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1.
刘晶磊  刘鹏泉  尚康君  王洋 《地震工程学报》2021,43(6):1394-1401,1418
为探究层状地基环形沟隔振中几何参数对其隔振效果的影响规律,文章采用振幅衰减比Ar值进行评价分析,并定义沟后Ar≤0.4区域为有效隔振区域,通过改变环形沟的几何参数,得到其对有效隔振区域影响变化规律,从而确定环形沟不同几何参数对其隔振效果的影响。结果表明:层状地基土中环形沟深度位于土层分界面附近时,环形沟隔振效果相对较弱;当宽度参数在0.01~0.35之间不断增大时,有效隔振区域占比变化幅度仅为4.8%,即环形沟宽度变化对环形沟隔振效果影响较小;随着环形沟弧长的增加,有效隔振区域面积的扩大速率减缓,弧长参数达到2.20以后,隔振效果趋于稳定;振源与环形沟之间及环形沟末端位置区域存在振动放大区。  相似文献   

2.
通过室外试验的方法绘制相对加速度的二维等值线图,并依据桩周土体的振动情况进行区域划分,进一步研究单桩几何尺寸变化时其周围土体振动区域的变化情况。结果表明:单桩桩前、桩两侧存在振动加强区,桩前的振动加强现象更强,以桩角处尤为明显;当桩长与波长的比值在0.109~0.840时,隔振区、反射区的面积增长幅度较大,而绕射区的面积则迅速减小,当比值在0.840~0.962时,隔振区、反射区以及绕射区的面积变化很小,数据趋于缓和;桩径与波长的比值对桩周振动区域的影响较大,随着比值在0.013~0.163之间增大,隔振区与反射区的面积分别增加了0.249 m~2、0.129 m~2,增长的速率均较快,而绕射区的面积以较快的速率降低了0.088 m~2;振源距与波长的比值对隔振区与反射区的面积影响较大,当比值在0.163~0.961时,隔振区与反射区的面积急速下降,当比值在0.961~1.068时,变化趋势趋于缓和,对于绕射区面积,随着比值的增加,绕射区的面积仅仅增加了0.037 m~2。  相似文献   

3.
基于GM4磁通门磁力仪秒数据,分析研究了2008-2014年天水地磁台的地磁极化值和转换函数变化,结果表明在2013年岷县6.6级地震前天水台地磁极化值和转换函数存在不同程度的异常:(1)转换函数|A|和|B|在震前均出现了下降-转折-上升的异常变化,在上升至最高点时发生了岷县6.6级地震;(2)较短的周期转折上升变化更明显,幅度也更大,如|A|的20~80 s和|B|的20~110 s;(3)3.20 s、50 s和80 s周期的帕金森矢量方位角在震前出现转向并指向震中的现象;(4)4.5~100 s周期的极化值Yzh在震前3个月出现2次超3倍均方差的高值异常。  相似文献   

4.
在分析已有资料的基础上划分了兰州盆地与建设工程分布密切相关的T0、T1、T2、T3和T4级黄河阶地,建立201个土层地震反应模型。通过一维等效线性化计算和反应谱分析,得出兰州盆地沉积阶地50年超越概率10%地表地震动参数,分析阶地高度和vS≤500 m/s覆盖层厚度特征与地震动参数峰值加速度Am和加速度反应谱特征周期Tg的相关性。表明兰州盆地T0~T2阶地覆盖层厚度与50年超越概率10%Am呈正相关,T3及以上阶地覆盖层厚度对Am增大有明显的减小作用。Tg值随T0~T3阶地覆盖层厚度的增加而变大,当覆盖层厚度进一步变大,Tg值不再同步增大,阶地覆盖层厚度对Tg的影响是有限的,阶地海拔高度与地表50年超越概率10%地震动参数没有关系。  相似文献   

