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相关概念视频

Equation of Motion: Center of Mass01:14

Equation of Motion: Center of Mass

202
The equation of motion for a single particle can be expanded to encompass a system of particles consisting of n particles. For any arbitrarily chosen particle within this system, the net force acting upon it is the aggregate of both internal and external forces. Extending this principle to all particles within the system results in the equation of motion for the entire assembly.
Internal forces between any pair of particles manifest as collinear pairs of equal magnitude but opposite directions,...
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Equilibrium Conditions for a Particle01:23

Equilibrium Conditions for a Particle

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When an object is in equilibrium, it is either at rest or moving with a constant velocity. There are two types of equilibrium: static and dynamic. Static equilibrium occurs when an object is at rest, while dynamic equilibrium occurs when an object is moving with a constant velocity. In both cases, there must be a balance of forces acting on the object.
To understand the concept of equilibrium, let us first consider the forces acting on an object. When different forces act on an object, they can...
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Kinematic Equations: Problem Solving01:15

Kinematic Equations: Problem Solving

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When analyzing one-dimensional motion with constant acceleration, the problem-solving strategy involves identifying the known quantities and choosing the appropriate kinematic equations to solve for the unknowns. Either one or two kinematic equations are needed to solve for the unknowns, depending on the known and unknown quantities. Generally, the number of equations required is the same as the number of unknown quantities in the given example. Two-body pursuit problems always require two...
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Euler Equations of Motion01:19

Euler Equations of Motion

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Imagine a rigid body that is rotating at an angular velocity of ω within an inertial frame of reference. Along with this, picture a second rotating frame that is attached to the body itself. This frame moves along with the body and possesses an angular velocity of Ω. The total moment about the center of mass is calculated by adding the rate of change of angular momentum about the center of mass in relation to the rotating frame and the cross-product of the body's angular velocity...
326
Rigid Body Equilibrium Problems - II01:21

Rigid Body Equilibrium Problems - II

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A rigid body is in static equilibrium when the net force and the net torque acting on the system are equal to zero.
Consider two children sitting on a seesaw, which has negligible mass. The first child has a mass (m1) of 26 kg and sits at point A, which is 1.6 meters (r1) from the pivot point B; the second child has a mass (m2) of 32 kg and sits at point C. How far from the pivot point B should the second child sit (r2) to balance the seesaw?
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Principle of Linear Impulse and Momentum for a System of Particles01:21

Principle of Linear Impulse and Momentum for a System of Particles

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In the context of a system of particles moving relative to an inertial frame of reference, the equation of motion is a crucial tool for understanding the dynamics of the system. This equation, which accounts for external forces acting on each particle, plays a fundamental role in describing the system's behavior.
Notably, internal forces between particles, occurring in equal and opposite collinear pairs, cancel out and are not part of the equation of motion. This exclusion simplifies the...
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相关实验视频

Updated: Sep 13, 2025

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
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全球变得本地化:全球主方程的高效多体动力学

Alexander Schnell1

  • 1Technische Universität Berlin, Institut für Physik und Astronomie, 10623 Berlin, Germany.

Physical review letters
|July 31, 2025
PubMed
概括

这项研究引入了一种新的方法来简化复杂的量子多体系统. 它通过使用局部主方程的新扩展来避免困难的计算,使量子模拟更容易获得.

科学领域:

  • 量子力学就是量子力学.
  • 凝聚物质物理学 凝聚物质物理学
  • 量子信息科学是一种量子信息科学.

背景情况:

  • 全球主方程,如Redfield主方程,需要计算密集的哈密尔顿对角化.
  • 这种对角化是研究相互作用的量子多体系统的一个重要障碍.
  • 现有的局部总方程方法在适用性方面存在局限性.

研究的目的:

  • 开发一种方法,绕过全球主方程中完全哈密尔顿对角化的需求.
  • 建立适用于更广泛的系统范围的本地总方程的非启发式基础.
  • 为量子多体系统模拟提供一种更易于计算的方法.

主要方法:

  • 在相互空间中采用了短浴相关时间扩张.
  • 这导致跳跃运算符的序列扩展,避免了哈密尔顿对角化.
  • 当地的Redfield主方程被映射到一个新的本地Lindblad形式.

主要成果:

  • 该方法允许将全球Redfield跳跃运营商扩展到本地合浴的本地运营商.
  • 产生了一个新的本地林德布拉德形式,扩大了本地主方程的适用性.
  • 为本地总方程建立了一个非启发式的基础.

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结论:

  • 开发的扩展为全球主方程的完全对角化提供了一个计算效率高的替代方案.
  • 新的局部林德布拉德形式为模拟更广泛的量子系统提供了强大的工具.
  • 这项工作为将先进的多体技术与强大的本地主方程相结合铺平了道路.