功能材料
功能材料
공능재료
JOURNAL OF FUNCTIONAL MATERIALS
2014年
7期
7112-7115
,共4页
Fe-16Cr-2. 5Mo合金%阻尼性能%冷却方式%内应力
Fe-16Cr-2. 5Mo閤金%阻尼性能%冷卻方式%內應力
Fe-16Cr-2. 5Mo합금%조니성능%냉각방식%내응력
Fe-1 6Cr-2.5Mo alloy%damping capacity%cooling mode%internal stress
将 Fe-16Cr-2.5Mo 合金在1100℃真空保温1 h 后分别炉冷,空冷和油冷,研究了热处理冷却方式对 Fe-16Cr-2.5Mo 合金阻尼性能的影响.分析了不同冷却方式所得合金的微观结构、内应力与阻尼性能之间的关系.结果表明,随冷却速度减小,对数衰减率峰值增大,峰值所对应的应变振幅减小.合金阻尼性能随冷却方式的变化可用 SB 内应力分布理论解释,保温后炉冷时,冷却速度较慢,晶粒较大,C 原子和部分置换原子容易沿晶界析出,且合金的空位浓度降低,致使内应力小于空冷和油冷,这是保温后炉冷阻尼性能最高的本质原因.
將 Fe-16Cr-2.5Mo 閤金在1100℃真空保溫1 h 後分彆爐冷,空冷和油冷,研究瞭熱處理冷卻方式對 Fe-16Cr-2.5Mo 閤金阻尼性能的影響.分析瞭不同冷卻方式所得閤金的微觀結構、內應力與阻尼性能之間的關繫.結果錶明,隨冷卻速度減小,對數衰減率峰值增大,峰值所對應的應變振幅減小.閤金阻尼性能隨冷卻方式的變化可用 SB 內應力分佈理論解釋,保溫後爐冷時,冷卻速度較慢,晶粒較大,C 原子和部分置換原子容易沿晶界析齣,且閤金的空位濃度降低,緻使內應力小于空冷和油冷,這是保溫後爐冷阻尼性能最高的本質原因.
장 Fe-16Cr-2.5Mo 합금재1100℃진공보온1 h 후분별로랭,공랭화유랭,연구료열처리냉각방식대 Fe-16Cr-2.5Mo 합금조니성능적영향.분석료불동냉각방식소득합금적미관결구、내응력여조니성능지간적관계.결과표명,수냉각속도감소,대수쇠감솔봉치증대,봉치소대응적응변진폭감소.합금조니성능수냉각방식적변화가용 SB 내응력분포이론해석,보온후로랭시,냉각속도교만,정립교대,C 원자화부분치환원자용역연정계석출,차합금적공위농도강저,치사내응력소우공랭화유랭,저시보온후로랭조니성능최고적본질원인.
To clarify the effect of cooling mode on the damping capacity of Fe-1 6Cr-2.5Mo alloy,the specimens were annealed at 1 100 ℃ in vacuum by 1 h and cooled down in furnace,air and oil condition respectively.The relationships between the damping capacity,the microstructure and the internal stress of the alloy obtained by different cooling code are analyzed.The results show that the maximum logarithmic decrement would increase and the strain where the maximum logarithmic decrement appearing would decrease with the decreasing of cool-ing rate .This can be explained by introducing the SB theory,which elaborating the relationship between the ferromagnetic damping and the internal stress.The internal stress can block the motion of domain wall and thus deteriorating the damping capacity.Compared with being cooled in air and oil condition,the specimen cooled in furnace would accesses a smaller internal stress because the segregation of carbon near the grain boundary,the reduction of vacancy concentration and a smaller density of the grain boundary.