04 Kinematics of Local Fluid Motion

04 Kinematics of Local Fluid Motion - EGM 6812 Fluid...

Info iconThis preview shows pages 1–4. Sign up to view the full content.

View Full Document Right Arrow Icon
EGM 6812 Fluid Mechanics 1 - Fall 2004 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 x t Define: i r as the position of a material point as it travels through space ( 29 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 r t $ 3.1.2 Eulerian Viewpoint Control region or field
Background image of page 1

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon
EGM 6812 Fluid Mechanics 1 - Fall 2004 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: ( 29 , dx V x t dt = r r r , integrate w.r.t. time, then determine constants by specifying a location at a given time, i.e., particle passes through 0 x r at 0 t . Streaklines It is a locus of particles that have passed through a given point To find the streakline: ( 29 , dx V x t dt = r r r , 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 d x r V r 0 example: 1 dx dy dz V d x u v w x V i j t = = = = + + r r r To find the equation for the streamline: ( 29 ( 29 0 0 0 1 0 1 1 ln or y y t dy v t dx u x y y t x x x x e - + + = = - = + = Timelines a set of particles (Lagranian) that form a line at a given instant in time.
Background image of page 2
EGM 6812 Fluid Mechanics 1 - Fall 2004 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” ( 29 0 ˆ , L i F F x t = “Eulerian” ( 29 , E i F F x t = where ( 29 0 ˆ , i i i x r x t = Transformation “Law” between Lagrangian, Eulerian methods of descriptions ( 29 ( 29 ( 29 ( 29 ( 29 0 0 0 ˆ ˆ , ˆ ˆ ˆ , , , ˆ ˆ ˆ i i i L i E i i i L E i E E E i i i E E t t r x t x F F x t F x r x t t t F F dx F dt F F v t x dt t dt t x F V F t = = = = = = = + = + = + r Stokes gave this special notation ( 29 ( 29 ( 29 ( 29 ( 29 ( 29 ( 29 Index: Gibbs: i i D u Dt t x D V Dt t = + = + For acceleration F V = ( 29 Index: Gibbs: j j j i i Du u u u Dt t x DV V V V Dt t = + = +
Background image of page 3

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon
Image of page 4
This is the end of the preview. Sign up to access the rest of the document.

This note was uploaded on 01/17/2012 for the course EGM 6812 taught by Professor Renweimei during the Fall '09 term at University of Florida.

Page1 / 14

04 Kinematics of Local Fluid Motion - EGM 6812 Fluid...

This preview shows document pages 1 - 4. Sign up to view the full document.

View Full Document Right Arrow Icon
Ask a homework question - tutors are online