03%20Kinematics%20of%20Local%20Fluid%20Motion%20EMG%206812%20F11

# 03%20Kinematics%20of%20Local%20Fluid%20Motion%20EMG%206812%20F11

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EGM 6812, F11, University of Florida, M. Sheplak 1/14 Section 3, Kinematics 3 Kinematics of Local Fluid Motion Kinematics is a branch of mechanics that treats motion without reference to forces causing that motion. 3.1 Lagrangian and Eulerian Methods of Description 3.1.1 Lagrangian Viewpoint General form of conservation law (system, “convected,” material region) Attention is focused on material particles as they move through the flow. It is natural extension of particle mechanics. Each particle in the flow is formally labeled and identified by Original position 0 i x Time t There are 2 independent variables in the Lagrangian method: 0 ˆ , i xt Define: i r as the position of a material point as it travels through space   0 , i i i r r x t  Velocity: i r t Acceleration: 2 2 i r t 2 r 1 r 0 i x @ i rt

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EGM 6812, F11, University of Florida, M. Sheplak 2/14 Section 3, Kinematics 3.1.2 Eulerian Viewpoint Control region or field Focuses on the properties of the flow at a given point in the flow (move convenient for fluid flow) All flow properties such as , ,etc. i i i r v a are functions of the following independent variables in the Eulerian method of description Space: i x Time: t 3.2 Streamlines, Streaklines, Pathlines, and Timelines Line Patterns to Visualize Flow (*all equal for steady flow except timeline*) Pathlines consider one particle (Lagranian) and the path that it traces out in time. To find the pathline:   , dx V x t dt , integrate w.r.t. time, then determine constants by specifying a location at a given time, i.e., particle passes through 0 x at 0 t . Streaklines It is a locus of particles that have passed through a given point To find the streakline:   , dx V x t dt , integrate w.r.t. time, then determine constants by specifying an initial condition. Streamlines a line that is everywhere tangent to the velocity vector at any instant in time dx V 0 example: 1 dx dy dz V d x u v w x V i j t  To find the equation for the streamline:     0 00 1 0 1 1 ln or yy t dy v t dx u x y y t x x x x e    
EGM 6812, F11, University of Florida, M. Sheplak 3/14 Section 3, Kinematics Timelines a set of particles (Lagranian) that form a line at a given instant in time. 3.3 Substantial Derivative (“material derivative”) Express the time rate of change of a particle property or material property in Eulerian variable. Let F be property of the flow under consideration “Lagrangian”   0 ˆ , Li F F x t “Eulerian”   , Ei F F x t where   0 ˆ , i i i x r x t Transformation “Law” between Lagrangian, Eulerian methods of descriptions (really just the chain rule)           0 00 ˆ ˆ , ˆ ˆ ˆ , , , ˆ ˆ ˆ i i i L i E i i i L E i E E E i ii E E tt r x t x F F x t F x r x t t t F F dx F dt F F u t x dt t dt t x F VF t 

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03%20Kinematics%20of%20Local%20Fluid%20Motion%20EMG%206812%20F11

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