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1.
A new method is introduced to solve potential flow problems around axisymmetric bodies. The approach relies on expressing the infinite series expansion of the Laplace equation solution in terms of a finite sum which preserves the Laplace solution for the potential function under a Neumann-type boundary condition. Then the coefficients of the finite sum are calculated in a least squares approximation sense using the Gram-Schmidt orthonormalization method. Sample benchmark problems are presented and discussed in some detail. The solutions are accurate and converged faster when a rather small number of terms were used. The method is simple and can be easily programmed.  相似文献   
2.
If A q(β, α, k) is the scattering amplitude, corresponding to a potential , where D⊂ℝ3 is a bounded domain, and is the incident plane wave, then we call the radiation pattern the function , where the unit vector α, the incident direction, is fixed, β is the unit vector in the direction of the scattered wave, and k>0, the wavenumber, is fixed. It is shown that any function , where S 2 is the unit sphere in ℝ3, can be approximated with any desired accuracy by a radiation pattern: , where ∊ >0 is an arbitrary small fixed number. The potential q, corresponding to A(β), depends on f and ∊, and can be calculated analytically. There is a one-to-one correspondence between the above potential and the density of the number of small acoustically soft particles D mD, 1≤ mM, distributed in an a priori given bounded domain D⊂ℝ3. The geometrical shape of a small particle D m is arbitrary, the boundary S m of D m is Lipschitz uniformly with respect to m. The wave number k and the direction α of the incident upon D plane wave are fixed. It is shown that a suitable distribution of the above particles in D can produce the scattering amplitude , at a fixed k>0, arbitrarily close in the norm of L 2(S 2× S 2) to an arbitrary given scattering amplitude f(α ', α), corresponding to a real-valued potential qL 2(D), i.e., corresponding to an arbitrary refraction coefficient in D. MSC: 35J05, 35J10, 70F10, 74J25, 81U40, 81V05, 35R30. PACS: 03.04.Kf.  相似文献   
3.
Diffusion from spherical bodies has been a subject of interest since the earliest times of modern sciences and a few equivalent analytical formulations of the problem are taught in engineering textbooks dealing with cooling rates of hot spheres. However, all these former studies assume that the diffusing material is transferable to/from the surrounding space through the whole surface of the spherical body. Conversely, the development of nanoscience and the improved knowledge of microscopic biological events have evidenced that diffusion from spherical bodies is a ubiquitous problem. It often occurs in situations where the nanosphere surfaces are not isotropic and partly impermeable to diffusing materials. This work elaborates on this issue and theoretically establishes that—with some specific allowance—the basic analytical equation of diffusion from/to fully accessible spherical bodies may be used.  相似文献   
4.
5.
Using M-addition,an asymmetric Orlicz centroid inequality for absolutely continuous probability measures is established corresponding to Paouris and Pivovarov’s recent result on the symmetric case.As an application,we extend Haberl and Schuster’s asymmetric Lp centroid inequality from star bodies to compact sets.  相似文献   
6.
Duals of the basic projection and mixed projection inequalities are established for intersection and mixed intersection bodies.   相似文献   
7.
直接敏感地平是一种典型自主天文导航方法,该方法简单可靠,易于实现,但是由于常用卫星轨道动力学J2模型精度有限,地球敏感器精度较低,因此导航精度不高。加速度计是测量运载体线加速度的常用惯性导航设备,当航天器在轨运行时,星载加速度计能够测量航天器所受发散力。结合上述两种方法的特点,提出一种将加速度计和天文相结合的自主天文导航新方法。在常用卫星轨道动力学模型基础上,引入大气阻力和太阳光压系数模型作为自主导航系统状态方程的一部分,并建立近地空间环境下星载加速度计的测量模型,将其与直接敏感地平均作为导航系统观测方程。设计基于信息融合的自主导航滤波方法,通过对多种导航模式进行数值仿真及结果分析,结果表明所设计方法提高了系统定位精度62.8%和速度精度63.9%,增强了系统可靠性。  相似文献   
8.
