格子博尔茨曼方法用于多项时间分数混合扩散和扩散波方程.
Jia Tong1, Fangfang Wu1, Xiaoxiao Dong1
1Shenyang University of Technology, College of Science, Shenyang 110870, People's Republic of China.
Physical review. E
|November 18, 2025
概括
一个新的格子博尔兹曼模型有效地解决复杂的多项时间分数方程. 这种计算流体动力学方法与分析解决方案有很好的一致性,验证了它对扩散和波浪现象的效率.
科学领域:
- 计算物理学的计算物理.
- 应用数学 应用数学 应用数学
- 数字分析 数字分析
背景情况:
- 分数微分方程 (FDE) 模型复杂的现象.
- 多项时间分数方程带来了重要的计算挑战.
- 现有的方法可能缺乏效率或普遍性.
研究的目的:
- 开发一个统一的格子博尔茨曼模型,用于多术语的时间分数混合扩散和扩散波方程.
- 通过数值模拟来验证模型的准确性和效率.
- 为微积分微积分应用提供一个强大的计算工具.
主要方法:
- 使用数值分化和复合集成规则对卡普托衍生项的近似计算.
- 选择特定的辅助和平衡分布函数.
- 实现用于解决FDE的格子博尔兹曼方法.
主要成果:
- 提出的格子博尔兹曼模型成功地恢复了宏观方程.
- 数字模拟表明模型的结果与分析解决方案之间有很好的一致.
- 统一模型的效率和准确性得到了验证.
结论:
- 开发的格子博尔茨曼模型提供了一种高效和准确的方法来解决多术语时间分数混合扩散和扩散波方程.
- 这种方法为涉及分数微积分的问题提供了可靠的计算框架.
- 这项研究证实了格子博尔茨曼方法在复杂的科学领域的广泛适用性.
相关概念视频
Carrier Transport
889
The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
889
Bewley Lattice Diagram
1.4K
The Bewley lattice diagram, developed by L. V. Bewley, effectively organizes the reflections occurring during transmission-line transients. It visually represents how voltage waves propagate and reflect within a transmission line, making it easier to understand the complex interactions that occur.
1.4K
Maxwell-Boltzmann Distribution: Problem Solving
2.8K
Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
2.8K
Transmission-Line Differential Equations
942
Transmission lines are essential components of electrical power systems. They are characterized by the distributed nature of resistance (R), inductance (L), and capacitance (C) per unit length. To analyze these lines, differential equations are employed to model the variations in voltage and current along the line.
Line Section Model
A circuit representing a line section of length Δx helps in understanding the transmission line parameters. The voltage V(x) and current i(x) are measured from...
Line Section Model
A circuit representing a line section of length Δx helps in understanding the transmission line parameters. The voltage V(x) and current i(x) are measured from...
942
The de Broglie Wavelength
32.9K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
32.9K
Poisson's And Laplace's Equation
4.1K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
4.1K


