| 研究生: |
林英志 Lin, Yin-Chih |
|---|---|
| 論文名稱: |
合金元素添加對鐵磁形狀記憶Fe-Pd合金
微結構與性質之影響 Effects of Alloying Elements Addition on the Microstructures and Properties of Ferromagnetic Shape Memory Fe-Pd Alloys |
| 指導教授: |
李驊登
Lee, Hwa-Teng |
| 學位類別: |
博士 Doctor |
| 系所名稱: |
工學院 - 機械工程學系 Department of Mechanical Engineering |
| 論文出版年: | 2010 |
| 畢業學年度: | 98 |
| 語文別: | 中文 |
| 論文頁數: | 206 |
| 中文關鍵詞: | Fe-Pd30合金 、添加微量銠(Rh)、鋁(Al)、與鎳(Ni)元素 、晶粒細化 、顯微結構 、磁特性 |
| 外文關鍵詞: | Fe-Pd30 alloys, addition trace elements of Rh, Al, and Ni, grain size refinement, microstructures, magnetic properties |
| 相關次數: | 點閱:121 下載:1 |
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本研究論文,主要在鐵(Fe)-30 (at.%)鈀(Pd)之鐵磁性形狀記憶合金中,各別添加微量銠(Rh)、鋁(Al)、與鎳(Ni)元素,再分為三部份,分別探討上述三種不同微元素添加後,對Fe-Pd30系鐵磁性形狀記憶合金,所產生之磁性相微結構與磁特性的影響。
首先實驗證明添加微量Rh元素後,能顯著提升Fe-Pd30系合金的磁致伸縮應變值,其原因可能是Rh原子取代Pd的晶格位置,改變了磁原子間之交互作用,導致此合金磁晶體異向能常數(Ku)之增加,此外調幅式示差掃描量熱計(DSC)實驗結果顯示,在Fe-Pd30合金內添加微量Rh元素後,能有效的提高此合金系之沃斯田鐵相開始變態溫度(As),與沃斯田鐵相完成變態溫度(Af),其原因可能是添加Rh元素在Fe-Pd30合金中,降低了L10麻田散鐵相成核的自由能,促成L10麻田散鐵雙晶相容易成核,並使得L10麻田散鐵相更容易在較高溫度產生,此外Fe68-Pd30-Rh2與Fe66-Pd30-Rh4合金鍛造應變35~40%,經950–1050 ℃持溫適當時間,固溶退火再結晶處理,細化晶粒之後,能實質改善此合金之: (a)磁致伸縮應變值,(b)磁致伸縮應變/磁化率比值(rλ║s/rH),(c)作用磁場垂直試樣縱軸方向之飽和磁致伸縮應變值(λ^s),(d)增加延展性,(e)提高飽和磁感應強度(Ms),與增加磁晶體異向能常數(Ku)。掃描式與穿透式電子顯微鏡,對磁性相微結構的觀察發現,Fe-Pd-Rh合金,經鍛造應變固溶退火再結晶細化晶粒後,提升了磁致伸縮應變值,主要原因為固溶退火再結晶處理誘發晶粒細化,與再結晶處理所產生的變形雙晶(deformation twins)、變態雙晶(transformation twins)、與橫向雙晶(transverse twins)。磁滯(M-H)曲線實驗結果,顯示此合金試樣在低溫(100 K),具有較高的飽和磁感應強度(Ms),與較高的磁晶體異向能常數(Ku),這種現象主要歸因於在常溫(300 K)的(正方晶L10+單斜晶L1m)混合相,於低溫(100 K),相變態為單一正方晶L10麻田散鐵相所致。
