基于小世界网络的软件安全风险传播分析

针对软件安全风险传播难以直观描述的问题,应用小世界网络理论对其进行了研究.首先,介绍了软件安全风险的相关概念和小世界网络的性质及模型.其次,在分析软件系统网络拓扑结构的基础上,基于小世界网络理论建立了软件构件间安全风险传播的动力学模型,得到软件安全风险的传播结果,并分析影响软件安全风险传播的关键因素.最后,以某型飞机软...     

1，3，5-三（4-（苯丙烯酰基）苯基）苯的合成

以苯乙酮为原料,氯化亚砜-无水乙醇体系作催化剂,合成了1,3,5-三苯基苯．用二硫化碳-无水三氯化铝作催化剂,合成了1,3,5-三（4-乙酰基苯基）苯．在稀碱的催化下,1,3,5-三（4一乙酰基苯基）苯与苯甲醛反应,进一步合成了1,3,5-Z（4-（苯丙烯酰基）苯基）苯．采用傅立叶红外光谱和核磁共振（1H—NMR）对目标产物进行表征并得到了一致的结果．     

珍禽蛋溶菌酶制备工艺优化及稳定性研究

溶菌酶广泛存在于动、植物及微生物中,以鸡蛋蛋清中含量最高.珍禽蛋蛋清中溶菌酶酶活力远高于普通鸡蛋中溶菌酶酶活力,更适宜作为优质溶菌酶生产来源.文中以珍禽蛋与阳离子交换树脂为原料,建立一条适合工业化生产的珍禽蛋溶菌酶的制备工艺,研究主要分为以下几个方面：溶菌酶提取原料及树脂型号的选用,高原乌鸡鸡蛋溶菌酶制备工艺的建立,高原乌鸡鸡蛋溶菌酶质量评价.     

五参胶囊镇静催眠作用及其机制的实验研究

目的观察五参胶囊(Wu Shen Capsules,WSh C)对小鼠镇静催眠作用的影响,并探讨其作用机制.方法将ICR小鼠随机分为对照组、五参胶囊高剂量组、中剂量组和低剂量组.五参胶囊高剂量组用药量为200 mg/(kg·d~(-1)),中剂量组用药量为100 mg/(kg·d~(-1)),低剂量组用药量为50 mg/(kg·d~(-1)),给药时间为15 d,于给药结束后进行小鼠自主活动实验和协同戊巴比妥钠阈上剂量睡眠时间实验,测定5 min内各组小鼠的活动次数和站立次数,记录各组小鼠的睡眠潜伏期和睡眠持续时间.采用酶联免疫吸附法检测小鼠下丘脑5-羟色胺(5-Hydroxytryptamine,5-HT)、5-羟吲哚乙酸(5-Hydroxyindole acetic acid,5-HIAA)、γ-氨基丁酸(γ-aminobutyric acid,GABA)、谷氨酸(glutamine,Glu)含量,并计算5-HIAA/5-HT比值及Glu/GABA比值.结果与对照组比较,WSh C各给药组小鼠活动次数减少,睡眠潜伏期缩短,睡眠持续时间延长(P0.01),WSh C能升高小鼠下丘脑5-HIAA含量和5-HIAA/5-HT比值,降低Glu含量和Glu/GABA比值.结论 WSh C具有明显镇静催眠作用,其机制可能与调节中枢兴奋性和抑制性神经递质有关.     

一种基于微蜂窝小区用户比例公平的改进资源分配算法

在微蜂窝小区用户速率比例公平约束条件下,以最大化系统和速率为目标,提出了一种改进资源分配算法,并用拉格朗日法求解优化功率.结果表明:相比于传统的最低比例速率的资源分配算法,本算法在频率和总功率固定的条件下,能减少计算复杂度,且系统速率提高了约2%.     

CuO/C催化剂的制备及其脱除烟气中NO的研究

以褐煤为原料,先通过干馏、活化的方法制取活性半焦,再采用水热法在活性半焦上负载CuO制备CuO/C催化剂,利用XRD和SEM等技术对其晶体结构和微观形貌进行表征,并分析CuO/C催化剂对模拟烟气中NO脱除效果的影响因素。结果表明,活性半焦含有丰富的含氧官能团,是一种较好的催化剂载体和还原剂;在120℃和2h的制备条件下制备CuO/C催化剂时,在活性半焦表面生长的CuO晶体较多,尺寸较小且分散均匀;当C-NO的反应温度为250℃、空速为19 200h~(-1)、氧气含量为4%时,在120℃和2h制备条件下所制得的CuO/C催化剂对NO脱除效果好,其NO脱除率可达95.26%。     

