不同煤阶煤孔隙特征及其吸附能力响应

我国是煤炭资源大国，煤层气储量规模相当可观，但煤储层又具有低孔、低渗的不足，照搬国外或常规石油天然气的开采程序和方法已被证实是走不通的。应结合实际，根据不同地质条件、不同煤阶的开采程序，进行孔隙特征研究。煤孔隙特征、连通性和吸附能力对煤层气开采影响尤为重要，为研究煤孔隙结构特征随煤变质程度的变化关系及其吸附能力的响应特点，采取不同地区不同变质程度煤样，进行压汞测试和等温吸附实验。实验结果表明，煤孔隙度和平均孔径均随变质程度增加呈现降低—升高—降低的趋势；煤中孔隙连通性随煤变质程度增加逐渐变差；随煤变质程度增加，其最大吸附能力也呈现降低—升高—降低的总体趋势。     

淬火配分处理对锻态Fe-0.2C-9Mn-3.5Al钢显微组织及力学行为的影响

分析了淬火配分处理对锻态Fe-0.2C-9Mn-3.5Al钢显微组织及力学行为的影响。结果表明,热处理态试验钢主要由块状δ-铁素体、马氏体和板条状残留奥氏体等多相构成;残留奥氏体的体积分数随等温淬火温度升高而增大,在310 ℃时达到峰值;310 ℃等温淬火后在400 ℃配分3 min时可以获得较优的综合力学性能,抗拉强度和断后伸长率分别为1175 MPa和21.50%,强塑积达到25.26 GPa·%;应力-应变曲线中存在着明显的“锯齿”状起伏,可能与亚稳态的残留奥氏体集中转变为马氏体有关。     

激光淬火对高速动车组EA4T车轴钢组织和性能的影响

为提高EA4T车轴钢的表面硬度和耐磨性能,采用激光淬火对调质态车轴进行表面改性。利用扫描电镜、显微硬度计、纳米压痕仪等对激光淬火层的微观组织、相变层深度和硬度进行了详细的表征。结果表明:EA4T车轴钢表面经过不同工艺激光淬火后,相变层内的淬火组织主要由细小的板条马氏体和粒状贝氏体组成,其深度根据工艺不同从100 μm到800 μm不等,并呈现随淬火功率的增加和扫描速度减小,相变层深度逐渐增加的趋势。淬火相变层区域内,车轴钢的显微硬度基本保持在450 HV0.2左右,约为基体硬度的2倍,耐磨性显著提高。由于淬火道次之间搭接的原因,淬火层呈现波形分布,其中波谷马氏体含量高于波峰位置,因此其硬度明显高于波峰处。     

5A06铝合金鞍型横梁等温挤压近净成形工艺

针对某5A06铝合金鞍型横梁,设计了等温挤压近净成形试验。通过Deform有限元分析研究了鞍型横梁等温挤压过程中金属流动规律和缺陷产生原因,并进行了毛坯尺寸和热挤压件图的优化。设计了鞍型横梁等温挤压近净成形模具,可实现在普通压力机上加热管加热方式升温、成形后多顶杆同步脱模功能。通过等温挤压近净成形方法制备了长为580 mm、最薄壁厚为4 mm、筋高为8 mm、筋宽为6 mm的薄壁复杂多筋鞍型横梁,该构件90%以上部位尺寸精度可达到±0. 3 mm,其余部位尺寸精度可达±0. 5 mm,抗拉强度达340 MPa,伸长率约为25%。对等温挤压件装配部位进行少量机加,可获得3种不同尺寸的鞍型横梁。     

淬火处理对轧辊用高硼高速钢组织和性能的影响

利用光学显微镜、扫描电镜、X射线衍射、硬度计及MM-200磨损试验机,研究了淬火温度对轧辊用高硼高速钢显微组织和性能的影响。结果表明,高硼高速钢的铸态组织由马氏体、铁素体、珠光体和沿晶界呈连续网状分布的共晶硼碳化物组成,共晶硼碳化物主要是M2B和M7(C,B)3;随着淬火温度的升高,基体全部转变成为马氏体,并有二次硼碳化物M23(C,B)6析出;高硼高速钢的硬度和耐磨性随着淬火温度的升高而明显增加,在1150℃淬火时硬度最高、耐磨性最好。     

