Name: linear shear between moving plates
Uploaded: 2025-02-13T15:43:26.000Z
Duration: 1 min 22 s
Channel: JoVE

Поток Куэтта описывает движение жидкости между двумя параллельными пластинами, где одна из них неподвижна, а другая движется с постоянной скоростью, создавая устойчивый ламинарный поток, приводимый в движение сдвигом.
Такая установка упрощает уравнения Навье-Стокса, которые могут быть выражены в безразмерной форме.
Безразмерный параметр, относящийся к градиенту давления, определяет изменения профилей потока Куэтта.
Когда градиент давления вдоль направления потока отсутствует, этот параметр становится нулем, указывая на линейное изменение скорости между двумя пластинами.
Профиль скорости жидкости между пластинами является линейным, увеличиваясь от нуля на неподвижной пластине до скорости движущейся пластины.
Метод Куэтта обычно используется для моделирования поведения жидкости в подшипниках с малой нагрузкой на скольжение, например, в водяных насосах, где тонкий слой смазки отделяет вращающийся вал в неподвижном корпусе.
В этих подшипниках с малой нагрузкой влияние давления минимально, поэтому характеристики текучести очень похожи на характеристики чистого потока по Куэтту.
Напряжение сдвига и скорость потока слоя смазки зависят от частоты вращения вала и ширины зазора между валом и корпусом.

Течение Куэтта

Couette Flow

Течение Куэтта представляет собой поток жидкости между двумя параллельными пластинами, одна из которых зафиксирована, а другая движется с постоянной скоростью. Такая конфигурация позволяет проводить упрощенный анализ с использованием уравнений Навье-Стокса, которые управляют движением жидкости в условиях вязкости и несжимаемости. Для течения Куэтта предположения включают устойчивый, ламинарный, несжимаемый поток с нулевым градиентом давления в направлении потока. Этот тип потока полезен для понимания потоков, вызванных сдвигом, и актуален для приложений в сценариях смазки и гражданского строительства, таких как перенос осадков и эрозия.

В установке с течением Куэтта ось x выровнена с направлением движения верхней пластины, а ось y перпендикулярна обеим пластинам. Течение устойчивое, ламинарное и полностью развившееся, без изменений.

Для течения Куэтта уравнение распределения скорости задается как:

<img alt="Equation 1" src="/files/ftp_upload/18064/18064_Equation_1.svg" style="text-align: center; height: 30px;" />

Где:

<ol style="list-style-type: circle;">
	<li>U — постоянная скорость верхней пластины,</li>
	<li>b — расстояние между пластинами,</li>
	<li>μ — динамическая вязкость жидкости.</li>
	<li>В безразмерной форме, разделив обе части на U, получаем:</li>
</ol>

<img alt="Equation 2" src="/files/ftp_upload/18064/18064_Equation_2.svg" style="text-align: center; height: 30px;" />

Где u/U представляет собой безразмерную скорость, а y/b — нормализованное расстояние от неподвижной пластины. Для анализа конкретных условий мы определяем безразмерный параметр P как:

<img alt="Equation 3" src="/files/ftp_upload/18064/18064_Equation_3.svg" style="text-align: center; height: 30px;" />

В этих условиях P становится равным нулю, когда нет градиента давления (∂p/∂x=0) в направлении x, что сводит уравнение скорости к следующему:

<img alt="Equation 4" src="/files/ftp_upload/18064/18064_Equation_4.svg" style="text-align: center; height: 26px;" />

Этот линейный профиль указывает на то, что скорость жидкости линейно увеличивается от нуля на неподвижной пластине до U на движущейся пластине, что приводит к равномерной скорости сдвига по всему слою жидкости.

Поток Куэтта описывает движение жидкости между двумя параллельными пластинами, где одна из них неподвижна, а другая движется с постоянной скоростью, создавая устойчивую, ...

Education

JoVE Core

Civil Engineering

Unit 1

Раздел 1

Differential Analysis of Fluid Flow

Дифференциальный анализ потока жидкости

KEY TERMS AND CONCEPTS

ОСНОВНЫЕ ТЕРМИНЫ И ПОНЯТИЯ

linear shear between moving plates

Linear shear between moving plates describes fluid motion in a simple channel with two parallel plates. One plate stays fixed, and the other moves at a constant speed. This setup helps show how viscosity and incompressible flow shape fluid motion under the Navier-Stokes equations.

The model uses a steady, laminar, incompressible flow with no pressure gradient in the flow direction. The x-axis points along the moving direction of the upper plate, and the y-axis is perpendicular to both plates. These assumptions make the flow fully developed and easier to analyze.

For this case, the velocity changes with distance from the stationary plate. The upper plate speed is U, the plate spacing is b, and the fluid’s dynamic viscosity is μ. In dimensionless form, the velocity is written as u/U, and the position is written as y/b.

A dimensionless parameter P is used to describe pressure effects. When there is no pressure gradient in the x-direction, P becomes zero because ∂p/∂x = 0. The velocity equation then reduces to a straight line, so the fluid speed rises from zero at the fixed plate to U at the moving plate.

This linear profile creates a uniform shear rate across the fluid layer. Shear-driven flow like this is useful for understanding lubrication and civil engineering problems. It also helps explain processes such as sediment transport and erosion.

