標題: Titlebook: Atomic Dynamics in Liquids; N. H. March,M. P. Tosi Textbook 1976Latest edition N. H. March and M. P. Tosi 1976 collision.elastic scatterin [打印本頁] 作者: 拼圖游戲 時間: 2025-3-21 16:37
書目名稱Atomic Dynamics in Liquids影響因子(影響力)
書目名稱Atomic Dynamics in Liquids影響因子(影響力)學科排名
書目名稱Atomic Dynamics in Liquids網絡公開度
書目名稱Atomic Dynamics in Liquids網絡公開度學科排名
書目名稱Atomic Dynamics in Liquids被引頻次
書目名稱Atomic Dynamics in Liquids被引頻次學科排名
書目名稱Atomic Dynamics in Liquids年度引用
書目名稱Atomic Dynamics in Liquids年度引用學科排名
書目名稱Atomic Dynamics in Liquids讀者反饋
書目名稱Atomic Dynamics in Liquids讀者反饋學科排名
作者: aerobic 時間: 2025-3-21 21:43
Static Structure and Thermodynamics,natomic. In eqn (1.1), .(.) is the atomic scattering factor, i.e. the Fourier transform of the electron density in the atom. .(.) falls from a value ., the atomic number, at . = 0 to zero at large ., the asymptotic behaviour being proportional to ..作者: 靈敏 時間: 2025-3-22 00:44 作者: 容易生皺紋 時間: 2025-3-22 07:56 作者: 銀版照相 時間: 2025-3-22 11:19 作者: Alpha-Cells 時間: 2025-3-22 13:46
Fuzzy Information and Engineering-2019ful for some purposes. We immediately confirm that, if we note that the ratio of the specific heats . for simple metals at their melting points is ～1.2 or 1.3, whereas for a hard-sphere like system such as argon . ～2.2 at the triple point.作者: oncologist 時間: 2025-3-22 20:57 作者: 船員 時間: 2025-3-23 00:21
Xiuqin Xu,Jialiang Xie,Shuili Chenso Kubo, 1966). It will be instructive to introduce this formalism through a study of the simplest time-dependent correlation function, which is the velocity autocorrelation function for a particle in a classical fluid, before proceeding to the discussion of .(.).作者: NAG 時間: 2025-3-23 05:21 作者: Affiliation 時間: 2025-3-23 06:56
Liquid Dynamics and Time-Dependent Correlation Functions,ent times. This function can be expressed in the form.The average of the . function involved in eqn (3.1) is obviously the probability that at time . the .th atom will be at . with respect to the position of the .th atom at time . = 0. We then sum this probability over . and average over .(.) is the space-time pair correlation function.作者: deficiency 時間: 2025-3-23 13:45 作者: Abnormal 時間: 2025-3-23 14:15
The Liquid Surface,), giving the number of molecules per unit volume at position .. Similarly, we define a two-body function .(., .) as the average density of pairs of molecules such that one molecule is situated in the element of volume d. and the other in d..作者: septicemia 時間: 2025-3-23 18:25 作者: apiary 時間: 2025-3-24 00:27 作者: 兵團 時間: 2025-3-24 06:15 作者: 火海 時間: 2025-3-24 07:35 作者: 闖入 時間: 2025-3-24 14:29
https://doi.org/10.1007/978-981-15-2459-2ons which were phonon-like for small wave vector and of a more complex (roton) character at larger wave vectors, around the peak of the static structure factor .(.) as needed to account for superfluid properties. This description was made fairly precise by the work of Feynman (1954), which we shall first briefly summarize.作者: maudtin 時間: 2025-3-24 17:08
https://doi.org/10.1007/978-1-349-00929-9collision; elastic scattering; molecule; particles; scattering作者: 反省 時間: 2025-3-24 22:56
N. H. March and M. P. Tosi 1976作者: 無法解釋 時間: 2025-3-25 00:50
Bipolar Fuzzy ,-ideals in ,-algebrasce the structure of a crystal is determined experimentally by observing the Bragg reflections of X-rays, it is natural to seek a quantitative description of the liquid structure via the intensity . of X-rays scattered through an angle 2. say, from the liquid. If we introduce the usual variable . = 4作者: 勾引 時間: 2025-3-25 04:12 作者: 使人入神 時間: 2025-3-25 08:45
Xiuqin Xu,Jialiang Xie,Shuili Chen (.) the meaning of their Fourier transforms as frequency spectra of dissipation by suitable external probes; (.) their relation to macroscopic fluid dynamics (i.e. hydrodynamics) and to transport coefficients in the limit .→0 and .→0; and (.) their short-time behaviour as expressible through moment作者: 軟膏 時間: 2025-3-25 15:25