5.
为调查饱和珊瑚砂液化相关特性与发展规律,针对饱和Chibishi珊瑚砂,开展一系列不排水循环三轴试验,研究相对密度Dr和循环应力比CSR对饱和Chibishi珊瑚砂的超孔隙水压力Δu、轴向应变εa及动强度特性的影响,并分析不同地区珊瑚砂抗液化强度的差异性。结果表明,饱和Chibishi珊瑚砂的Δu发展模式根据不同的CSR水平可以分为前期均匀增长型、前期突增型和后期突增型;此外,采用一种新的孔压模型对前期均匀增长型、前期突增型的孔压比ru进行表征,Chibishi珊瑚砂在相同的Dr条件下,双幅应变εDA达到5%的循环次数N随着CSR水平的增加而逐渐减小;各珊瑚砂在同一里氏震级对应的等效循环振动次数下,抗液化强度CRR的增长模式存在显著差异。研究结果可丰富对珊瑚砂液化特征的认知,同时对近岸和沿海工程的抗震设计提供参考依据。  相似文献   

6.
利用云南11个地磁台站的秒采样观测数据,计算和分析了地磁垂直强度极化值Yzh在2019年8月13日、14日通海MS5.0地震前及2019年9月8日墨江MS5.9地震前的时空变化特征。研究表明,地磁台站Yzh值的幅度在震前会出现同步增强现象。而与以往的极化震例研究相比,Yzh值的高值异常在震前出现时间要更早些,可能会在震前2~5个月出现,距发震时间越近,产生的异常幅值可能越大,异常持续时间也越长。同时,研究还发现2次地震主要发生在异常空间等值线的高值区内,尤其在零值阈值线附近,这可能对今后发震地点的预测有一定的指示意义。对比异常产生时段内的Dst指数,认为该高值异常并非由空间电流体系所引起。  相似文献   

7.
刘晶磊      张冲冲      刘航      梅名彰     《世界地震工程》2021,(2):132-142
为了研究分层土地基(上层为粘土层,下层为砂层)条件下几何参数对单排混凝土桩的隔振效果,该试验通过缩尺比例为1∶15的缩尺模型试验,以激振器作为点振源产生振动波向四周扩散,通过对比单排桩前后两侧振动加速度极值,清晰地展现出了单排桩对振动波的的影响区域,并得到了几何参数的隔振影响作用。在该试验条件下得出结论:相对于其他影响因素,桩长是影响隔振效果的重要参数,当桩长参数由0.28增至0.57时可提高约9%的隔振面积,同时增加桩长和隔振区长度可使隔振区域振幅大幅度减小与有效隔振面积大幅增加,但同时会造成桩前一侧振动增强;对于低频振动,单排桩隔振屏障对中频和高频有更好的隔振作用,该试验条件下隔振效果可相差约3%,且频率越高,穿透性越强,且将在桩后形成一个振动加强区;增加振源距可有效提高隔振效果,但当频率较低时,中远振源的隔振效果相近。  相似文献   

8.
计算和分析了云南地区5次ML ≥ 6.5强震前的应变扰动εi值.结果表明,地震前5~8年,归一化为4级的地震的εi出现明显的高值异常;未来震中区域εi值变小,周围地区增大,形成空区;εi值有由零星分布逐渐向震中区收缩、集中并增强的趋势.  相似文献   

9.
余娜  蒋长胜  马玉虎 《地震工程学报》2016,38(4):609-615,623
采用时间序列的“传染型余震序列”(ETAS)模型和最大似然法对2010年4月14日青海玉树MS7.1地震序列的参数进行了估计。为考察其结果的稳定性,设定不同的截止震级和不同的拟合截止时间分别进行序列参数估算。选用截止震级MC=ML1.5对玉树MS7.1地震序列整体的参数进行拟合,计算获得α=0.948 2,p=1.059 6和b=0.817 3。与中国大陆M>7.0地震序列的平均序列参数相比较表明,玉树MS7.1地震序列表现为触发次级余震的能力较弱,序列衰减速率较快。研究表明,截止震级MCα、kp值有一定的影响。随截止震级逐渐增大,参数k值逐渐减小,α值总体上有增加的趋势,而对p值的影响较小。在地震序列的早期阶段,ETAS模型参数中的p值和α值在震后14天内随时间的变化幅度较为明显,其后各参数变化相对平稳。  相似文献   

