Bilingual edition: English is preserved and Chinese follows each unit. Terminology uses the confirmed v20260916 glossary; automated semantic review remains traceable.
中英双语版:英文原文完整保留,中文紧随对应单元;术语采用 v20260916 确认表,自动语义审校结果可追溯。

Kinetic Energy of Tube Flow

管流的动能
To get the kinetic energy of laminar flow in a tube, an average of the square of the velocity must be taken to account for the velocity profile.

The average of the square of the speed is given by

速度的平方的平均值由

The average kinetic energy per unit volume of the flowing fluid can be expressed in terms of the fluid density ρ and the maximum flow velocity vm.

流动流体的单位体积平均动能可以表示为流体密度ρ和最大流速v_m的函数。
要计算管内层流的动能,必须对速度分布进行平方的平均处理。
Index

Poisuille's law concepts
索引皮萨定律概念
 
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Velocity Relationship, Tube Flow

速度关系,管流

The nature of viscosity is such that successive lamina in the tube exert forces on each other according to the viscous force relationship:

粘性本质在于管内的各层依次对彼此施加力,根据粘性力关系:

When a pressure gradient dP/dx drives a section of lamina of length Δx at constant velocity, the force equation takes the form:

当压力梯度dP/dx驱动一段长度为Δx的层流,在恒定速度下,力方程的形式为:
For a short segment Δx of a given lamina, dA = 2πr dr and the forces take the form shown. This leads to an equation for the velocity in the tube.

Development of velocity equation
速度方程的发展
Equation solution
方程解
Illustration of velocity profile.
速度分布示意图
对于给定薄片的一个短段Δx,dA = 2πr dr,力的形式如图所示。这导致了管中速度的方程。
Index

Poisuille's law concepts
索引皮萨定律概念
 
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Velocity Equation, Tube Flow

速度方程,管流

Collecting terms gives the velocity equation in terms of radius r.

将项合并得到以半径 r 表示的速率方程
Discussion of velocity equation
速度方程的讨论
Equation solution
方程解
Illustration of velocity profile.
速度分布示意图
Index

Poisuille's law concepts
索引皮萨定律概念
 
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Velocity Profile for Tube Flow

管流速度分布
The relationship governing the velocity as a function of distance r from the center of a tube under conditions of laminar flow is:

Show
显示

Show details
显示详细信息

The general form of the solution to this differential equation is v = A + Br2 where A and B are constants which must be fit to the boundary condition of the flow: v=0 at r=R. Substituting the general solution by taking the derivatives gives:

该微分方程的通解形式为 v = A + Br²,其中 A 和 B 是常数,必须根据流动的边界条件进行拟合:在 r=R 处,v=0。将通解代入并求导后得到:
Discussion of velocity equation
速度方程的讨论
Development of equation
方程的发展
Illustration of velocity profile.
速度分布示意图
在层流条件下,管中心到距离r处的速度关系为:
Index

Poisuille's law concepts
索引皮萨定律概念
 
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Velocity Profile for Tube Flow

管流速度分布

Under conditions of laminar flow, the nature of viscosity dictates a flow profile where the velocity increases toward the center of the tube as illustrated.

在层流条件下,粘度的性质决定了流动剖面,其中速度向管子中心增加,如图所示。
Discussion of velocity equation
速度方程的讨论
Development of equation
方程的发展
Equation solution
方程解
Index

Poisuille's law concepts
索引皮萨定律概念
 
HyperPhysics***** Mechanics ***** Fluids
HyperPhysics ***** 力学 ***** 流体
R Nave
Go Back
返回