is above 3J/kg is multiplied by K. The production method is: mix raw materials of La, Fe, Co, and Al by chemical composition, and place them in a melting furnace, which is vacuumed to 4 is multiplied by 10-3Pa. And then argon gas is injected to obtain the compound with even composition after cooling. The melted compound is placed into cold water after going through evening treatment for 120 to 360 hours under the temperature of 900-1100 DEG C. The method has the advantages of: Simple producing technique, large magnetic entropy change under the condition of low magnetic field and high temperature, and application to magnetic refrigeration conditioner after forming compound material with GD.
Description
Technical field
The invention belongs to technical field of magnetic, a kind of high temperature low magnetic field large magnetic material and preparation method thereof particularly is provided.
Background technology
In recent years, because the magnetic Refrigeration Technique is considered to one of a kind of environmental protection, energy-efficient new Refrigeration Technique of future generation, has the magnetic refrigerating material exploratory development that huge magnetic entropy becomes and caused people's very big concern.To the application of magnetic Refrigeration Technique in air-conditioning, carried out detailed research especially.If but the magnetic Refrigeration Technique will be used for air conditioner refrigerating, need Curie temperature at room temperature and the big magnetic entropy material that is higher than room temperature.The material that the Curie temperature of now having reported is higher than the huge magnetic entropy change of having of room temperature has MnFeP
1-xAs
xBased compound, when x=0.55, Tc=305K, the magnetic entropy changing value Δ S when outside magnetic field changes 2T is 14Jkg
-1K
-1(US7069729B2), MnAs
1-xSb
xBased compound when temperature is higher than room temperature, has big magnetic entropy changing value (US6826915B2), and adding H in addition can be with La (Fe as interstitial atom
1-xSi
x)
13The Curie temperature of compound is brought up to the above and magnetic entropy changing value Δ S constant substantially (US7063754B2) of room temperature, for example at La (Fe
0.88Si
0.12)
13H
yIn when y=1.5, Tc=323K, the magnetic entropy changing value Δ S when outside magnetic field changes 2T is-19Jkg
-1K
-1Also has the Ni of report recently
55.5Mn
20Ga
24.5Alloy, Tc are greatly about 315K, and the magnetic entropy changing value Δ S when outside magnetic field changes 2T is for being about-15Jkg
-1K
-1(ZL200410009188.2) or the like.But, can not prepare in a large number now because the preparation process of above-mentioned material is all comparatively complicated.And, therefore be necessary to explore the magnetic refrigerating material that more Curie temperature is higher than room temperature because they are to belong to first order phase change, and heat stagnation that has and magnetic hysteresis are still waiting to overcome.
Cube NaZn
13La (the Fe of type
1-yCo
y)
13-xAl
xAlloy has high Curie temperature.It is reported La (Fe
1-xCo
x)
11.44Al
1.56When x=0.4, Tc=320K has magnetic entropy and becomes Δ S=-4.56Jkg under 5T
-1K
-1Bibliographical information La (Fe is also arranged
0.92Co
0.08)
11.83Al
1.17Curie temperature be 303K, and great magnetic entropy variation Δ S=-4.5Jkg is arranged when 2T
-1K
-1But, in this article,, need under 1273K, anneal 50 days in order to obtain uniform 1:13 phase.Therefore there is complex process, is not easy mass-produced problem.In addition, use as air-conditioning, also need Curie temperature to be higher than the material that big magnetic entropy is arranged of room temperature in order to make the magnetic refrigeration.Particularly at the material that under downfield, shows big magnetic entropy more than the room temperature.In order to solve this problem, the present invention proposes a kind of big magnetic entropy material of downfield that can be operated in more than the room temperature.
Summary of the invention
The object of the present invention is to provide a kind of high temperature low magnetic field large magnetic material and preparation method thereof, working temperature is higher than room temperature, and has great magnetic entropy variation compound and preparation method thereof under downfield, is suitable for the magnetic Refrigeration Technique of using in the refrigeration such as air-conditioning.
