找回密碼
 To register

QQ登錄

只需一步,快速開始

掃一掃,訪問微社區(qū)

打印 上一主題 下一主題

Titlebook: Magnetohydrodynamic Modeling of the Solar Corona and Heliosphere; Xueshang Feng Book 2020 Springer Nature Singapore Pte Ltd. 2020 Solar an

[復(fù)制鏈接]
樓主: Coarctation
31#
發(fā)表于 2025-3-26 21:54:58 | 只看該作者
Data-Driven MHD Modeling of Solar Wind,ion. In fact, solar wind is constantly time varying. Data-driven modeling of solar wind here means to use continuously time-varying solar observations as input to drive models to produce solar wind background and reproduce eruptive process of solar active region, instead of using one instantaneous c
32#
發(fā)表于 2025-3-27 02:55:43 | 只看該作者
33#
發(fā)表于 2025-3-27 05:41:02 | 只看該作者
34#
發(fā)表于 2025-3-27 11:26:07 | 只看該作者
Modeling Coronal Mass Ejections by CESE MHD Model,dverse space weather disturbances that strongly affect our high-tech activities of humankind. Even the fastest CMEs require almost a day to arrive at Earth and initiate a geomagnetic storm. This allows, in principle, sufficient time to predict their impact. The geoeffectiveness of CMEs, that is, of
35#
發(fā)表于 2025-3-27 13:45:07 | 只看該作者
36#
發(fā)表于 2025-3-27 21:41:43 | 只看該作者
37#
發(fā)表于 2025-3-28 01:22:31 | 只看該作者
A Finite Volume MHD Code in Spherical Coordinates for Background Solar Wind, from generalized Lagrange multiplier (GLM) formulation of MHD system and constrained transport (CT) method, are employed. In this chapter, an FVM is described exemplarily on a six-component composite grid system by using a minmod limiter for oscillation control. Additionally, an implicit dual time-
38#
發(fā)表于 2025-3-28 02:52:50 | 只看該作者
3D SIP-CESE MHD Model on Triangular Prism Grids,that the MHD model possesses the ability to model the Sun-Earth environment. Finally, the evolution of the large-scale coronal magnetic structure during solar cycle 23 is investigated by the SIP-CESE MHD model.
39#
發(fā)表于 2025-3-28 09:47:52 | 只看該作者
3D SIP-CESE MHD Model on Six-Component Overset Grid System,l effect of the magnetic field expansion factor . and the minimum angular distance . (at the photosphere) between an open field foot point and its nearest coronal hole boundary. The simulation result for the 3D steady-state background solar wind during Carrington rotation (CR) 1911 from the Sun to E
40#
發(fā)表于 2025-3-28 12:46:38 | 只看該作者
 關(guān)于派博傳思  派博傳思旗下網(wǎng)站  友情鏈接
派博傳思介紹 公司地理位置 論文服務(wù)流程 影響因子官網(wǎng) 吾愛論文網(wǎng) 大講堂 北京大學(xué) Oxford Uni. Harvard Uni.
發(fā)展歷史沿革 期刊點(diǎn)評(píng) 投稿經(jīng)驗(yàn)總結(jié) SCIENCEGARD IMPACTFACTOR 派博系數(shù) 清華大學(xué) Yale Uni. Stanford Uni.
QQ|Archiver|手機(jī)版|小黑屋| 派博傳思國(guó)際 ( 京公網(wǎng)安備110108008328) GMT+8, 2025-10-12 06:28
Copyright © 2001-2015 派博傳思   京公網(wǎng)安備110108008328 版權(quán)所有 All rights reserved
快速回復(fù) 返回頂部 返回列表
定襄县| 徐水县| 桓仁| 鄂尔多斯市| 邛崃市| 钦州市| 宜川县| 神木县| 南召县| 武冈市| 明水县| 东宁县| 康乐县| 渝北区| 万年县| 大宁县| 浪卡子县| 吉首市| 辛集市| 云南省| 缙云县| 衡水市| 永胜县| 涞水县| 开化县| 昌宁县| 巴里| 海阳市| 凯里市| 杭锦后旗| 牟定县| 庄河市| 剑阁县| 大理市| 平远县| 子洲县| 芒康县| 海兴县| 明溪县| 上犹县| 邹城市|