围绕联合形态化的前端和后端翼翼的短暂流动的数值模拟
Musavir Bashir1, Mir Hossein Negahban1, Ruxandra Mihaela Botez1
1Research Laboratory in Active Controls, Avionics and Aeroservoelasticity (LARCASE), Department of Systems Engineering, École de Technologie Supérieure, 1100 Notre-Dame West, Montreal, QC H3C1K3, Canada.
Biomimetics (Basel, Switzerland)
|February 23, 2024
概括
本研究介绍了用于主动流量控制的联合形态领尖和尾尖 (CoMpLETE) 技术. 仿生灵感设计有效地减轻了流量分离,并通过动态调整气翼形状来增强起重.
科学领域:
- 流体动力学 流体动力学
- 空气动力学 航空动力学
- 生物电子学 生物电子学
背景情况:
- 积极的流量控制对于管理空气动力学性能至关重要,特别是防止流量分离.
- 现有的方法往往侧重于单个控制面,限制了协同作用的潜力.
- 生物灵感为动态流量管理提供了新的策略.
研究的目的:
- 提出和评估用于主动流量控制的联合形态化领尖和尾尖 (CoMpLETE) 技术.
- 为了研究 morphing 领先和尾随边缘在流量分离控制上的协同效应.
- 为了分析动态变形的气形状的空气动力学性能,灵感来自于海豚和鱼的运动.
主要方法:
- 开发一个参数化模型,用于一个变形的气形翼,具有可变的曲率.
- 使用过渡式SST (切割应力传输) 模型来模拟流体现象.
- 对空气动力学力,速度流线和旋流轮的实验性评估.
- 调查各种变形参数:位置,振幅,开始时间和频率.
主要成果:
- CoMpLETE技术有效地减少了不利的压力梯度,防止了大量的流量分离.
- 空气凸的动态调整会导致流量重新连接,并增加最大提升系数 (cl,max).
- 与单个控制器相比,前端和后端的协同变形显示出在减轻流量分离方面具有重大潜力.
结论:
- CoMpLETE技术为主动流量控制提供了一个有前途的综合方法.
- 气翼边缘的动态变形显著提高了空气动力学性能,特别是升力.
- 仿生灵感设计为复杂的流量管理挑战提供了有效的解决方案.
相关概念视频
Bernoulli's Equation for Flow Along a Streamline
969
Bernoulli's equation relates the energy conservation in a fluid moving along a streamline. The equation applies to incompressible and inviscid fluids under steady flow. For such a flow, Newton's second law is applied to a small fluid element, which experiences forces due to pressure differences, gravity, and velocity variations. The force balance leads to the following form of Bernoulli's equation:
969
Bernoulli's Equation for Flow Normal to a Streamline
861
Bernoulli's equation for flow normal to a streamline explains how pressure varies across curved streamlines due to the outward centrifugal forces induced by the fluid's curvature. The pressure is higher on the inner side of the curve, near the center of curvature, and decreases outward to balance these centrifugal forces.
The pressure difference depends on the fluid's velocity and radius of curvature. The pressure variation is minimal in flows with nearly straight streamlines.
The pressure difference depends on the fluid's velocity and radius of curvature. The pressure variation is minimal in flows with nearly straight streamlines.
861
Laminar and Turbulent Flow
8.5K
Fluid dynamics is the study of fluids in motion. Velocity vectors are often used to illustrate fluid motion in applications like meteorology. For example, wind—the fluid motion of air in the atmosphere—can be represented by vectors indicating the speed and direction of the wind at any given point on a map. Another method for representing fluid motion is a streamline. A streamline represents the path of a small volume of fluid as it flows. When the flow pattern changes with time, the...
8.5K
Steady, Laminar Flow in Circular Tubes
208
Hagen-Poiseuille flow describes a viscous fluid's steady, incompressible flow through a cylindrical tube with a constant radius R. This flow profile is often applied to understand fluid transport in narrow channels, such as capillaries. It serves as a foundational example of laminar flow. In this model, cylindrical coordinates (r,θ,z) are used to describe the radial (r), angular (θ), and axial (z) dimensions within the tube. For Hagen-Poiseuille flow, the velocity profile is...
208
Steady, Laminar Flow Between Parallel Plates
192
Understanding steady, laminar flow between parallel plates is essential for analyzing and designing flow in narrow rectangular channels, commonly found in various water conveyance and drainage systems. The Navier-Stokes equations govern fluid motion and are generally challenging to solve due to their nonlinearity. However, simplifications are possible in certain cases, like the steady laminar flow between parallel plates. For this scenario, we assume steady, incompressible, laminar flow.
192
Turbulent Flow
190
Turbulent flow is characterized by unpredictable fluctuations in velocity and pressure, which result in a chaotic fluid movement distinct from the orderly patterns of laminar flow. While laminar flow is governed by smooth, parallel layers with minimal mixing, turbulent flow exhibits highly irregular, three-dimensional patterns. This behavior arises due to instabilities in the fluid's velocity profile, and amplifies as the flow velocity increases. Minor disturbances, known as turbulent...
190