The present invention relates to a kind of La (Fe of the NaZn13 of having structure
yCo
1-y)
13-xAl
xMaterial is characterized in that 1.50 〉=x 〉=1.2, and La (Fe, M)
13(Al) the compound space group is Fm3c for M=Co, Si, and their magnetic performance is very responsive to the content of M.LaFe
11.37Al
1.63Two magnetic phase transitions of compound, one is first order phase change, another is a second-order phase transistion, along with the rising of temperature at first occurs occurring the second-order phase transistion of antiferromagnetic state to the paramagnetic attitude afterwards by the primary magnetic phase change of ferrimagnetic state to antiferromagnetic state.When material was in antiferromagnetic zone, downfield promptly can cause the change magnetic transition of antiferromagnetic state to ferrimagnetic state, shows LaFe
11.44Si
1.63And LaFe
11.37Al
1.63Magnetic free energy difference in the compound between ferrimagnetic state and the antiferromagnetic state is very little.In order to make material be in stable ferromagnetism phase, in the present invention, the content of Al is reduced to below 1.50 preferably about 1.3.If but the content of Al is reduced to 1.2 when following, form single 1:13 and will pass through long term annealing mutually, is unfavorable for suitability for industrialized production.In addition, its Curie temperature can descend, and is unfavorable for using as the magnetic refrigerating material more than the room temperature.
In addition, the feature of material of the present invention has secondary magnetic phase transition, M
2With μ
0The curve that H/M changes is linear near Curie temperature.Material does not have heat stagnation and magnetic hysteresis like this, and can stablize at the externally-applied magnetic field magnetic.
And the Curie temperature of material of the present invention is greater than 305K, less than 360K.This series material can use as composite material simultaneously with the Gd of Curie temperature at 295K like this, makes between refrigeration area in room temperature to more than the room temperature.Air conditioner refrigerating scope just.
Another feature of material of the present invention is that La can be by rare earth element Pr, and Nd replaces, and the replacement amount is from 3% to 20% of atomic ratio.Pr, the replacement of Nd can be finely tuned Curie temperature and magnetic entropy and be changed.
Other features of material of the present invention are values from 0.075 to 0.15 of y.Because La (Fe
xAl
1-x)
13The Curie temperature of compound is on the low side, improve its Curie temperature so add Co, but Co should not add, and Curie temperature is elevated to more than the air-conditioning work temperature.And the increase of the content of Co, also can reduce the maximum magnetic entropy variable value.
Other features of material of the present invention are that Al can be by Si, Ge, and Sn replaces, and the replacement amount is within atomic ratio 10%.Use Si, Ge, Sn replaces Al also can finely tune Curie temperature, can also finely tune the size of magnetic entropy.
Other features of material of the present invention are to be under the 2T in changes of magnetic field, and on the temperature variant curve of magnetic entropy, the product (relative refrigerating capacity RCP) of half corresponding temperature range Δ T of maximum magnetic entropy variable value and maximum magnetic entropy variable value is greater than 155, less than 300.And in changes of magnetic field is under the 2T, and the maximum magnetic entropy variable value is greater than 3J/Kg.K, less than 8J/Kg.K.。The present invention is to provide a kind of material, because the content of Al is lower, so just can obtain bigger magnetic entropy change and refrigerating capacity after the match low with big refrigerating capacity.
The method of The compounds of this invention is: La, Fe, Co, Al raw material are pressed La (Nd, Pr) (Fe
yCo
1-y)
13-xAl
xCarry out proportioning, put into smelting furnace, be evacuated to 4 * 10 before the melting
-3More than the Pa, feed argon gas then, evenly melting; The compound that obtains after the even melting was handled 120～360 hours 900～1100 ℃ of following homogenizing, put into frozen water then and cool off, to obtain single NaZn
13Phase.Best annealing time 240 hours.
Smelting furnace of the present invention is a vacuum arc furnace ignition, induction furnace or other smelting furnace.
The invention has the advantages that the working temperature of material is more than room temperature, and in the magnetic field range that permanent magnet can provide, refrigerating capacity and maximum magnetic entropy variable are big relatively, and preparation is simple, and Curie temperature is adjustable, do not have heat stagnation and magnetic hysteresis, can be widely used in the magnetic Refrigeration Technique.