The Busemann–Petty problem asks whether origin-symmetric convex bodies in Rn with smaller areas of all central hyperplane sections necessarily have smaller n-dimensional volume. The solution was completed in the end of the 1990s, and the answer is affirmative if n4 and negative if n5. Since the answer is negative in most dimensions, it is natural to ask what information about the volumes of central sections of two bodies does allow to compare the n-dimensional volumes of these bodies in all dimensions. In this article we give an answer to this question in terms of certain powers of the Laplace operator applied to the section function of the body.  相似文献   
9.
GJ 436b is a Neptune-size planet with 23.2 Earth masses in an elliptical orbit of period 2.64 days and eccentricity 0.16. With a typical tidal dissipation factor (Q′∼106) as that of a giant planet with convective envelope, its orbital circularization timescale under internal tidal dissipation is around 1 Ga, at least two times less than the stellar age (> 3 Ga). A plausible mechanism is that the eccentricity of GJ 436b is modulated by a planetary companion due to their mutual perturbation. Here we investigate this possibility from the dynamical viewpoint. A general method is given to predict the possible locations of the dynamically coupled companions, including nearby/distance non-resonant or mean motion resonance orbits with the first planet. Applying the method to GJ 436 system, we find it is very unlikely that the eccentricity of GJ 436b is maintained at the present location by a nearby/distance companion through secular perturbation or mean motion resonance. In fact, in all these simulated cases, GJ 436b will undergo eccentricity damp and orbital decay, leaving the present location within the stellar age. However, these results do not rule out the possible existence of planet companions in nearby/distance orbits, although they are not able to maintain the eccentricity of GJ 436b. Supported by the National Natural Science Foundation of China (Grant Nos. 10833001 and 10778603) and the National Basic Research Program of China (Grant No. 2007CB4800)  相似文献   
10.
    
The nematode spermatozoa represent a highly modified (aberrant) type of male gametes that lack a flagellum but for which the process of spermatogenesis culminates in the production of a crawling spermatozoon on the basis of the cytoskeletal component known as “major sperm protein”, or MSP. MSP is also known as an important hormone triggering oocyte maturation and ovulation in the model nematode Caenorhabditis elegans, where this protein was first identified. However, direct evidence of MSP localization and of its fate in nematode spermatogenic cells is rare. In this study, the spermatogenesis and sperm structure in the rhabditid nematode Acrobeles complexus (Rhabditida: Tylenchina: Cephalobomorpha: Cephaloboidea: Cephalobidae) has been examined with electron microscopy. Morphological observations were followed by high-pressure freezing and freeze-substitution fixation which allows post-embedding immunogold localization of MSP in all stages of sperm development using antibodies raised for MSP of C. elegans. In spermatocytes, synthetic activity results in the development of specific cellular components, fibrous bodies (FB) and membranous organelles (MO), which appear as FB-MO complexes where the filamentous matter of FB has been MSP-labeled. The spermatids subdivide into a residual body with superfluous cytoplasm, and a main cell body which contains nucleus, mitochondria and FB-MO complexes. These complexes dissociate into individual components, MO and FB, with the MSP being localized in FB. Immature spermatozoa from testes are opaque cells where a centrally located nucleus is surrounded by mitochondria, MO and FB clustered together, the MSP still being localized only in FB. Cytoplasm of mature spermatozoa from spermatheca is segregated into external pseudopods lacking organelles and a central cluster of mitochondria with intact MO surrounding the central nucleus. The FB ultimately disappear, and the MSP labeling becomes concentrated in the filamentous content of pseudopods and cytoplasm of the main cell body. Although the spermatogenesis and sperm structure of A. complexus is similar to that of many other rhabditid nematodes, their intact MO makes the morphology of the mature spermatozoa distinct from the “rhabditid pattern” and may be considered as a synapomorphy. The MSP localization in spermatogenic cells of A. complexus also follows the “rhabditid pattern” described in C. elegans and Ascaris spp. Our results and techniques of MSP labeling of A. complexus spermatogeneous cells reveal new possibilities to elucidate different research questions on MSP localization in nematodes related to C. elegans. Furthermore, the laboratory-cultured A. complexus strains can be used as a new and fascinating model to study MO and MSP functions in nematode reproduction.  相似文献   
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