共查询到20条相似文献,搜索用时 78 毫秒
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如果放在光滑桌面上的物体只受一只弹簧的作用,那么物体所作的运动是简揩运动.简谐运动是一种最简单的基本运动,它的动力学特点是物体所受合力满足F=-kx,该力叫回复力.简谐运动的特点是具有周期性,周期T=2π√m/k,其中m是振动物体质量,k是回复力 相似文献
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弹簧是中学物理中一个重要模型,可与物理中的诸多知识点有机结合来考查同学们的分析和推理能力.下面通过几例高考题谈谈此类问题的解答方法. 相似文献
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组合线性弹簧振子中的非线性振动 总被引:1,自引:0,他引:1
从拉格朗日方程出发,分析了几种常见的线性弹簧组合,对作非线性振动弹簧振子进行了数值求解.当作微小振动时,正好是几种典型的非线性振动.通过计算得出解析解并与数值解进行了对比. 相似文献
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用分子动力学方法研究了N,O,Si,P,S等5种杂质对扶手椅型(5,5)和锯齿型(9,0)单壁碳纳米管杨氏模量的影响.结果表明:直径为0.678和0.704 nm的扶手椅型(5,5)和锯齿型(9,0)碳纳米管在无掺杂时其杨氏模量分别为948和804 GPa.在掺杂浓度10%以下,碳纳米管的拉伸杨氏模量均随掺杂浓度增加近似呈线性下降规律,下降率以Si掺杂最大,N掺杂最小.对与C同周期的元素掺杂,随原子序数增加碳纳米管的杨氏模量下降率增大;与C不同周期的元素掺杂,碳纳米管的杨氏模量随掺杂浓度增加下降率更大,但
关键词:
碳纳米管
杂质
杨氏模量
分子动力学方法 相似文献
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采用电化学腐蚀制备多孔硅,利用场致发射扫描式电子显微镜(field emission scanning electron microscope,FESEM)观测多孔硅的二维微观形貌,利用Nano Indenter XP中的纳米轮廓扫描仪组件(nano profilometry, NP)得到其三维拓扑分析图像,分析了微观结构差异的原因并讨论了多孔硅内部微观结构对其机械性能的影响;利用MTS Nano Indenter XP纳米压入测量仪器,研究了多孔硅的显微硬度和杨氏模量随压入深度的变化规律,比较了不同孔隙率多孔硅的机械性能差别.实验结果测得40mA/cm2,60mA/cm2,80mA/cm2和100mA/cm2四个不同腐蚀电流密度条件下制备多孔硅样品的孔隙率在60%—80%范围内,孔隙率随着腐蚀电流密度的增加而增大;在氢氟酸(HF)浓度为20%的条件下制备出多孔硅样品的厚度在40μm—50μm范围内;测得多孔硅的平均硬度、平均杨氏模量分别在0.478GPa—1.171GPa和10.912GPa—17.15GPa范围内,并且其数值随腐蚀电流密度的增加而减小,在纳米硬度范围内随压入深度的增加而减小,在显微硬度范围内其数值保持相对恒定,分析了样品表面、厚度、微观结构,及环境对其机械性能的影响,得到了多孔硅力学性能随其微观尺度形貌的变化规律.
关键词:
多孔硅
微观结构
硬度
杨氏模量 相似文献
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Asymmetric plate impact experiments are conducted on LY12 aluminium alloy in a pressure range of 85-131 GPa. The longitudinal sound speeds axe obtained from the time-resolved particle speed profiles of the specimen measured with Velocity Interferometer System for Any Reflector (VISAR) technique, and they are shown to be good agreement with our previously reported data of this alloy in a pressure range of 20-70 GPa, and also with those of 2024 aluminium reported by McQueen. Using all of the longitudinal speeds and the corresponding bulk speeds calculated from the Gruneisen equation of state (EOS), shear moduli of LY12 aluminium alloy are obtained. A comparison of the shear moduli in the solid phase region with those estimated from the Steinberg model demonstrate that the latter are systematically lower than the measurements. By re-analysing the pressure effect on the shear modulus, a modified equation is proposed, in which the pressure term of P/η^1/3 in the Steinberg model is replaced by a linear term. Good agreement between experiments and the modified equation is obtained, which implies that the shear modulus of LY12 aluminium varies linearly both with pressure and with temperature throughout the whole solid phase region. On the other hand, shear modulus of aluminium in a solid-liquid mixed phrase region decreases gradually and smoothly, a feature that is very different from the drastic dropping at the melting point under static conditions. 相似文献
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Asymmetric plate impact experiments are conducted on LY12 aluminium
alloy in a pressure range of 85--131\,GPa. The longitudinal sound
speeds are obtained from the time-resolved particle speed profiles of
the specimen measured with Velocity Interferometer System for Any
Reflector (VISAR) technique, and they are shown to be good agreement
with our previously reported data of this alloy in a pressure range
of 20--70\,GPa, and also with those of 2024 aluminium reported by
McQueen. Using all of the longitudinal speeds and the corresponding
bulk speeds calculated from the Gruneisen equation of state (EOS),
shear moduli of LY12 aluminium alloy are obtained. A comparison of
the shear moduli in the solid phase region with those estimated from
the Steinberg model demonstrate that the latter are systematically
lower than the measurements. By re-analysing the pressure effect on
the shear modulus, a modified equation is proposed, in which the
pressure term of $P/\eta^{1/3}$ in the Steinberg model is replaced by
a linear term. Good agreement between experiments and the modified
equation is obtained, which implies that the shear modulus of LY12
aluminium varies linearly both with pressure and with temperature
throughout the whole solid phase region. On the other hand, shear
modulus of aluminium in a solid-liquid mixed phrase region decreases
gradually and smoothly, a feature that is very different from the
drastic dropping at the melting point under static conditions. 相似文献
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