標(biāo)題: Titlebook: Elementary Lectures in Statistical Mechanics; George D. J. Phillies Textbook 2000 Springer-Verlag New York, Inc. 2000 classical systems.co [打印本頁] 作者: 分期 時(shí)間: 2025-3-21 19:39
書目名稱Elementary Lectures in Statistical Mechanics影響因子(影響力)
書目名稱Elementary Lectures in Statistical Mechanics影響因子(影響力)學(xué)科排名
書目名稱Elementary Lectures in Statistical Mechanics網(wǎng)絡(luò)公開度
書目名稱Elementary Lectures in Statistical Mechanics網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Elementary Lectures in Statistical Mechanics被引頻次
書目名稱Elementary Lectures in Statistical Mechanics被引頻次學(xué)科排名
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書目名稱Elementary Lectures in Statistical Mechanics年度引用學(xué)科排名
書目名稱Elementary Lectures in Statistical Mechanics讀者反饋
書目名稱Elementary Lectures in Statistical Mechanics讀者反饋學(xué)科排名
作者: 煩憂 時(shí)間: 2025-3-21 21:36 作者: CHARM 時(shí)間: 2025-3-22 03:09
Ensembles: Fundamental Principles of Statistical Mechanics, either time averages or ensemble averages, can be made in a straightforward manner. In contrast, to make a time average via a theoretical calculation on a model requires that one integrates vast numbers of differential equations and that one supplies equally vast numbers of experimentally inaccess作者: hysterectomy 時(shí)間: 2025-3-22 08:22
The One-Atom Ideal Gastical simplicity, this Lecture considers a system which contains only one gas atom, Aside A shows what happens if the system contains two atoms. Lecture 5 extends the treatment to .-atom systems, while Lecture 6 treats atom-wall interactions, thereby obtaining the gas pressure. The calculations repr作者: LOPE 時(shí)間: 2025-3-22 09:40
The Two-Atom Ideal Gasween the one-atom ideal gas discussed in Lecture 4, and the .-atom (where . might be similar to Avogadro’s number) ideal gas treated in Lecture 5. In this Aside, I develop the canonical ensemble description of the two-atom ideal gas. I show how the lists of variables and integrals change form as the作者: Mutter 時(shí)間: 2025-3-22 12:55
N-Atom Ideal Gasystem of . such atoms. We could have gone directly from Lecture 3 to the calculation below, and skipped Lecture 4 and the Aside. There would have been a pedagogical penalty; our first serious calculation would have involved 6.-dimensional integrals for. Lecture 4 already involved quite enough new id作者: Mutter 時(shí)間: 2025-3-22 20:40 作者: Horizon 時(shí)間: 2025-3-22 22:05
How Do Thermometers Work?—The Polythermal Ensembleergy, the mean-square energy and mean-square energy fluctuation, and the import of fluctuations for experimental measurements of ..We then used three separate paths to compute the pressure of an ideal gas, finding that these paths gave the same answer to all questions on which agreement should have 作者: LINE 時(shí)間: 2025-3-23 05:25 作者: 蚊帳 時(shí)間: 2025-3-23 07:04 作者: 刺激 時(shí)間: 2025-3-23 12:50
Open Systems; Grand Canonical Ensemblenor decrease. This Lecture treats open systems in which particles may enter or leave the system. Open systems arise naturally in experiment. For example, if one studies a large volume of liquid by using a microscope with a narrow field of view, the small unenclosed volume under examination is an ope作者: 征服 時(shí)間: 2025-3-23 15:49 作者: magnanimity 時(shí)間: 2025-3-23 19:42 作者: 占線 時(shí)間: 2025-3-24 01:33
Quantum Mechanicstical mechanics were used to compute partition functions, average energies, and specific heats for rigid rotators, noninteracting spins in an external field, and quantum harmonic oscillators such as those found in crystalline solids. The objective in this Aside and the next Lecture is to give these 作者: Insatiable 時(shí)間: 2025-3-24 03:14
Formal Quantum Statistical Mechanics. The analysis is in two parts. The first, more conventional, part will show why a sum over energy eigenstates is an appropriate procedure for evaluating ensemble averages, and why your decision to use a particular set of basis vectors has no effect on the number you get when you calculate the ensem作者: constitute 時(shí)間: 2025-3-24 06:36 作者: UTTER 時(shí)間: 2025-3-24 13:06 作者: 裂隙 時(shí)間: 2025-3-24 16:35 作者: Conduit 時(shí)間: 2025-3-24 21:36