Description of drawings
Fig. 1 is La (Fe of the present invention
0.919Co
0.081)
11.7Al
1.3X ray diffracting spectrum at room temperature.Wherein, abscissa is the angle of diffraction, and ordinate is an intensity.
Fig. 2 is La (Fe of the present invention
0.919Co
0.081)
11.7Al
1.3The M-T curve.Wherein, abscissa is a temperature, and ordinate is the magnetization.
Fig. 3 is La (Fe of the present invention
0.919Co
0.081)
11.7Al
1.3Magnetization curve, wherein, abscissa is magnetic field, ordinate is the magnetization.
Fig. 4 is La (Fe of the present invention
0.919Co
0.081)
11.7Al
1.3The curve of Arrott.Wherein, abscissa is μ
0H/M, ordinate are M
2
Fig. 5 is La (Fe of the present invention
0.919Co
0.81)
11.7Al
1.3Magnetic entropy becomes with the variation of temperature curve under 2T magnetic field.Wherein, abscissa is a temperature, and ordinate is that magnetic entropy becomes.
Fig. 6 is La of the present invention
0.8Nd
0.2(Fe
0.919Co
0.081)
11.7Al
1.3X ray diffracting spectrum at room temperature.Wherein, abscissa is the angle of diffraction, and ordinate is an intensity.
Fig. 7 is La of the present invention
0.8Nd
0.2(Fe
0.919Co
0.081)
11.7Al
1.3Magnetic entropy becomes with the variation of temperature curve under 2T magnetic field.Wherein, abscissa is a temperature, and ordinate is that magnetic entropy becomes.
Fig. 8 is La of the present invention
0.8Nd
0.2(Fe
0.919Co
0.081)
11.7Al
1.3RCP with the change curve of Δ H, wherein, abscissa is the change in magnetic field, ordinate is RCP.
Embodiment
Embodiment 1:
With La, Fe, Si, raw material such as Co are by chemical constituent La (Fe
0.919Co
0.081)
11.7Al
1.3Proportioning is put into vacuum arc furnace ignition, in induction furnace or other smelting furnace, is evacuated to 4 * 10
-3Pa or more than, feed argon gas, obtain the compound of uniform ingredients after the melt back cooling.The compound that melting obtains was handled 240 hours 1000 ℃ of following homogenizing, directly put into the frozen water fast quenching then.For preventing the sample oxidation, homogenizing is handled and annealing process can be carried out under vacuum or argon shield.Sample proves single NaZn through X-ray diffraction
13Phase is seen Fig. 1.Adopt SQUID to measure magnetization curve and vary with temperature, as Fig. 2,3.Through the compound that above-mentioned steps makes, Curie temperature is 315K, sees Fig. 2.And be second-order phase transistion, see Fig. 4.Result of calculation shows that under 2T magnetic field, magnetic entropy becomes 3.6J/kgK, sees Fig. 5.Refrigerating capacity RCP (Relative Cooling Power) value is by the maximum magnetic entropy variable absolute value relatively | Δ S|
MaxWarm area width δ T with magnetic entropy varied curve half-peak height place
FWHMMultiply each other and draw:
RCP＝|ΔS|
max×δT
FWHM
According to computing formula, La (Fe
0.919Co
0.081)
11.7Al
1.3RCP=168.6J/kg under Δ H=1.9T, result of calculation is listed in the table 1.In table 1, also listed some that from document, obtain and had the RCP that huge magnetic entropy becomes material at high temperature.Therefrom as can be known, though La (Fe
0.919Co
0.081)
11.7Al
1.3The magnetic entropy of material becomes and is not very big, but its RCP ability and MnFeP
0.45As
0.65, La (Fe
0.88Si
0.12)
13H
yAnd La (Fe
0.99Mn
0.01)
11.7Si
1.3H
yQuite.But La is (Fe
0.919Co
0.081)
11.7Al
1.3Material is owing to have second-order phase transistion, so material performance when using as refrigeration working medium is very stable, and preparation is simple relatively.It is a kind of magnetic cooling air conditioner material of great practical value.