Linear Shear Between Moving Plates

euler&#39;s equations of motion

Pressure and Velocity in Inviscid Flow

Pressure and velocity in inviscid flow are linked by Euler's equations of motion. In fluid mechanics, viscosity creates shear stress, which is a force that acts along a surface. For low-viscosity fluids like water, these shear stresses are very small. That lets the fluid be treated as inviscid, or frictionless. In an inviscid fluid, shear stresses are absent. Only normal stresses remain, and these act perpendicular to a fluid element. Pressure is the negative of the normal stress. It stays the...

stream function

Stream Function for Incompressible Flow

The stream function helps describe two-dimensional incompressible flow. In this type of flow, the continuity equation keeps mass conserved. That means fluid entering a region must be balanced by fluid leaving it. For incompressible flow, the density stays constant. The continuity requirement then becomes a zero-divergence condition for the velocity field. In two dimensions, the horizontal and vertical velocity components are usually written as u and v. A stream function, written as ψ, is used...

irrotational flow

Irrotational Flow Near Boundaries

Irrotational flow is fluid motion in which particles do not spin around their own axes. It has zero vorticity, which means the curl of the velocity field is zero. That condition places limits on the velocity gradients in the flow. A simple example is uniform flow. In this case, the velocity u stays constant, while v and w are both zero. This satisfies the irrotational conditions and gives a basic model of non-rotating flow. When a solid object is added, irrotational flow usually remains only...

velocity potential

Velocity Potential in Pipe Flow

Velocity potential in pipe flow describes the motion of fluid in the central region of a long, straight pipe with a uniform cross-section. In this region, the flow is steady, incompressible, and irrotational. Irrotational means the fluid particles do not spin around their own axes. A scalar function called the velocity potential, written as φ, is used to describe this motion. The velocity field V is defined as the gradient of φ. Because the curl of a gradient is always zero, this form of V...

plane potential flows

Plane Potential Flow Patterns and Models

Plane potential flows describe fluid motion using simple flow patterns and models. They assume the fluid is irrotational and incompressible. These assumptions let the flow be written with a velocity potential function, φ, which gives the flow speed in a direction, and a stream function, ψ, which shows the flow path. Both are governed by Laplace's equation and are useful for estimating flow patterns, velocity distributions, and pressure fields around hydraulic structures. Uniform flow is the...

navier&#8211;stokes equations

Fluid Stress and Flow Equations

Fluid stress and flow equations describe how incompressible Newtonian fluids move under pressure, shear, and gravity. In these fluids, density stays constant, and stress changes linearly with the rate of deformation. The main stress types are normal stress and shear stress. Normal stress depends on pressure acting on the fluid and on deformation rate in specific directions. Shear stress acts along the surface of a fluid layer. It shows how neighboring layers slide past one another, so velocity...

steady, laminar flow between parallel plates

steady-laminar-flow-between-parallel-plates

Laminar Flow Profile Between Parallel Plates

Laminar flow between parallel plates shows how fluid moves through a narrow, flat channel. This model helps describe flow in water conveyance and drainage systems, where the space is limited and the motion stays orderly. It is also useful for analyzing flow in rectangular channels used in many engineering settings. The flow is studied with the Navier-Stokes equations, which govern fluid motion. These equations are often difficult to solve because they are nonlinear. In this case, the problem...

couette flow

Linear shear between moving plates describes fluid motion in a simple channel with two parallel plates. One plate stays fixed, and the other moves at a constant speed. This setup helps show how viscosity and incompressible flow shape fluid motion under the Navier-Stokes equations. The model uses a steady, laminar, incompressible flow with no pressure gradient in the flow direction. The x-axis points along the moving direction of the upper plate, and the y-axis is perpendicular to both plates.

steady, laminar flow in circular tubes

Parabolic Flow in Circular Tubes

Parabolic flow in circular tubes describes the steady, incompressible motion of a viscous fluid through a tube with a constant radius. This Hagen-Poiseuille flow is a classic example of laminar flow. It is often used to study fluid transport in narrow channels, including capillaries. Cylindrical coordinates are used to describe the tube. The radial direction is r, the angular direction is θ, and the axial direction is z. In this flow, the velocity is purely axial. That means the fluid moves...

design example: flow of oil through circular pipes

design-example-flow-of-oil-through-circular-pipes

Pressure Drop in Oil Pipe Design

Pressure drop in oil pipe design depends on pipe size, oil properties, and the flow rate needed through a circular pipe. For steady, incompressible, laminar flow, Hagen-Poiseuille's law gives an exact solution from the Navier-Stokes equations. It is used to find the pressure difference needed to keep oil moving through a pipeline section. The pressure drop equation uses the oil's dynamic viscosity, the pipeline length, the desired volumetric flow rate, and the pipe's inner radius. This...

key terms and concepts

Learn how fluid moves between two parallel plates when one plate is fixed and the other moves. See the linear velocity profile, shear rate, and key assumptions.

Linear Shear Between Moving Plates | JoVE K12

JoVE Core Civil Engineering provides a foundational exploration of essential construction materials in civil engineering, focusing on bricks, stones, steel, wood, and concrete through easy-to-understand animated videos. This collection covers the properties, manufacturing processes, and practical applications of these materials. Additionally, the accompanied science-in-action videos demonstrate the research experiments performed in laboratories.

civil engineering

Linear Shear Between Moving Plates

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