Fuzzy Information and Engineering-2019sts that, for such systems with relatively soft cores and long-range forces, an approach using essentially independent density fluctuations may be useful for some purposes. We immediately confirm that, if we note that the ratio of the specific heats . for simple metals at their melting points is ～1.作者: blithe 時間: 2025-3-25 19:07 作者: 溝通 時間: 2025-3-25 20:38
Jing Ma,Gen-nian Sun,Sheng-quan Mady, even for liquid sodium, it is not correct in all respects—the liquid is evidently formed from singly-charged positive ions and conduction electrons. More obviously, no one would describe liquid lithium iodide without starting out from an ionic picture.作者: 咒語 時間: 2025-3-26 00:29 作者: expansive 時間: 2025-3-26 04:37
Decision-Making Under Fuzziness,parable. However, in this chapter we shall discuss the region near the critical point, where liquid and gas densities become comparable. Although the arguments we presented earlier relating the direct correlation function .(.) to the pair potential .(.) break down here, since the required inequality作者: 火花 時間: 2025-3-26 12:02
Conclusions and Future Directions,Most obviously, instead of the homogeneity of the one-body density in the bulk liquid, if we have a planar surface perpendicular to the . axis, then one of the basic quantities characterising the liquid surface is the density .(.). This, of course, is a particular case of a general local density .(.作者: Aboveboard 時間: 2025-3-26 15:32 作者: Adjourn 時間: 2025-3-26 20:10 作者: LINES 時間: 2025-3-26 23:32 作者: 母豬 時間: 2025-3-27 05:10
Helium Liquids,ons which were phonon-like for small wave vector and of a more complex (roton) character at larger wave vectors, around the peak of the static structure factor .(.) as needed to account for superfluid properties. This description was made fairly precise by the work of Feynman (1954), which we shall first briefly summarize.作者: 不要不誠實 時間: 2025-3-27 09:01
Static Structure and Thermodynamics,ce the structure of a crystal is determined experimentally by observing the Bragg reflections of X-rays, it is natural to seek a quantitative description of the liquid structure via the intensity . of X-rays scattered through an angle 2. say, from the liquid. If we introduce the usual variable . = 4作者: cuticle 時間: 2025-3-27 11:21
Liquid Dynamics and Time-Dependent Correlation Functions,n Hove 1954.). We argue purely classically at first. Suppose that we define .(.) as the average density of atoms at the point . at time ., if an atom was at the origin . = 0 at time . = O. Thus, .(.) gives us the correlation in the positions of two atoms, which may or may not be different, at differ作者: Insufficient 時間: 2025-3-27 15:31 作者: evaculate 時間: 2025-3-27 20:32 作者: 輕快帶來危險 時間: 2025-3-28 00:42
Structure and Dynamics of Binary Fluids,ralise, we shall present the treatment in terms of binary mixtures. The discussion, naturally enough, will start out with structure, at first static structure, but later we shall generalise this to dynamic properties.作者: 臨時抱佛腳 時間: 2025-3-28 03:14 作者: observatory 時間: 2025-3-28 07:56 作者: heirloom 時間: 2025-3-28 12:28
Critical Phenomena,parable. However, in this chapter we shall discuss the region near the critical point, where liquid and gas densities become comparable. Although the arguments we presented earlier relating the direct correlation function .(.) to the pair potential .(.) break down here, since the required inequality作者: Stress 時間: 2025-3-28 15:55 作者: PANT 時間: 2025-3-28 21:45
9樓作者: 值得 時間: 2025-3-29 02:50
9樓作者: 莎草 時間: 2025-3-29 05:39
9樓作者: 詢問 時間: 2025-3-29 08:07
10樓作者: exhibit 時間: 2025-3-29 14:23
10樓作者: 新字 時間: 2025-3-29 16:40
10樓作者: 改革運動 時間: 2025-3-29 20:20
10樓