The RCP value of the magnetic refrigerating material of several Curie temperature of table 1 more than room temperature is (Δ H=2T) relatively
| Material | Curie temperature (K) | |ΔS| max(J/(kg·K)) | RCP(J/kg) |
| Comparative example: La (Fe 0.88Si 0.12) 13H 1.5 | 323 | 19 | 146.6 |
| Comparative example: MnFeP 0.45As 0.65 | 332 | 11.8 | 146.9 |
| Comparative example: Gd | 295 | 4 | 169.4 |
| Comparative example: La (Fe 0.98Mn 0.02) 11.7Si 1.3H y (y≈2.0) | 315 | 12.9 | 132.3 |
| Comparative example: La (Fe 0.99Mn 0.01) 11.7Si 1.3H y (≈2.0) | 339 | 16 | 155.4 |
| Example of the present invention: La (Fe 0.919Co 0.081) 11.7Al 1.3 | 315 | 3.6 | 168.6 |
Embodiment 2:
With La, Nd, Fe, Si, raw material such as Co are by chemical constituent La
0.8Nd
0.2(Fe
0.919Co
0.081)
11.7Al
1.3Proportioning is put into vacuum arc furnace ignition, in induction furnace or other smelting furnace, is evacuated to 4 * 10
-3Pa or more than, feed argon gas, obtain the compound of uniform ingredients after the melt back cooling.The compound that melting obtains was handled 240 hours 1100 ℃ of following homogenizing, directly put into the frozen water fast quenching then.For preventing the sample oxidation, homogenizing is handled and annealing process can be carried out under vacuum or argon shield.Sample proves single NaZn through X-ray diffraction
13Phase is seen Fig. 6.Adopting SQUID to measure magnetization curve varies with temperature.Through the compound that above-mentioned steps makes, Curie temperature is 313K, and under 2T magnetic field, magnetic entropy becomes 4.5J/kg K, sees Fig. 7.The RCP of material sees Fig. 8 with Δ H variation relation curve.As Fig. 7, shown in 8, resulting La behind the adding Nd
0.8Nd
0.2(Fe
0.919Co
0.081)
11.7Al
1.3No matter be | Δ S|
MaxStill RCP has remarkable rising.The alternative La of adding Nd can improve magnetic refrigerating material | Δ S|
MaxAnd RCP.
Claims (10)
1. a high temperature low magnetic field large magnetic material is characterized in that: have NaZn
13La (the Fe of structure
yCo
1-y)
13-xAl
xMaterial, 1.50 〉=x 〉=1.2, the value of y from 0.075 to 0.15; M
2With μ
0The curve that H/M changes is linear at Curie temperature, and Curie temperature is greater than 305K, less than 360K.
2. according to the described compound of claim 1, it is characterized in that: La is by single or more than one rare earth element Pr, and Nd replaces, and the amount that substitutes is calculated with atomic percent, in from 3% to 20% scope.
3. according to the described compound of claim 1, it is characterized in that: Al is replaced by Si, Ge, Sn, and the amount that substitutes is calculated with atomic percent, within 10%.
4. according to the described compound of claim 1, it is characterized in that: in changes of magnetic field is under the 2T, on the temperature variant curve of magnetic entropy, the product of half corresponding temperature range Δ T of the absolute value of maximum magnetic entropy variable value and maximum magnetic entropy variable value is greater than 155, less than 300.
5. according to the described compound of claim 1, it is characterized in that: in changes of magnetic field is under the 2T, and on the temperature variant curve of magnetic entropy, the absolute value of maximum magnetic entropy variable value is greater than 3J/Kg.K, less than 8J/Kg.K.
6. according to the described compound of claim 1, it is characterized in that: its magnetic phase transition is a second-order phase transistion.
7. a method for preparing the described compound of claim 1 is characterized in that: La, Fe, Co, Al raw material are carried out proportioning by chemical constituent, put into smelting furnace, be evacuated to 4 * 10 before the melting
-3More than the Pa, feed argon gas then, evenly melting; The compound that obtains after the even melting was handled 120～360 hours 900～1100 ℃ of following homogenizing, put into frozen water then and cool off, to obtain single NaZn
13Phase.
