標(biāo)題: Titlebook: Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface; G. A. Martynov,R. R. Salem Textbook 1983 Springer-Verlag Berlin [打印本頁(yè)] 作者: 征募 時(shí)間: 2025-3-21 18:02
書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface影響因子(影響力)
書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface影響因子(影響力)學(xué)科排名
書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface網(wǎng)絡(luò)公開(kāi)度
書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface網(wǎng)絡(luò)公開(kāi)度學(xué)科排名
書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface被引頻次
書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface被引頻次學(xué)科排名
書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface年度引用
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書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface讀者反饋
書(shū)目名稱Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface讀者反饋學(xué)科排名
作者: 不妥協(xié) 時(shí)間: 2025-3-21 22:32 作者: FATAL 時(shí)間: 2025-3-22 01:56 作者: receptors 時(shí)間: 2025-3-22 07:03 作者: Devastate 時(shí)間: 2025-3-22 10:48
,Charakteristik der R?hre (Ahb. 15),lute electrolyte solutions. Here we shall continue to analyse this system and show that it includes two dimensionless parameters: the dimensionless ion charge . and the dimensionless electrode charge .. As the electrolyte concentration decreases, . tends to zero, while . increases. Therefore, in the作者: Ptsd429 時(shí)間: 2025-3-22 13:20
https://doi.org/10.1007/978-3-642-60304-4II) and show that in the presence of specific adsorption forces this system leads to the Stern isotherm (in the preceding chapter we demonstrated that in the absence of these forces the systems leads to the Gouy-Chapman and Wagner-Onsager-Samaras equations). Thus, using system (81), (82), one can co作者: Ptsd429 時(shí)間: 2025-3-22 20:48 作者: 宴會(huì) 時(shí)間: 2025-3-22 22:12
https://doi.org/10.1007/978-3-642-60693-9ent on surface tension of a (liquid) electrode σ on the potential ., and also the differential capacity curves C.(.) for a metal-solution interface. Unfortunately, the information carried both by the former and the latter is identical, to a considerable extent. Indeed, it is known from thermodynamic作者: 浮雕 時(shí)間: 2025-3-23 01:30
https://doi.org/10.1007/978-3-662-25671-8be on its basis the most typical features of the zero-charge point (§ 20) and the integral capacity curves (§ 21). At the same time, we shall take every opportunity to compare theory and experiment (as we have already noted, the results of such a comparative analysis are not in favour of the theory)作者: 察覺(jué) 時(shí)間: 2025-3-23 09:28
Broder J. Merkel,Britta Planer-Friedrich of electrochemistry) of its existence has not been provided so far. The situation is quite different for the electronic capacitor. It does exist at a metal surface. This unambiguously follows from the physical facts reliably established long ago: namely, the existence of free conduction electrons i作者: Mystic 時(shí)間: 2025-3-23 12:42 作者: angina-pectoris 時(shí)間: 2025-3-23 14:27
Electrical Double Layer at a Metal-dilute Electrolyte Solution Interface978-3-642-48700-2Series ISSN 0342-4901 Series E-ISSN 2192-6603 作者: 下垂 時(shí)間: 2025-3-23 20:43 作者: UTTER 時(shí)間: 2025-3-24 00:19
Zur klinisch-therapeutischen Forschung,formal statistical theory much easier), and on the other hand, to prove that the classical theories alone are insufficient to explain a large number of experimental facts, so that further development of the theory is necessary.作者: uncertain 時(shí)間: 2025-3-24 03:53
https://doi.org/10.1007/978-3-662-25671-8be on its basis the most typical features of the zero-charge point (§ 20) and the integral capacity curves (§ 21). At the same time, we shall take every opportunity to compare theory and experiment (as we have already noted, the results of such a comparative analysis are not in favour of the theory).作者: 過(guò)份 時(shí)間: 2025-3-24 08:28
Classical Theories of Electrical Double Layerformal statistical theory much easier), and on the other hand, to prove that the classical theories alone are insufficient to explain a large number of experimental facts, so that further development of the theory is necessary.作者: 遍及 時(shí)間: 2025-3-24 10:41