10.
人为干扰和气候变化会改变湖泊水位状态,明确不同水位条件下湖泊沉积物有机碳矿化特征及其影响因素,对了解内陆水生态系统碳循环具有重要意义.为探究干旱区典型盐湖沉积物有机碳矿化速率对水位变化的响应,以巴里坤湖干涸湖底原状沉积物为研究对象,初步探究了0(T1)、-9(T2)、-23(T3)、-34(T4)和-45 cm(T5)水位处理对沉积物有机碳矿化速率的影响.结果表明,T1、T2和T3处理有机碳矿化速率在试验初期较高(0~10 d),10 d后缓慢下降,T4和T5处理有机碳矿化速率呈先增加后降低趋势;T1(1.718 μmol/(m2·s))与T3(1.784 μmol/(m2·s))处理有机碳矿化速率不存在显著差异,T1处理有机碳矿化速率是T2、T4和T5处理的1.09、3.31和3.57倍,不同处理有机碳累积矿化量表现为T3 > T1 > T2 > T4 > T5.有机碳累积矿化量(Ct)占沉积物有机碳(C0)的比例(Ct/C0)介于0.012~0.044之间,沉积物有机碳潜在排放量(Ci)占C0的比例(Ci/C0)介于0.018~0.045之间;水位降低,沉积物有机碳矿化常数(k值)减小,T1处理k值最大(0.137 d),T4处理最小(0.032 d).线性方程Cr=0.008x+0.488能较好地模拟有机碳矿化速率(Cr)与水位(x)的关系;不同水位处理有机碳矿化速率与模拟柱中沉积物5 cm温度呈显著的指数函数关系,T4、T5处理有机碳矿化温度敏感系数(Q10)显著高于T1、T2和T3处理,即水位降低增加了巴里坤湖干涸湖底沉积物Q10.因此,就巴里坤湖干涸湖底沉积物而言,水位从0 cm降至-45 cm时有机碳矿化速率降低,Q10增加;反之水位上升则会促进有机碳矿化分解,Q10降低.水位持续下降抑制有机碳矿化可能是维持干旱区盐湖沉积物碳库稳定的机制之一.  相似文献   

11.
双排桩计算方法探讨   总被引:4,自引:0,他引:4  
双排桩围护结构是一种新型的围护结构,这种结构具有较大的侧向刚度,可以有效地限制围护结构的变形,不必设置支撑,是深基坑支护结构的优选方案之一。但其实际受力机理比较复杂,前后排桩之间的土对结构的作用较难确定,针对这一问题,本文提出了一个新的计算模型,即将前、后排桩及桩间土视为一个整体;前排桩爱驻动土压力,基坑深度以下的后排桩受被动土压力,并进行了桩-接触面-土的非线性分析,提出了一些具有参考价值的结论。  相似文献   

12.
The transient dynamic response of single piles in a layered half-space under a time-dependent vertical force is analyzed by an FEM-BEM coupling approach. The pile is modeled by FEM and the layered half-space is modeled by a general cylindrical coordinates time-domain BEM. Only one-dimensional discretization is necessary on the boundaries of the three-dimensional layered half-space by virtue of the Fourier theory, while the pile shaft can be discretized as a one-dimensional elastic beam. The compatibility and equilibrium conditions between pile shaft and soil layers are employed to assemble respective equations into one. Fairly good agreement between two unknown solutions and the current approach is found. Parametric studies reveal the influences of several dimensionless factors, such as Ep/Es, l/r0, p/s and νs. The effect of soil layering and the support condition of the pile tip is also reported by numerical examples.  相似文献   

