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相关概念视频

Moment of Inertia about an Arbitrary Axis01:20

Moment of Inertia about an Arbitrary Axis

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The moment of inertia is typically associated with principal axes, but it can also be computed for any random axis. When an arbitrary axis is under consideration, the moment of inertia is determined by integrating the mass distribution of the object along that specific axis. It is crucial in applications like the design of machinery, where components rotate about various axes, and balance and stability are essential.
In this scenario, the perpendicular distance between the chosen arbitrary axis...
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Angular Momentum about an Arbitrary Axis01:11

Angular Momentum about an Arbitrary Axis

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Imagine a rigid body with a mass denoted as 'm', which has its center of mass at point G and is rotating around an inertial reference frame. The angular momentum at an arbitrary point P can be calculated by taking the cross product of the position vector and linear momentum vector for each individual mass element.
The velocity of a mass element comprises its translational velocity and the relative velocity instigated by the body's rotation. Substituting the velocity equation into...
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Directing Effect of Substituents: meta-Directing Groups01:09

Directing Effect of Substituents: meta-Directing Groups

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Substituents on the benzene ring that direct an incoming electrophile to undergo substitution at the meta position are called meta directors. All meta directors either have a positive charge on the atom directly bonded to the ring or a partial positive charge. These groups function by withdrawing electrons from the ring through inductive and resonance effects. Consider the carbocation intermediates formed upon the addition of an electrophile on nitrobenzene at the...
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Thermal expansion and Thermal stress: Problem Solving01:27

Thermal expansion and Thermal stress: Problem Solving

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San Francisco's Golden Gate Bridge is exposed to temperatures ranging from -15 °C to 40 °C. At its coldest, the main span of the bridge is 1275 m long. Assuming that the bridge is made entirely of steel, what is the change in its length between these temperatures?
To solve the problem, first, identify the known and unknown quantities. The initial length (L) of the bridge is 1275 m, the coefficient of linear expansion (α) for steel is 12 x 10-6/°C, and the change in temperature (ΔT) is 55...
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Thermal Strain01:19

Thermal Strain

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Thermal strain is a concept that arises when we consider how temperature changes affect structures. Unlike the conventional assumption that structures remain constant under load, real-world scenarios often involve temperature fluctuations that can significantly impact these structures. Consider a homogeneous rod with a uniform cross-section resting freely on a flat horizontal surface. If the rod's temperature increases, the rod elongates. This elongation is proportional to the temperature...
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Thermal Expansion01:22

Thermal Expansion

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The expansion of alcohol in a thermometer is one of many commonly encountered examples of thermal expansion, which is the change in size or volume of a given system as its temperature changes. The most visible example is the expansion of hot air. When air is heated, it expands and becomes less dense than the surrounding air, which then exerts an upward force on the hot air to, for example, make steam and smoke rise, and hot air balloons float. The same behavior happens in all liquids and gases,...
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相关实验视频

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Scale-up Chemical Synthesis of Thermally-activated Delayed Fluorescence Emitters Based on the Dibenzothiophene-S,S-Dioxide Core
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超连贯的元发射器适应任意的热波前线.

Rui Chen1,2, Tianle Chen1, Mengqi Liu3

  • 1State Key Lab of Modern Optical Instrumentation, Centre for Optical and Electromagnetic Research, International Research Center for Advanced Photonics, College of Optical Science and Engineering, Zhejiang University, Hangzhou, Zhejiang, China.

Nature communications
|January 31, 2026
PubMed
概括

研究人员开发了一种新的元发射器,用于精确控制热辐射波面. 这一突破使热聚焦和全息等高级功能成为可能,将热力学与光子工程集成为新技术.

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科学领域:

  • 光子学和纳米技术的使用.
  • 热力学和热工程热力学.

背景情况:

  • 传统的光操纵与不连贯的热源作斗争.
  • 现有的热光子技术提供了定向发射,但缺乏任意的波浪控制.
  • 控制热波前线对于像聚焦和全息等先进应用至关重要.

研究的目的:

  • 开发一种设计元发射器的通用方法,使得任意的热波前线控制.
  • 为了克服连贯的光场技术和不连贯的热辐射之间的内在冲突.
  • 通过定制的热发射来实现热聚焦和全息等功能.

主要方法:

  • 设计具有合损耗和无损耗外界的元发射器.
  • 使用单模波导将表面合并将不连贯的热光子转换为连贯的表面波.
  • 通过设计面模式独立优化光子寿命和传播长度,用于空间连贯性工程.

主要成果:

  • 实验证明了近衍射有限的自我聚焦热辐射.
  • 创建一个准2D高质量的热全息,没有斑点噪声.
  • 实现了空间复合全息,并建议空间连贯性超过1000λ0.0.的潜力.

结论:

  • 拟议的元发射器设计为将热力学发射与光子工程相结合提供了一个范式转变.
  • 这项工作为开发信息丰富的热辐射技术开辟了新的途径.
  • 设计热波前线的能力为热源的先进光学功能铺平了道路.