Molecular Capacitorbe on its basis the most typical features of the zero-charge point (§ 20) and the integral capacity curves (§ 21). At the same time, we shall take every opportunity to compare theory and experiment (as we have already noted, the results of such a comparative analysis are not in favour of the theory).作者: 無(wú)情 時(shí)間: 2025-3-24 15:04 作者: admission 時(shí)間: 2025-3-24 20:45
ConclusionsNow we shall formulate in brief the main results.作者: 大雨 時(shí)間: 2025-3-25 00:37 作者: Triglyceride 時(shí)間: 2025-3-25 03:29 作者: 喚起 時(shí)間: 2025-3-25 08:01
0342-4901 Fur- thermore, we shall dwell at length on the comparison of the theory with experiment: without such a comparative analysis, any theory, however elegant it may978-3-540-11995-1978-3-642-48700-2Series ISSN 0342-4901 Series E-ISSN 2192-6603 作者: Ingenuity 時(shí)間: 2025-3-25 13:26
,Charakteristik der R?hre (Ahb. 15), non-zero electrode charge. Solving the latter system, we can find a correction to the Gouy-Chapman formula for the Gouy layer capacity. Comparison of the theory thus improved with experiment shows that ions with specific negative adsorption (NaF on X mercury) approach the electrode surface at a dis作者: Antigen 時(shí)間: 2025-3-25 18:14 作者: 種屬關(guān)系 時(shí)間: 2025-3-26 00:00 作者: 無(wú)聊的人 時(shí)間: 2025-3-26 02:13
Electrostatic Adsorption in the Gouy Layer non-zero electrode charge. Solving the latter system, we can find a correction to the Gouy-Chapman formula for the Gouy layer capacity. Comparison of the theory thus improved with experiment shows that ions with specific negative adsorption (NaF on X mercury) approach the electrode surface at a dis作者: 放氣 時(shí)間: 2025-3-26 07:54 作者: airborne 時(shí)間: 2025-3-26 08:46 作者: 瘋狂 時(shí)間: 2025-3-26 13:57 作者: tackle 時(shí)間: 2025-3-26 20:07 作者: figure 時(shí)間: 2025-3-26 22:57 作者: ASSAY 時(shí)間: 2025-3-27 03:38 作者: 誤傳 時(shí)間: 2025-3-27 07:00 作者: 硬化 時(shí)間: 2025-3-27 12:57 作者: Airtight 時(shí)間: 2025-3-27 14:36
Beschaffenheit und Beurteilung des Wassers,he capacitor plates). The model becomes a little more complicated in the case of specific adsorption, since two planes of maximum approach, rather than one, exist in this case (see § 7). We shall not, however, touch upon such details because in this section we shall consider, for the sake of simplicity, only surface-inactive electrolytes.作者: 接觸 時(shí)間: 2025-3-27 20:10
Introduction in the interpretation of electrochemical experiments, in the theory of stability of DLVO colloids ., in the theory of surface forces ., in the theory of electrokinetic phenomena ., etc. Actually, the Gouy-Chapman theory is at present one of the basic theories of the equilibrium double layer.作者: 圓柱 時(shí)間: 2025-3-28 00:10 作者: CURB 時(shí)間: 2025-3-28 05:31 作者: bromide 時(shí)間: 2025-3-28 07:26 作者: Nuance 時(shí)間: 2025-3-28 12:26 作者: 個(gè)阿姨勾引你 時(shí)間: 2025-3-28 18:36
Physical Principles of the Statistical Theory of the Double Layera to be described satisfactorily, especially at high electrolyte concentrations and electrode potentials, in solvents of low dielectric permittivity, and in the case of multi-charged ions. The situation is even worse with the Stern theory of specific adsorption, which cannot be used in practice for 作者: Oversee 時(shí)間: 2025-3-28 20:08
Electrostatic Adsorption in the Gouy Layerlute electrolyte solutions. Here we shall continue to analyse this system and show that it includes two dimensionless parameters: the dimensionless ion charge . and the dimensionless electrode charge .. As the electrolyte concentration decreases, . tends to zero, while . increases. Therefore, in the作者: Hectic 時(shí)間: 2025-3-29 02:50
Specific Adsorption in the Stern LayerII) and show that in the presence of specific adsorption forces this system leads to the Stern isotherm (in the preceding chapter we demonstrated that in the absence of these forces the systems leads to the Gouy-Chapman and Wagner-Onsager-Samaras equations). Thus, using system (81), (82), one can co作者: 悠然 時(shí)間: 2025-3-29 06:40 作者: crucial 時(shí)間: 2025-3-29 07:26
Experimental Dataent on surface tension of a (liquid) electrode σ on the potential ., and also the differential capacity curves C.(.) for a metal-solution interface. Unfortunately, the information carried both by the former and the latter is identical, to a considerable extent. Indeed, it is known from thermodynamic