8. in accordance with the method for claim 7, it is characterized in that described smelting furnace is a vacuum arc furnace ignition, induction furnace or other smelting furnace.
9. in accordance with the method for claim 7, it is characterized in that with La Nd, or Pr is alternative, the replacement amount is from 3% to 20% of atomic ratio.
10. in accordance with the method for claim 7, it is characterized in that, Al is substituted with Si, Sn or Ge, within 10%.
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| CN100501882C CN100501882C (en) | 2009-06-17 |
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Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101368243B (en) * | 2008-09-24 | 2010-04-21 | 上海大学 | Production method for magnetic refrigeration working medium material Y2Fe17 at room temperature |
| CN101831278A (en) * | 2010-02-09 | 2010-09-15 | 江苏大学 | Preparation method of stratified compound magnetic cooling working medium |
| CN102017026B (en) * | 2008-03-31 | 2014-04-09 | 亨利庞加莱南锡第一大学 | Intermetallic compounds, their use and process for preparing same |
| WO2014115057A1 (en) * | 2013-01-24 | 2014-07-31 | Basf Se | Performance improvement of magnetocaloric cascades through optimized material arrangement |
| CN104559943A (en) * | 2013-10-09 | 2015-04-29 | 中国科学院宁波材料技术与工程研究所 | Crystalline-state magnetic refrigeration metal material and preparation method thereof |
| US9245673B2 (en) | 2013-01-24 | 2016-01-26 | Basf Se | Performance improvement of magnetocaloric cascades through optimized material arrangement |
| CN105834407A (en) * | 2015-01-15 | 2016-08-10 | 中国科学院宁波材料技术与工程研究所 | Preparation method for rare earth ferrous alloy compound with NaZn13 type structure |
| CN112368790A (en) * | 2018-02-22 | 2021-02-12 | 通用工程与研究有限责任公司 | Magnetocaloric alloys for magnetic refrigeration applications |
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2007
- 2007-05-18 CN CNB2007100993777A patent/CN100501882C/en not_active Expired - Fee Related
Cited By (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102017026B (en) * | 2008-03-31 | 2014-04-09 | 亨利庞加莱南锡第一大学 | Intermetallic compounds, their use and process for preparing same |
| CN101368243B (en) * | 2008-09-24 | 2010-04-21 | 上海大学 | Production method for magnetic refrigeration working medium material Y2Fe17 at room temperature |
| CN101831278A (en) * | 2010-02-09 | 2010-09-15 | 江苏大学 | Preparation method of stratified compound magnetic cooling working medium |
| WO2014115057A1 (en) * | 2013-01-24 | 2014-07-31 | Basf Se | Performance improvement of magnetocaloric cascades through optimized material arrangement |
| US9245673B2 (en) | 2013-01-24 | 2016-01-26 | Basf Se | Performance improvement of magnetocaloric cascades through optimized material arrangement |
| US9915447B2 (en) | 2013-01-24 | 2018-03-13 | Basf Se | Performance improvement of magnetocaloric cascades through optimized material arrangement |
| CN104559943A (en) * | 2013-10-09 | 2015-04-29 | 中国科学院宁波材料技术与工程研究所 | Crystalline-state magnetic refrigeration metal material and preparation method thereof |
| CN105834407A (en) * | 2015-01-15 | 2016-08-10 | 中国科学院宁波材料技术与工程研究所 | Preparation method for rare earth ferrous alloy compound with NaZn13 type structure |
| CN105834407B (en) * | 2015-01-15 | 2018-07-27 | 中国科学院宁波材料技术与工程研究所 | With NaZn13The preparation method of the rare-earth iron-based alloy cpd of type structure |
| CN112368790A (en) * | 2018-02-22 | 2021-02-12 | 通用工程与研究有限责任公司 | Magnetocaloric alloys for magnetic refrigeration applications |
| CN112368790B (en) * | 2018-02-22 | 2024-04-26 | 通用工程与研究有限责任公司 | Magnetocaloric alloy for magnetic refrigeration applications |
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