標(biāo)題: Titlebook: Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas; John Rice Book 2022 Springer Nature Switzerland AG 2022 r [打印本頁(yè)] 作者: affidavit 時(shí)間: 2025-3-21 19:02
書(shū)目名稱(chēng)Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas影響因子(影響力)
書(shū)目名稱(chēng)Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas影響因子(影響力)學(xué)科排名
書(shū)目名稱(chēng)Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas網(wǎng)絡(luò)公開(kāi)度
書(shū)目名稱(chēng)Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas網(wǎng)絡(luò)公開(kāi)度學(xué)科排名
書(shū)目名稱(chēng)Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas被引頻次
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書(shū)目名稱(chēng)Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas讀者反饋
書(shū)目名稱(chēng)Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas讀者反饋學(xué)科排名
作者: wreathe 時(shí)間: 2025-3-21 20:51 作者: BRINK 時(shí)間: 2025-3-22 00:28
Management und Managerkompetenzens acting in the direction opposite to the ambient velocity, a true momentum sink is one that damps the magnitude of the rotation regardless of the initial state. Two examples of sinks will be treated in this section: neutral damping (Sect. 3.1) and magnetic braking (Sect. 3.2) due to neo-classical t作者: stress-response 時(shí)間: 2025-3-22 06:27
Management und Managerkompetenzen and sinks will be compared to the predictions of neo-classical theory, which accounts for collisions in the tokamak geometry. The momentum diffusivity (Chap. .) observed in experiments is generally found to be anomalously large compared to neo-classical levels so it is prudent to check measured tor作者: 含沙射影 時(shí)間: 2025-3-22 09:40 作者: 會(huì)犯錯(cuò)誤 時(shí)間: 2025-3-22 16:20 作者: 會(huì)犯錯(cuò)誤 時(shí)間: 2025-3-22 19:52
Führen Sie die Dinge mit Erfolg durch!st and not even qualitative at worst. Even in the most fundamental example of direct external drive (Sect. .), a substantial fraction of the rotation observed following NBI is not in fact due to direct drive from the beams. As has been shown in DIII-D H-mode plasmas, the intrinsic torque is as large作者: 紡織品 時(shí)間: 2025-3-22 22:12
John RiceRepresents the first book-length work on the subject of rotation and momentum transport in tokamak plasmas.Provides a comprehensive review of all relevant observations, from the original to the most r作者: JADED 時(shí)間: 2025-3-23 03:01
Springer Series on Atomic, Optical, and Plasma Physicshttp://image.papertrans.cn/e/image/282898.jpg作者: 荒唐 時(shí)間: 2025-3-23 07:56
Driven Rotation, Self-Generated Flow, and Momentum Transport in Tokamak Plasmas978-3-030-92266-5Series ISSN 1615-5653 Series E-ISSN 2197-6791 作者: 恩惠 時(shí)間: 2025-3-23 12:19
https://doi.org/10.1007/978-3-030-92266-5rotation measurement; rotation measurement techniques; directly driven rotation; indirectly driven rota作者: THE 時(shí)間: 2025-3-23 17:41
978-3-030-92268-9Springer Nature Switzerland AG 2022作者: triptans 時(shí)間: 2025-3-23 18:25 作者: Externalize 時(shí)間: 2025-3-23 23:41 作者: extrovert 時(shí)間: 2025-3-24 06:20
Momentum Sinks,tial state. Two examples of sinks will be treated in this section: neutral damping (Sect. 3.1) and magnetic braking (Sect. 3.2) due to neo-classical toroidal viscosity (NTV) resulting from non-axisymmetric magnetic fields. The effects of edge localized modes (ELMs) on rotation are considered in Sect. 3.3.作者: Cleave 時(shí)間: 2025-3-24 07:27
https://doi.org/10.1007/978-3-322-94562-4mbipolar radial particle shifts or orbit losses (Sect. 2.2), the latter due to toroidal magnetic field ripple for example. Direct rotation drive can be from neutral beam injection, transfer of momentum from radio frequency waves (ICRF, LH or EC) or from neutral gas or compact torus injection.作者: 該得 時(shí)間: 2025-3-24 12:51