转炉夹持器间隙及倾动加速度对自调螺栓冲击力的影响

利用三维建模软件并结合转炉实际尺寸进行建模,运用多体动力学与有限元方法对转炉进行动态仿真。对自调螺栓以及球形垫片进行子模型细化计算,将炉体与自调螺栓接触面的位移作为子模型边界条件,在稳定的热胀状态下进行瞬态分析,通过危险位置应力曲线分析夹持器间隙、倾动加速度对自调螺栓冲击力的影响。结果表明,夹持器间隙越大,自调螺栓所受的冲击力就越大,自调螺栓的振动发生在倾动加速度较大的倾角位置。     

Comparative study on the corrosion behavior of X52, 3Cr,and 13Cr steel in an O2–H2O–CO2 system: products,reaction kinetics,and pitting sensitivity

The corrosionbehaviors of X52, 3Cr low-alloy steel, and 13Cr stainless steel were investigated inanO2–H2O–CO2 environment at varioustemperaturesand O2–CO2partial-pressure ratios. The results showed thatthe corrosion rates of X52, 3Cr, and 13Cr steels in-creased with increasing temperature. The corrosion ratesslowly increased at temperaturesless than100℃ and increased sharply when the temperature exceeded100℃. In the absence of O2, X52, 3Cr, and 13Cr exhibited uniform corrosion morphology and FeCO3 was the main corrosion product. When O2 was introduced into the system, various forms of Fe2O3 appeared on the surface of the samples. The Cr content strongly influenced the corrosion resistance. The 3Cr steel with a low Cr content was more sensitive to pitting than the X52 or 13Cr steel. Thus, pitting occurred on the surface of 3Cr when 1.25 MPa of O2 was added; this phenomenon is related to the non-uniform distribution of Cr in 3Cr.     

Mechanism and simulation of droplet coalescence in molten steel

Droplet coalescence in liquid steel was carefully investigated through observations of the distribution pattern of inclusions in solidified steel samples. The process of droplet coalescence was slow, and the critical Weber number (We) was used to evaluate the coalescence or separation of droplets. The relationship between the collision parameter and the critical We indicated whether slow coalescence or bouncing of droplets occurred. The critical We was 5.5, which means that the droplets gradually coalesce when We ≤ 5.5, whereas they bounce when We > 5.5. For the carbonate wire feeding into liquid steel, a mathematical model implementing a combined computational fluid dynamics (CFD)-discrete element method (DEM) approach was developed to simulate the movement and coalescence of variably sized droplets in a bottom-argon-blowing ladle. In the CFD model, the flow field was solved on the premise that the fluid was a continuous medium. Meanwhile, the droplets were dispersed in the DEM model, and the coalescence criterion of the particles was added to simulate the collision-coalescence process of the particles. The numerical simulation results and observations of inclusion coalescence in steel samples are consistent.     

Microstructure evolution and mechanical properties of a large-sized ingot of Mg-9Gd-3Y-1.5Zn-0.5Zr (wt%) alloy after a lower-temperature homogenization treatment

In this paper, a large-sized ingot of Mg-9Gd-3Y-1.5Zn-0.5Zr (wt%) alloy with a diameter of 600 mm was successfully prepared by the semi-continuous casting method. The alloy was subsequently annealed at a relatively low temperature of 430℃ for 12 h as a homogenization treatment. The microstructure and room-temperature mechanical properties of the alloy were investigated systematically. The results show that the as-cast alloy contained a mass of discontinuous lamellar-shaped 18R long-period stacking ordered (LPSO) phases with a composition of Mg₁₀ZnY and an α-Mg matrix, along with net-shaped Mg₅(Y,Gd) eutectic compounds at the grain boundaries. Most of the eutectic compounds dissolved after the homogenization treatment. Moreover, the amount and dimensions of the lamellar-shaped LPSO phase obviously increased after the homogenization treatment. The structure of the phase transformed into 14H-type LPSO with composition Mg₁₂Zn(Y,Gd). The mechanical properties of the heat-treated large-sized alloy ingot are uniform. The ultimate tensile strength (UTS) and tensile yield strength (TYS) of the alloy reached 207.2 MPa and 134.8 MPa, respectively, and the elongation was 3.4%. The high performances of the large-sized alloy ingot after the homogenization treatment is attributed to the strengthening of the α-Mg solid solution and to the plentiful LPSO phase distributed over the α-Mg matrix.