13.
高速铁路、地铁、轻轨等轨道交通迅速发展深入城市内部人群密集地区,对环境产生的振动影响不容忽视。空沟、碎石填充沟和排桩是三种常用的轨道交通隔振措施。通过大比例尺试验,采用加速度作为振动的评价指标,分别研究空沟、碎石填充沟和排桩的隔振效果。各组试验除隔振措施外其他条件均完全相同,使不同隔振措施的隔振效果具有较强的可比性,通过比较三种隔振措施与无隔振措施下影响区的加速度衰减率,评价其隔振效果,同时通过三种隔振措施下距离振源不同位置处的加速度比较其隔振效果。研究成果可为轨道交通隔振措施及方案的选取提供依据。  相似文献   

14.
The influence of nonlinearity on the dynamic response of cast-in-situ reinforced concrete piles subjected to strong vertical excitation was studied. Forced vibration test of single piles (L/d=10, 15, 20) and 2×2 pile groups (s/d=2, 3, 4 for each L/d) were conducted in the field for two different embedded conditions of pile cap. From the measured nonlinear response curves, the effective pile–soil system mass, stiffness and damping were determined and the nonlinear response curves were back-calculated using the theory of nonlinear vibration. The test results were compared with the continuum approach of Novak with dynamic interaction factor approach using both linear and linear-equivalent numerical methods. Reasonable match between the measured and predicted response was found for linear-equivalent methods by introducing a weak boundary-zone around the pile to approximately account for the nonlinear behaviour of pile–soil system. The test data were used to establish the empirical relationship in order to estimate the extent of soil separation around the pile with soil under vertical vibration.  相似文献   

15.
The behaviour under seismic loading of inclined piles embedded in two idealized soil profiles, a homogeneous and a non-homogenous “Gibson” soil, is analysed with 3D finite elements. Two structures, modeled as single-degree-of-freedom oscillators, are studied: (1) a tall slender superstructure (H st = 12 m) whose crucial loading is the overturning moment, and (2) a short structure (H st = 1 m) whose crucial loading is the shear force. Three simple two-pile group are studied: (a) one comprising a vertical pile and a pile inclined at 25°, (b) one consisting of two piles symmetrically inclined at 25°, and (c) a group of two vertical piles. The influence of key parameters is analysed and non-dimensional diagrams are presented to illustrate the role of raked piles on pile and structure response. It is shown that this role can be beneficial or detrimental depending on a number of factors, including the slenderness of the superstructure and the type of pile-to-cap connection.  相似文献   

16.
Summary Within each sunspot cycle the yearly means (A) of the daily sunspot areas increase faster than the corresponding sunspot numbers (R) from the minimum to the maximum of solar activity and then decrease also faster than these numbers till the next minimum. Relation (A)=16.7 (R), frequently used so far, is approximately valid only for the years in the vicinity of the sunspot maximum. Instead of that, author gives the relations: for the years preceding the sunspot maximum, for the years following the sunspot maximum, wherea andb are constants,T R is the time of rise of the corresponding sunspot cycle expressed in years, andk takes the valuek=0 for the year of maximum solar activity andk=1, 2, 3, ... for the first, second, third ... year preceding or following that of maximum solar activity. The monthly means of the daily sunspot areas show a similar variation, but in this case the ratioq=AR varies with a greater amplitude both within each sunspot cycle and from cycle to cycle. The values ofq corresponding to all months of a given year in the sunspot cycle are contained between two limits depending on the time of rise.
Résumé Les valeurs moyennes (A) des aires diurnes des taches solaires à chaque année depuis 1878 augmentent plus rapidement du minimum vers le maximum de l'activité solaire que les nombres de Wolf correspondants (R). Elles diminuent aussi plus rapidement que les nombres de Wolf du maximum vers le minimum de l'activité solaire. La relation adoptée (A)=16.7 (R) ne s'applique pas avec une approximation satisfaisante que seulement pour les années voisines celle du maximum de l'activité solaire. L'auteur propose les relations: pour les années qui précédent le maximum, pour les années qui suivent le maximum, oùa, b sont des constantes,T R le temps d'ascension du cycle correspondant exprimé en années et la parametrek prend la valeurk=0 à l'année du maximum de l'activité solaire etk=1, 2, 3 ... pour les années qui précédent et qui suivent celle du maximum. Les valeurs moyennes des aires diurnes des taches à chaque mois, suivent la même marche mais dans ce cas le rapportq=AR present des larges variations. Il oscille pourtant extre deux limites qui dependent du temps d'ascension.
  相似文献   