Das Gesetz der Einstellungs-Annuit?tree parameters. In certain circumstances it is possible to isolate each of the three, or two of the three, and the results will be covered in Sects. 6.1, 6.2, and 6.3, respectively, with a comparison to theory in Sect. 6.4作者: GOAD 時(shí)間: 2025-3-24 18:36 作者: CLIFF 時(shí)間: 2025-3-24 21:38 作者: magnate 時(shí)間: 2025-3-25 01:19
Management und Managerkompetenzential state. Two examples of sinks will be treated in this section: neutral damping (Sect. 3.1) and magnetic braking (Sect. 3.2) due to neo-classical toroidal viscosity (NTV) resulting from non-axisymmetric magnetic fields. The effects of edge localized modes (ELMs) on rotation are considered in Sect. 3.3.作者: 成份 時(shí)間: 2025-3-25 04:38 作者: 惡意 時(shí)間: 2025-3-25 09:41 作者: 截?cái)?nbsp; 時(shí)間: 2025-3-25 15:32
Comparison with Neo-Classical Theory, Helander (Phys Plasmas 13:102505, 2006), and Wong et al. (Phys Plasmas 15:082503, 2008) and have been incorporated into a variety of codes including NCLASS, HAGIS, NEOART and NEO. In Sect. 4.3, edge poloidal asymmetries will be addressed.作者: 卵石 時(shí)間: 2025-3-25 19:41
Momentum Sources,mbipolar radial particle shifts or orbit losses (Sect. 2.2), the latter due to toroidal magnetic field ripple for example. Direct rotation drive can be from neutral beam injection, transfer of momentum from radio frequency waves (ICRF, LH or EC) or from neutral gas or compact torus injection.作者: 放氣 時(shí)間: 2025-3-25 22:16
Momentum Transport,ree parameters. In certain circumstances it is possible to isolate each of the three, or two of the three, and the results will be covered in Sects. 6.1, 6.2, and 6.3, respectively, with a comparison to theory in Sect. 6.4作者: 罵人有污點(diǎn) 時(shí)間: 2025-3-26 02:29 作者: 過(guò)多 時(shí)間: 2025-3-26 07:40
Entscheidungsfindung und Handelnples will be provided in this section of how the rotation can be driven by changes in various gradients, as well as the collisionality and magnetic configuration, using external heating and current drive, and in Ohmic plasmas. In the absence of external momentum sources, if the initial velocity and 作者: Debrief 時(shí)間: 2025-3-26 08:59 作者: Hyperplasia 時(shí)間: 2025-3-26 13:40 作者: 聲音刺耳 時(shí)間: 2025-3-26 17:02 作者: 隨意 時(shí)間: 2025-3-27 00:03 作者: Atheroma 時(shí)間: 2025-3-27 03:58 作者: 令人發(fā)膩 時(shí)間: 2025-3-27 09:11
Momentum Sources,rize momentum transport, the subject of Chap. .. In order to achieve this, momentum sources must first be understood. These sources fall into two general categories: direct momentum input from particle or wave interactions (Sect. 2.1) and indirect drive such as from the .×. forces arising from non-a作者: 減震 時(shí)間: 2025-3-27 09:28 作者: 音樂(lè)戲劇 時(shí)間: 2025-3-27 16:17
Comparison with Neo-Classical Theory, and sinks will be compared to the predictions of neo-classical theory, which accounts for collisions in the tokamak geometry. The momentum diffusivity (Chap. .) observed in experiments is generally found to be anomalously large compared to neo-classical levels so it is prudent to check measured tor作者: deactivate 時(shí)間: 2025-3-27 21:42
,Intrinsic Rotation and the Residual Stress Πres, stress, Π.. Diffusion and convection are strictly momentum transport coefficients which can affect the rotation profile shape and evolution, but cannot act as a momentum source. Multiple experiments have measured these, and they will be covered in detail in Chap. .. A unique feature of the third te作者: 宣傳 時(shí)間: 2025-3-28 01:53 作者: staging 時(shí)間: 2025-3-28 02:31 作者: myocardium 時(shí)間: 2025-3-28 09:14 作者: 無(wú)法解釋 時(shí)間: 2025-3-28 11:57
