全文获取类型
收费全文 | 100篇 |
免费 | 8篇 |
国内免费 | 3篇 |
专业分类
化学 | 8篇 |
力学 | 15篇 |
综合类 | 2篇 |
数学 | 58篇 |
物理学 | 28篇 |
出版年
2021年 | 3篇 |
2020年 | 2篇 |
2019年 | 1篇 |
2018年 | 1篇 |
2017年 | 1篇 |
2016年 | 2篇 |
2015年 | 2篇 |
2014年 | 3篇 |
2013年 | 11篇 |
2012年 | 3篇 |
2011年 | 3篇 |
2010年 | 1篇 |
2009年 | 4篇 |
2008年 | 5篇 |
2007年 | 5篇 |
2006年 | 6篇 |
2005年 | 12篇 |
2004年 | 1篇 |
2003年 | 4篇 |
2002年 | 3篇 |
2001年 | 6篇 |
2000年 | 5篇 |
1999年 | 1篇 |
1998年 | 2篇 |
1997年 | 3篇 |
1996年 | 3篇 |
1995年 | 3篇 |
1994年 | 2篇 |
1993年 | 2篇 |
1992年 | 1篇 |
1990年 | 1篇 |
1989年 | 1篇 |
1986年 | 1篇 |
1984年 | 1篇 |
1983年 | 1篇 |
1982年 | 3篇 |
1981年 | 1篇 |
1976年 | 1篇 |
排序方式: 共有111条查询结果,搜索用时 15 毫秒
1.
促进其线性频散特征另一种形式的Bousinesq方程 总被引:5,自引:1,他引:5
Bousinesq方程能够用于模拟表面重力波传播过程中的折射、绕射、反射以及浅化,非线性作用等现象.用不同垂直积分方法所得到的二维Boussinesq方程形式具有不同的线性频散特征.采用两个不同的水深层的水平速度变量组合,推导出一个新形式的Bousinesq方程.通过对其参数的设置可得到精确的线性频散解Pade近似4阶精度.其适用范围已由原来的浅水,向深水拓进.相速误差小于2%,其拓展适用范围可达到08个波长水深.应用所得到的新型Bousinesq方程,采用有限差分法,对经典工况进行了数值模拟,其计算结果表明,计算值与物模实验值吻合较好.这说明本文新形式的Boussinesq方程对变水深非线性效应所产生的能量频散有着较为精确的描述 相似文献
2.
The amounts of decreased charge at Al sites of Al-based (Al–Pd–Cr–Fe, Al–Si–Mn, and Al–Re–Si) and at Zn sites of Zn-based (Zn–Mg–Zr) quasicrystals and approximant crystals were estimated. The evaluation was done by comparisons between chemical shifts experimentally observed by soft-X-ray emission spectroscopy and the amount of valence charge obtained by Bader analysis for first principle calculations of reference materials (Al, α-Al2O3, Zn, and ZnO). Decreased charges at Al sites of Al-based quasicrystals and at Zn sites of Zn-based quasicrystals were evaluated to be 1.0–2.5 e–/atom and 1.1–1.2 e–/atom, respectively. A covalent bonding nature alloy of Al–Re–Si also showed a decrease in valence charge at Al sites. 相似文献
3.
4.
促进其线性频散特征另一种形式的Bousinesq方程 总被引:1,自引:0,他引:1
Bousinesq方程能够用于模拟表面重力波传播过程中的折射、绕射、反射以及浅化,非线性作用等现象.用不同垂直积分方法所得到的二维Boussinesq方程形式具有不同的线性频散特征.采用两个不同的水深层的水平速度变量组合,推导出一个新形式的Bousinesq方程.通过对其参数的设置可得到精确的线性频散解Pade近似4阶精度.其适用范围已由原来的浅水,向深水拓进.相速误差小于2%,其拓展适用范围可达到08个波长水深.应用所得到的新型Bousinesq方程,采用有限差分法,对经典工况进行了数值模拟,其计算结果表明,计算值与物模实验值吻合较好.这说明本文新形式的Boussinesq方程对变水深非线性效应所产生的能量频散有着较为精确的描述 相似文献
5.
