In recent years,magnetic refrigeration technology has been recognized as a promising new type of refrigeration technology due to its advantages of energy conservation,efficiency,and environmental protection,and is also a potential alternative to gas compression refrigeration.The key to the development of magnetic refrigeration technology is to explore giant magnetothermal materials that can meet the requirements of working at suitable temperatures.In this thesis,RE1-xRE’xCo Ni(RE,RE’=Dy,Ho,Er,x=0,0.25,0.5,0.75,1),Er Co2Bx(x=0,0.025,0.05,0.075,0.1)and RE6Ni2.3In0.7(RE=Ho,Er,Tm)intermetallic compounds were prepared by arc melting,and their structures,magnetism and magnetocaloric effects were systematically researched,and the following research results were obtained.The RE1-xRE’xCo Ni(RE,RE’=Dy,Ho,Er,x=0,0.25,0.5,0.75,1)compounds are Mg Cu2(C15)cubic structure,and the space group are Fd3m.With the increase of temperature,the compound will undergo a secondary magnetic phase transition from ferromagnetic state to paramagnetic state,with almost no hysteresis and thermal hysteresis.Moreover,with the increase of x,the Curie temperature TCof Dy1-xHoxCo Ni compounds linearly decreased from 67.0 K to 41.0 K,and the TCvalue of Ho1-xErxCo Ni linearly decreased from 41.0 K to 23.0 K,basically covering the entire cooling range in the mid-temperature region.WhenΔH=5 T,the maximum magnetic entropy change-ΔSMof RE1-xRE’xCo Ni compounds varies from 9.87 to 18.80 J/kg K;The average temperature magnetic entropy change TEC(5 K)varies from 9.79 to18.29 J/kg K;The refrigerant capacity RC varies from 330.23 to 433.27 J/kg;The relative cooling power RCP varies from 427.51 to 586.97 J/kg.It has been proved that RE1-xRE’xCo Ni material is a medium temperature magnetic refrigeration material with good application potential.The main phase of Er Co2Bx(x=0,0.025,0.05,0.075,0.1)doped with trace boron element is Mg Cu2type Laves phase structure,and the space group is Fd3m.The doping of trace boron will make the lattice constant decrease first and then increase,but the Curie temperature TCdoes not change significantly.The ferromagnetic-paramagnetic phase transition occurs with the increase of temperature.Although all compounds are first-order magnetic phase transitions,the doping of B element can effectively reduce the thermal hysteresis of the compounds.Er Co2Bxcompounds in external magnetic field change ofΔH=5 T,the maximum magnetic entropy change-ΔSMcan reach 28.10,30.07,26.78,27.71 and 25.62 J/kg K respectively;The average temperature magnetic entropy change TEC(5 K)is 26.62,28.17,24.94,26.36 and24.86 J/kg K respectively;TEC(10 K)is 22.09,24.98,20.97,24.07 and 21.99 J/kg K respectively.The refrigerant capacity RC is 204.98,258.76,205.02,265.95 and235.40 J/kg respectively;The relative cooling power RCP is 245.84,298.70,257.62,322.53 and 285.40 J/kg respectively.It is proved that B element doping can regulate the magnetic and magnetothermal properties of Er Co2,which makes Er Co2Bx(x=0,0.025,0.05,0.075,0.1)material have certain research value in the field of mid-temperature magnetic refrigeration.The ternary intermetallic compounds RE6Ni2.3In0.7(RE=Ho,Er,Tm)belong to Ho6Co2Ga type structure,and the space group is Immm.The three samples undergo continuous and complex magnetic phase transitions as the temperature increases.When external magnetic field changeΔH=2,5 and 7 T,the maximum magnetic entropy change-ΔSMof RE6Ni2.3In0.7(RE=Ho,Er,Tm)compounds can reach 1.27,5.97and 9.66 J/kg K,2.12,9.09 and 13.93 J/kg K,6.54,14.49 and 17.59 J/kg K respectively.In addition,whenΔH=5 T,the average temperature magnetic entropy change TEC(5K)and TEC(10 K)of RE6Ni2.3In0.7(RE=Ho,Er,Tm)compounds can reach 5.84 and5.70 J/kg K,8.78 and 8.48 J/kg K,13.90 and 12.79 J/kg K respectively.The RC and RCP can reach 140.24 J/kg and 179.75 J/kg,171.79 J/kg and 220.70 J/kg;182.86 J/kg and 234.45 J/kg,respectively.Among them,Tm6Ni2.3In0.7material not only has good refrigeration capacity,but also has a relatively wide refrigeration temperature range,which has potential application prospects in the field of magnetic refrigeration. |