其次實驗結果證明,在Fe-Pd30合金中,添加微量Al (4 at.%)後,經由TEM研究觀察顯示,在淬火狀態此Fe66-Pd30-Al4鐵磁性合金,內部包含一單斜晶L1m麻田散鐵相,這種L1m單斜晶麻田散鐵組織由兩種雙晶組成,即變形雙晶(L1m-D)與變態雙晶(L1m-T),而且變態雙晶L1m-T之模式鑑定為{101}L1m,此外穿透式電子顯微鏡(TEM)觀察研究顯示,序化型L10正方晶麻田散鐵,在淬火狀態係沿著平行{101}L1m-T單斜晶板狀變態雙晶面成核,TEM、SEM、振動試樣測磁儀(VSM)、與磁致伸縮量測儀研究結果顯示,此合金固溶再時效於475 ℃持溫19小時之後,L1m-T變態雙晶+L10相分解成等化學計量L10+L1m+αbct微結構,導致此合金的矯頑磁力增強,同時破壞了此合金之磁致伸縮應變。
最後在Fe-Pd30之鐵磁性形狀記憶合金中,添加微量Ni (4 at.%)後,用SEM、TEM、x-ray繞射儀(XRD)、振動試樣測磁儀(VSM)、與磁致伸縮量測儀,研究探討此Fe66-Pd30-Ni4合金之磁性相微結構與磁特性,研究結果發現,此合金固溶處理後之磁致伸縮應變值為λ║s=79×10−6,此應變值比原有狀態材料之磁致伸縮應變值λ║s=55×10−6高,原有狀態材料具較低之磁致伸縮應變值,其原因為原有狀態材料內部存在偏析,導致在磁場作用下,偏析阻礙了部分L10麻田散鐵雙晶晶界的移動,而造成原有狀態材料之磁致伸縮應變值較低。此外本研究之重要發現是;在Fe-Pd30系合金添加微量Ni替代Fe,則此合金鍛造應變,固溶退火再結晶處理,再經400 ℃ 持溫100小時時效處理後,似乎可以抑制L10+L1m雙晶相分解成等化學計量L10+L1m+αbct微結構,而使得此合金在400 ℃/持溫100小時,時效處理後之磁致伸縮應變值,仍然維持在λ║s=62×10−6;λ^s=−11×10−6,而且此時效試樣經x-ray繞射並未發現αbct相,此種磁特性證明此合金適合在高溫、高頻環境下(T<400 ℃)使用。又此合金鍛造應變,固溶退火再結晶處理後,試樣在500–700 ℃持溫100小時時效處理,經由x-ray繞射分析,發現試樣在500 ℃持溫100小時,時效處理後會有αbct相產生,此種αbct相的產生,導致此合金之磁致伸縮應變值大幅減少,同時造成此時效材料的維克氏微硬度值隨之上升,當此合金在600–700 ℃持溫100小時時效處理後,則發生過時效現象,同時促使L10+L1m+αbct麻田散鐵層狀組織再逐漸溶入基地,導致此合金之磁致伸縮應變值逐漸恢復。
This research paper mainly presents investigation of bulk ferromagnetic shape memory (FSM) Fe-30 (at.%) Pd alloys with additions of various trace amounts of Rh, Al, and Ni elements. The research paper is divided into 3 parts, and the influences of the various additions of Rh, Al, and Ni elements on the magnetic structures and magnetic properties are investigated in detail.
