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Cyclic Processes And Isolated Systems01:19

Cyclic Processes And Isolated Systems

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A thermodynamic system with zero heat exchange and work is an isolated system. For these systems, the internal energy remains constant.
In the case of a non-isolated system, the change in the internal energy is zero only if the process is cyclic. A thermodynamic process is considered cyclic if the system undergoes a series of changes and returns to its initial state. 
Consider a cyclic process that returns to its initial state, undergoing a four-step process. The heat transfer along each...
2.9K
Uniform Depth Channel Flow01:27

Uniform Depth Channel Flow

131
Uniform depth channel flow keeps fluid depth consistent along channels such as irrigation canals. In natural channels, such as rivers, approximate uniform flow is often assumed. This condition occurs when the channel’s bottom slope matches the energy slope, balancing potential energy lost from gravity with head loss due to shear stress. This balance prevents depth changes along the channel length, resulting in a steady, uniform flow.Uniform flow in open channels with a constant cross-section...
131
Bus Impedance Matrix01:24

Bus Impedance Matrix

161
Calculating subtransient fault currents for three-phase faults in an N-bus power system involves using the positive-sequence network. When a three-phase short circuit occurs at a specific bus, the analysis uses the superposition method to evaluate two separate circuits.
In the first circuit, all machine voltage sources are short-circuited, leaving only the prefault voltage source at the fault location. The positive-sequence bus impedance matrix can be determined by solving the nodal equations,...
161
Uniform Depth Channel Flow: Problem Solving01:18

Uniform Depth Channel Flow: Problem Solving

121
To calculate the flow rate for a trapezoidal channel, first, identify the bottom width, side slope, and flow depth of the channel. The cross-sectional area (A) corresponding to the depth of flow (y), channel bottom width (B), and side slope (θ) is determined by:Next, calculate the wetted perimeter, which includes the bottom width and the sloped side lengths in contact with the water. Using the values of the cross-sectional area and the wetted perimeter, determine the hydraulic radius by...
121
Network Covalent Solids02:18

Network Covalent Solids

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Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
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Electrostatic Boundary Conditions01:16

Electrostatic Boundary Conditions

571
Consider an external electric field propagating through a homogeneous medium. When the electric field crosses the surface boundary of the medium, it undergoes a discontinuity. The electric field can be resolved into normal and tangential components. The amount by which the field changes at any boundary is given by the difference between the field components above and below the surface boundary.
The surface integral of an electric field is given by Gauss's law in integral form and is related to...
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Author Spotlight: Unveiling Mitochondrial Contact Sites and Architectural Insights
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孤立した弾道非アベルのインターフェースチャネル

Bivas Dutta1, Vladimir Umansky1, Mitali Banerjee2

  • 1Braun Center for Submicron Research, Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel.

Science (New York, N.Y.)
|September 8, 2022
PubMed
まとめ
この要約は機械生成です。

研究者は,量子ハール状態の非アベルの性質を ν = 5/2 で確認した. 断片的なエッジモードを分離することで,彼らは熱伝導性を測定し,粒子穴のPfaffian トポロジカル・オーダーを検証しました.

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High Resolution Physical Characterization of Single Metallic Nanoparticles
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科学分野:

  • 凝縮物質物理学
  • 量子ホール効果
  • トポロジカルな量子物質

背景:

  • 量子ホール状態は,バルクエッジ対応により,ギャップレスエッジモードでトポロジカル・オーダーを示す.
  • ν = 5/2 量子ハール状態は,さまざまなエッジモード (整数,分数,中性) を有する非アベルのアニオンを宿していることが予測されています.
  • 断片的なエッジチャネルを分離することは,熱平衡とv = 5/2状態の正確な特徴付けに不可欠です.

研究 の 目的:

  • 量子ハール状態のn = 5/2の非アベルの性質を実験的に検証する.
  • 断片的なエッジチャネルの熱伝導性を分離し測定する.
  • 粒子ホールのn = 5/2状態のパッファフィアントポロジック順序を確認する.

主な方法:

  • 整数エッジモードは,n = 5/2状態と整数量子ハール状態 (n = 2とn = 3) をインタフェースする.
  • 結果的に分離された断片的インターフェースチャネルの熱伝導度を測定した.
  • 実験結果の解釈に,バルクエッジ対応原理を用いた.

主要な成果:

  • ν = 5/2量子ハール状態の断片的なエッジチャネルを成功裏に分離した.
  • 隔離チャネルで 半量子導電性を測定した
  • 実験結果は,非アベルの統計と粒子の穴のPfaffian トポロジカル・オーダーを確認します.

結論:

  • 発見は,n = 5/2量子ハール状態の非アベルの性質の強力な証拠を提供します.
  • 孤立したチャネルは,非アベルのアニオンによる将来の編み物実験のための有望なプラットフォームを提供します.
  • この研究は,トポロジカルな量子物質の理解と潜在的応用を進める.