Sensing Ice Clouds from Satellitesween the one-atom ideal gas discussed in Lecture 4, and the .-atom (where . might be similar to Avogadro’s number) ideal gas treated in Lecture 5. In this Aside, I develop the canonical ensemble description of the two-atom ideal gas. I show how the lists of variables and integrals change form as the number of particles in the system is increased.作者: 共同生活 時(shí)間: 2025-3-25 02:32 作者: 委托 時(shí)間: 2025-3-25 03:33 作者: Spinal-Tap 時(shí)間: 2025-3-25 10:18
The Two-Atom Ideal Gasween the one-atom ideal gas discussed in Lecture 4, and the .-atom (where . might be similar to Avogadro’s number) ideal gas treated in Lecture 5. In this Aside, I develop the canonical ensemble description of the two-atom ideal gas. I show how the lists of variables and integrals change form as the number of particles in the system is increased.作者: FOR 時(shí)間: 2025-3-25 12:37 作者: 細(xì)絲 時(shí)間: 2025-3-25 19:12
How Do Thermometers Work?—The Polythermal Ensembleergy, the mean-square energy and mean-square energy fluctuation, and the import of fluctuations for experimental measurements of ..We then used three separate paths to compute the pressure of an ideal gas, finding that these paths gave the same answer to all questions on which agreement should have been expected.作者: 討好美人 時(shí)間: 2025-3-25 20:35
Graduate Texts in Contemporary Physicshttp://image.papertrans.cn/e/image/307388.jpg作者: 中古 時(shí)間: 2025-3-26 04:05 作者: 錯(cuò)誤 時(shí)間: 2025-3-26 04:43 作者: 詼諧 時(shí)間: 2025-3-26 12:30
Light Pollution in MetropolisesMacroscopic” properties are those properties that can be obtained without having a detailed knowledge of atomic coordinates. Traditional thermodynamic quantities such as pressure, temperature, entropy, and free energy are macroscopic variables. By a “l(fā)arge system,” I mean a system whose complete mec作者: 一起 時(shí)間: 2025-3-26 12:40
Light Scattering Reviews, Vol. 6, either time averages or ensemble averages, can be made in a straightforward manner. In contrast, to make a time average via a theoretical calculation on a model requires that one integrates vast numbers of differential equations and that one supplies equally vast numbers of experimentally inaccess作者: Gobble 時(shí)間: 2025-3-26 19:06
Theory of Optical Processes in Liquid Heliumtical simplicity, this Lecture considers a system which contains only one gas atom, Aside A shows what happens if the system contains two atoms. Lecture 5 extends the treatment to .-atom systems, while Lecture 6 treats atom-wall interactions, thereby obtaining the gas pressure. The calculations repr作者: 臥虎藏龍 時(shí)間: 2025-3-26 22:25 作者: 惡心 時(shí)間: 2025-3-27 02:38
Atmosphere of Finite Optical Thicknessystem of . such atoms. We could have gone directly from Lecture 3 to the calculation below, and skipped Lecture 4 and the Aside. There would have been a pedagogical penalty; our first serious calculation would have involved 6.-dimensional integrals for. Lecture 4 already involved quite enough new id作者: brassy 時(shí)間: 2025-3-27 07:26
C. Allain,P. Lallemand,J. P. Boon force per unit area that a gas exerts on the walls of its container. This Lecture presents three physically distinct calculations of ..The first calculation uses a direct approach based on Gibbs’s ensemble method. In a second calculation, . is obtained by a thermodynamic derivative from a free ener作者: Expiration 時(shí)間: 2025-3-27 12:49
Ultraslow Optical Dephasing of Pr3+:LaF3ergy, the mean-square energy and mean-square energy fluctuation, and the import of fluctuations for experimental measurements of ..We then used three separate paths to compute the pressure of an ideal gas, finding that these paths gave the same answer to all questions on which agreement should have 作者: assent 時(shí)間: 2025-3-27 13:59 作者: adduction 時(shí)間: 2025-3-27 18:26
Masayoshi Nakasako,Satoru Tokutomically presented these results in 200 tightly-worded pages of his book [1], on which this section is based. In the following, Gibbs’s language (but not his notation) has generally been modernized; all paraphrases and quotes are from Gibbs’s volume. There are several points at which modern sources pla作者: Forehead-Lift 時(shí)間: 2025-3-27 22:19 作者: 話 時(shí)間: 2025-3-28 02:19