17.
This paper aims to develop an improved understanding of the critical response of structures to multicomponent seismic motion characterized by three uncorrelated components that are defined along its principal axes: two horizontal and the vertical component. An explicit formula, convenient for code applications, has been derived to calculate the critical value of structural response to the two principal horizontal components acting along any incident angle with respect to the structural axes, and the vertical component of ground motion. The critical response is defined as the largest value of response for all possible incident angles. The ratio rcr/rsrss between the critical value of response and the SRSS response—corresponding to the principal components of ground acceleration applied along the structure axes—is shown to depend on three dimensionless parameters: the spectrum intensity ratio γ between the two principal components of horizontal ground motion characterized by design spectra A(Tn) and γA(Tn); the correlation coefficient α of responses rx and ry due to design spectrum A(Tn) applied in the x‐ and y‐directions, respectively; and β = ry/rx. It is demonstrated that the ratio rcr/rsrss is bounded by 1 and . Thus the largest value of the ratio is , 1.26, 1.13 and 1.08 for γ = 0, 0.5, 0.75 and 0.85, respectively. This implies that the critical response never exceeds times the result of the SRSS analysis, and this ratio is about 1.13 for typical values of γ, say 0.75. The correlation coefficient α depends on the structural properties but is always bounded between −1 and 1. For a fixed value of γ, the ratio rcr/rsrss is largest if β = 1 and α = ±1. The parametric variations presented for one‐storey buildings indicate that this condition can be satisfied by axial forces in columns of symmetric‐plan buildings or can be approximated by lateral displacements in resisting elements of unsymmetrical‐plan buildings. Copyright © 2000 John Wiley & Sons, Ltd.  相似文献   

18.
Most laterally loaded piles are flexible in the sense that they are not deformed over their entire lengths. Instead, pile deflections become negligible below an ‘active pile length’ La. This La is an important parameter that governs the overall behavior of a rigidly capped pile group. In the present approach, piles closely grouped together beneath a superstructure are viewed as a single equivalent upright beam whose stiffness matrix determines La. This idea is verified for different cases of pile spacing, and is further extended for nonlinear behavior of soils surrounding grouped piles.  相似文献   

19.
By studying the pile-formula and stress-wave methods (e.g., CASE method), the authors propose a new method for testing piles using the single-impact energy and P-S curves. The vibration and wave figures are recorded, and the dynamic and static displacements are measured by different transducers near the top of piles when the pile is impacted by a heavy hammer or micro-rocket. By observing the transformation coefficient of driving energy (total energy), the consumed energy of wave motion and vibration and so on, the vertical bearing capacity for single pile is measured and calculated. Then, using the vibration wave diagram, the dynamic relation curves between the force (P) and the displacement (S) is calculated and the yield points are determined. Using the static-loading test, the dynamic results are checked and the relative constants of dynamic-static P-S curves are determined. Then the subsidence quantity corresponding to the bearing capacity is determined. Moreover, the shaped quality of the pile body can be judged from the formation of P-S curves. Foundation item: Key Projects of Tenth Five-year Plan of Yunnan Province (54-02-02).  相似文献   

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