应用势流理论,采用递推函数方法推导出一个新形式的Bousinesq方程。通过对新方程的参数设置,可以讨论出Boussinesq方程发展趋势和不同的发展形式。对浅水波动的描述方程,Boussinesq方程的发展趋势为适用水深范围的拓展。拓展应用范围的大小则由其方程频散特征向Airy波频散解逼近程度来决定。而Bousineq方程又不同于Airy波,主要原因是Boussinesq方程中含有线性频散项,Airy波则只是长波首项近似,无线性频散项。其频散特征为精确的线性频散解。对实际水波传播而言,Airy波理论的局限性是不言而喻的。 相似文献
6.
The zero field cooled (ZFC) and field cooled (FC) low-field magnetic moment m of a dense frozen ferrofluid containing Fe55Co45 particles of size 4.6nm in hexane exhibits irreversibility at temperatures T?T b≈ 30?K. FC in μ 0 H ≤ 1?T gives rise to shifted minor hysteresis loops below T b. At T c≈ 10?K, sharp peaks of m ZFC and of the ac susceptibility χ ′, a kink of the thermoremanent magnetic moment m TRM, a sizeable reduction of the coercive field H c, and the appearance of a spontaneous moment m SFM indicate a phase transition with near mean-field critical behaviour of both m SFM and χ ′ . These features are explained within a core-shell model of nanoparticles, whose strongly disordered shells gradually become blocked below T b, while their soft ferromagnetic cores couple dipolarly and become superferromagnetic (SFM) below T c. 相似文献
7.
We analyze the emission spectrum of a single organic quantum dot coupled to a microcavity in the strong coupling regime. We take into account non-linearities arising from both exciton–exciton interactions and the Pauli exclusion principle. We apply the recently developed Pade approximation for regular truncation of Green functions to calculate the emission spectrum. We show that as the number of excitations in the quantum dot increases the Rabi doublet evolves into a more complicated triplet structure. 相似文献
8.
The Al45Cr7 compound is considered to exhibit an approximant structure of the icosahedral Al4Cr phase. Its (010) surface has been investigated in detail using density functional calculations. Surface energy calculations show that the stable terminations result from a cleavage of the crystal between adjacent atomic planes, in agreement with the layered structure of the compound. The integrity of the icosahedral atomic arrangements (icosahedral clusters) found in the bulk structure, is predicted to be removed at the surface. This result is in contrast to what has been previously concluded for the (010) surface of the Al13Fe4 quasicrystal approximant. Our findings are discussed in relation to the bonding network in the compound, calculated using the Crystal Orbital Hamiltonian Population approach, as possible reasons for such contrasted behavior. 相似文献
9.
The construction of homoclinic and heteroclinic orbitals in asymmetric strongly nonlinear systems based on the Pad''e approximant 下载免费PDF全文
In this paper, the extended Pad'e approximant is used to construct the homoclinic and the heteroclinic trajectories in nonlinear dynamical systems that are asymmetric at origin. Meanwhile, the conservative system, the autonomous system, and the nonautonomous system equations with quadratic and cubic nonlinearities are considered. The disturbance parameter varepsilon is not limited to being small. The ranges of the values of the linear and the nonlinear term parameters, which are variables, can be determined when the boundary values are satisfied. New conditions for the potentiality and the convergence are posed to make it possible to solve the boundary-value problems formulated for the orbitals and to evaluate the initial amplitude values. 相似文献
10.
The function-valued Padé-type approximant (FPTA) was defined in the inner product space [8]. In this work, we choose the coefficients in the Neumann power series to make the inner product with both sides a function-valued system of equations to yield a scalar system. Then we express an FPTA in the determinant form. To avoid the direct computation of the determinants, we present the E-algorithm for FPTA based on the vector-valued E-algorithm given by Brezinski [4]. The method of FPTA via E-algorithm (FPTAVEA) not only includes all previous methods but overcomes their essential difficulties. The numerical experiment for a typical integral equation [1] illustrates that the method of FPTAVEA is simpler and more effective for obtaining the characteristic values and the characteristic functions than all previous methods. In addition, this method is also applicable to other Fredholm integral equations of the second kind without explicit characteristic values and characteristic functions. A corresponding example [12] is given and the numerical result is the same as that in [12]. 相似文献