https://doi.org/10.1007/3-7643-7829-8mber and . being the gas constant. In testing this equation, . is a known parameter, since it also appears in the ideal gas law . (10.2) . being the number of moles of gas present. When (10.1) was first developed, the sole known monoatomic gas was mercury; the specific heat of mercury vapor is in ac作者: resilience 時(shí)間: 2025-3-28 09:45
Afterimages and Contrast Phenomena,hallenge to the statistical mechanics of Gibbs, since experimentally the specific heat .. of a diatomic ideal gas is consistently, while the theoretical specific heat of the same material, computed within the confines of classical statistical mechanics, was irreducibly at least. Only with the advent作者: Rebate 時(shí)間: 2025-3-28 11:57 作者: 規(guī)范要多 時(shí)間: 2025-3-28 15:00
Light and Specular Microscopy of the Cornea. The analysis is in two parts. The first, more conventional, part will show why a sum over energy eigenstates is an appropriate procedure for evaluating ensemble averages, and why your decision to use a particular set of basis vectors has no effect on the number you get when you calculate the ensem作者: 允許 時(shí)間: 2025-3-28 20:40 作者: Extricate 時(shí)間: 2025-3-29 00:28
978-1-4612-7068-3Springer-Verlag New York, Inc. 2000作者: obscurity 時(shí)間: 2025-3-29 06:00 作者: 提名的名單 時(shí)間: 2025-3-29 10:32 作者: pellagra 時(shí)間: 2025-3-29 11:32 作者: 原始 時(shí)間: 2025-3-29 17:51 作者: 結(jié)構(gòu) 時(shí)間: 2025-3-29 22:10 作者: beta-cells 時(shí)間: 2025-3-30 00:58 作者: inflate 時(shí)間: 2025-3-30 05:31
Light-at-Night (LAN) as a General Stressorence to the possible validity of the atomic hypothesis, and quantum mechanics, which treats the electronic structure of single molecules but does not readily treat systems containing substantial numbers of unbonded atoms.作者: 完成 時(shí)間: 2025-3-30 10:40 作者: Jejune 時(shí)間: 2025-3-30 13:27
Light Scattering Reviews, Vol. 6ible initial conditions. Lecture 2 concluded by suggesting that a more attractive way to develop the theory would be to replace the operational average with an idealized average. The required average is the ensemble average developed below.作者: persistence 時(shí)間: 2025-3-30 20:02 作者: 結(jié)合 時(shí)間: 2025-3-31 00:30
C. Allain,P. Lallemand,J. P. Boongy. Finally, . will be found using a kinetic argument, based on counting collisions of gas molecules with container walls over a period of time. All three approaches give the ideal gas law..=... (6.1) in the appropriate limits.作者: considerable 時(shí)間: 2025-3-31 01:27 作者: 嘴唇可修剪 時(shí)間: 2025-3-31 05:38
https://doi.org/10.1007/978-3-031-27391-9n system, because particles are free to enter or leave an unenclosed volume. Systems with ongoing chemical equilibria may usefully be said to be open, in the sense that a molecule of a species ceases to be present within the volume when it turns into a molecule of a different species.作者: GIST 時(shí)間: 2025-3-31 10:03
Doppler Effects, Redshifts, and Blueshifts does not create a new state of the system, which has implications for the contents of the complete nonrepeating list of states that constitutes an ensemble. If the particles follow Fermi-Dirac statistics, then a maximum of one particle can be found in each quantum state.作者: 極端的正確性 時(shí)間: 2025-3-31 13:50 作者: squander 時(shí)間: 2025-3-31 19:49
0938-037X tive is to treat classical statistical mechanics and its modem applications, especially interacting particles, correlation functions, and time-dependent phenomena. My development is based primarily on Gibbs‘s ensemble formulation. Elementary Lectures in Statistical Mechanics is meant as a (relativel作者: insular 時(shí)間: 2025-4-1 01:00
Masayoshi Nakasako,Satoru Tokutomi his notation) has generally been modernized; all paraphrases and quotes are from Gibbs’s volume. There are several points at which modern sources place odd readings on Gibbs’s words, notably with respect to the so-called “Gibbs Paradox,” which is not due to Gibbs and which Gibbs explicitly saw as not entailing a paradox.
