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。 |
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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:
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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。 |
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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
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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:
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:
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在层流条件下,管中心到距离r处的速度关系为: |
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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。
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