中锰Q&P钢连续退火过程碳元素分配行为

采用扫描电镜、X射线衍射等研究了连续退火工艺中退火、淬火和配分等关键过程参数对中锰Q&P钢碳元素分配行为的影响,并分析了相应工艺条件下残留奥氏体量与碳含量的关系。结果表明:两相区退火温度的提高会导致奥氏体中的碳含量下降,微观组织表现为奥氏体含量增加,渗碳体量减少;退火时间10~60 s时,随着退火时间的延长,奥氏体含量和碳含量急剧增加,60 s后基本保持稳定;试验条件下淬火温度对残留奥氏体及碳含量的影响不显著;配分温度350~500℃时,随着配分温度的提高,奥氏体含量和碳含量呈现先增加后减小的趋势,配分温度450℃时均达到最大值;延长配分时间,残留奥氏体含量呈现先减少后增大再减少的趋势,残留奥氏体中的碳含量先减小后增加。     

Study on inhomogeneous cooling behavior of extruded profile with unequal and large thicknesses during quenching using thermo-mechanical coupling model

The interfacial heat transfer coefficient between hot profile surface and cooling water was determined by using inverse heat conduction model combined with end quenching experiment. Then, a Deform-3D thermo-mechanical coupling model for simulating the on-line water quenching of extruded profile with unequal and large thicknesses was developed. The temperature field, residual stress field and distortion of profile during quenching were investigated systematically. The results show that heat transfer coefficient increases as water flow rate increases. The peak heat transfer coefficient with higher water flow rates appears at lower interface temperatures. The temperature distribution across the cross-section of profile during quenching is severe nonuniform and the maximum temperature difference is 300 °C at quenching time of 3.49 s. The temperature difference through the thickness of different parts of profile first increases sharply to a maximum value, and then gradually decreases. The temperature gradient increases obviously with the increase of thickness of parts. After quenching, there exist large residual stresses on the inner side of joints of profile and the two ends of part with thickness of 10 mm. The profile presents a twisting-type distortion across the cross-section under non-uniform cooling and the maximum twisting angle during quenching is 2.78°.     

Isothermal crystallization kinetics and subsequent melting behavior of β‐nucleated isotactic polypropylene/graphene oxide composites with different ordered structure

The effects of ordered structure on isothermal crystallization kinetics and subsequent melting behavior of β‐nucleated isotactic polypropylene/graphene oxide (iPP/GO) composites were studied using differential scanning calorimetry. The ordered structure status was controlled by tuning the fusion temperature (T_f). The results showed that depending on the variation of crystallization rate, the whole T_f range could be divided into three regions: Region I (T_f > 179 °C), Region II (170 °C ≤ T_f ≤ 179 °C) and Region III (T_f < 170 °C). As T_f decreased from Region I to Region III, the crystallization rate would increase substantially at two transition points, due to the variation of the ordered structure status. Calculation of Avrami exponent n indicated that the ordered structure induced the formation of two‐dimensional growing crystallites rather than three‐dimensional growing crystallites. Moreover, in the case of isothermal crystallization, the ordered structure effect (OSE) can also greatly increase the relative content of β‐phase (β_c). In Region II, OSE took place, resulting in evident increase of β_c, achieving 92.4% at maximum. The variation of the isothermal crystallization temperature (T_iso) had little influence on the T_f range (Region II) of the OSE. The higher T_f in Region II was more favorable for the formation of higher β_c. The ordered structure was favorable for the improvement of the nucleating efficiency of β‐nucleating agent (β‐NE), and was more effective for the improvement of lower β‐NE. © 2018 Society of Chemical Industry