First, the experimental results indicate that additions of trace elements of Rh (2−4 at.%) to Fe-Pd30 alloy systems can significantly improve the magnetostrictive strains. The reason may be that Rh atom substitution for Pd in the atomic crystal position leads to a change the magnetic atomic interaction and an increase the magnetocrystalline anisotropy energy constant (Ku). In addition, the differential scanning calorimetry (DSC) test confirmed that Fe-Pd30 alloy systems doped with Rh (2−4 at.%) have an elevated austenite start transformation temperature (As) and austenite finish transformation temperature (Af). It can be inferred that doping Fe-Pd30 alloy system with Rh causes a decrease in L10 nucleation free energy, allowing easier generation of the L10 twin structure. Rh substitution for Pd in the Fe-Pd30 alloy systems also enhances the L10 phase formation at a higher temperature. In addition, the Fe68-Pd30-Rh2 and Fe66-Pd30-Rh4 (at.%) alloys strain-forged to a 35–40% reduction in thickness and recrystallized through thermal annealing at 950–1050 ℃ for proper times show improvements in the following: (a) magnetostrictive strains, (b) magnetostrictive susceptibility (rλ║s/rH), (c) perpendicular saturation magnetostriction (λ^s), (d) increase in ductility, and (e) elevation of the saturation magnetization and the magnetocrystalline anisotropy energy constant (Ku). SEM and TEM investigations indicate that the high magnetostriction of the strain-forged Fe-Pd-Rh alloy through solution treated (ST) and annealed recrystallization can mainly be ascribed to the grain refinement, as well as deformation twins, transformation twins, and transverse twins. The mass magnetization (M) versus magnetic field (H) M-H curves indicate that a specimen test at lower temperature (100 K) resulted in a higher saturated magnetization (Ms) as well as a higher magnetocrystalline anisotropy energy constant (Ku). This phenomenon is ascribed to the martensitic transformation from the mixed L10+L1m at RT (300 K) to a single L10 structure as the sample was tested at lower temperature (100 K).
Next, the experimental results present the results of doping the Fe-Pd30 alloy systems with additions of trace elements of Al (4 at.%). TEM observation indicated that in the as quenched condition, the alloys consisted of a monoclinic L1m martensite phase. The L1m monoclinic martensite structure was comprised of two types of twins: deformation twins (L1m-D) and transformation twins (L1m-T). The transformation twinning L1m-T mode was also identified as {101}L1m. In addition, TEM observation indicated that an ordered L10 tetragonal martensite nucleates along parallel {101}L1m-T monoclinic transformation twin plates during the quenching. TEM, SEM, vibrating sample magnetometer (VSM), and magnetostrictive-meter investigations demonstrated that after ST and aging of the alloys at 475 ℃ for 19 h, the decomposition of L1m-T transformation twins+L10 phase into stoichiometric L10+L1m+αbct structures simultaneously leads to an increase in the coercivity and a destruction of the magnetostriction.
Finally, the microstructures and magnetic properties of ferromagnetic shape memory Fe-Pd30 alloy systems additions of trace elements of Ni (4 at.%) were investigated by SEM, TEM, x-ray diffraction (XRD), VSM, and a magnetostriction meter. The research results show that the magnetostrictive strains of the Fe66-Pd30-Ni4 alloys after homogenization treatment (λ║s=79´10−6) are higher than those of as received materials (λ║s=55´10−6). The lower magnetostriction of the as received metal is due to segregation-impeded parts of the L10 twin boundary motion in realistic magnetic fields. In addition, an important discovery in this study was that doping the Fe-Pd30 alloy system with Ni substitution for Fe seems to prevent the decomposition of L10+L1m twin phase into stoichiometric L10+L1m+αbct structures, as the strain-forged alloys were ST and annealed recrystallization, then aged at 400 ℃ for 100 h. The magnetostrictive strains of the 400 ℃/100 h aged sample were maintained with λ║s=62×10−6;λ^s=−11×10−6, and the XRD analysis discovered no occurrence of the αbct phase in the aged sample. This magnetic property of the alloys is suitable for application in a high temperature and high frequency (T<400 ℃) environment. The strain-forged samples were ST and annealed recrystallization, then were aged at 500~700 ℃ for 100 h. Through analyzed by XRD, the formation of an αbct phase was observed as the specimen was aged at 500 ℃ for 100 h. This αbct phase occurrence caused large reductions in the magnetostrictive strains, while at the same time the hardness increased. When the samples were aged at 600~700 ℃ for 100 h, overaging occurred, the martensitic stoichiometric L10+L1m+αbct lamellar structures dissolved into the matrix simultaneously, and the magnetostrictive strains gradually recovered.
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