fluids and related notes

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Fluid Mechanics and Transport Phenomena: 1. Basic Definitions: 2. Navier-Stokes Equations: 3. Types of Flow: i. Planar Poiseuille Flow ii. Impulsively started single plate flow that is semi-infinite 4. dd Basic Definitons: Incompressible: Density, , is constant. Homogeneous: Density, , is the same for all fluid elements considered. Navier-Stokes Equations:  Continuity:   Momentum:  o  : Temporal and inertial/acceleration term. Equals 0 if steady.  o  : Temporal changes.  o : Inertial/acceleration term o : Pressure term (can sometimes account for gravity, o  : Viscous effects. (If inviscid this term is zero. Basis for Newton's Equation) o : Body forces (external body forces - can include gravity)  Where the material derivative is   Stress Tensor:   Rate of Strain Tensor, :  Types of Flow: Planar Poiseuille Flow:  Steady  Infinite channel  Assume unidirectional flow  Initial Conditions: o No Slip:  o Symmetric: Centre flow has no shear,  where          is the direction of flow  Notes:  In reality typically unstable for sufficiently high Re.  Introduction of perturbance (knocks, wall imperfections), the perturbance grows resulting in unsteady multidirectional flow.  Navier-Stokes solutions are not unique. Example: Planar Poiseuille Flow where x is the direction of flow and y is the height of the pipe  Steps:

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Page 1: Fluids and Related Notes

8/11/2019 Fluids and Related Notes

http://slidepdf.com/reader/full/fluids-and-related-notes 1/3

Fluid Mechanics and Transport Phenomena:

1. 

Basic Definitions:

2. 

Navier-Stokes Equations:

3. 

Types of Flow:

i. 

Planar Poiseuille Flowii.

 

Impulsively started single plate

flow that is semi-infinite

4. 

dd

Basic Definitons:

Incompressible: Density, , is constant.

Homogeneous: Density, , is the same for all

fluid elements considered.

Navier-Stokes Equations:

  Continuity:

 

  Momentum:

 

: Temporal and inertial/acceleration

term. Equals 0 if steady.  

: Temporal changes. 

: Inertial/acceleration term 

o  : Pressure term (can sometimes

account for gravity,

o  : Viscous effects. (If inviscid this term

is zero. Basis for Newton's Equation) 

o  : Body forces (external body forces - can

include gravity) 

Where the material derivative is

 

  Stress Tensor:

 

  Rate of Strain Tensor, :

 

 

Types of Flow:

Planar Poiseuille Flow:

  Steady

 

Infinite channel  Assume unidirectional flow

  Initial Conditions:

No Slip:

 

Symmetric: Centre flow has no

shear,  where        is the

direction of flow

 

Notes:

  In reality typically unstable for

sufficiently high Re.

  Introduction of perturbance (knocks,

wall imperfections), the perturbance

grows resulting in unsteady

multidirectional flow.

 

Navier-Stokes solutions are not unique.

Example: Planar Poiseuille Flow where x is the

direction of flow and y is the height of the pipe

 

Steps:

Page 2: Fluids and Related Notes

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1. 

Continuity

2. 

Navier-Stokes Equation applying

assumptions

3. 

Get expression for u. If considering

viscous terms, this will be a second

order pde and hence two b/c or i/c will

be required.

4. 

Express for maximum velocity

5. 

Determine average velocity

6. 

Determine mass flux

Continuity:

 

Momentum:

 

 

Assumptions:

  Steady:   

  Continuity:

 

 

  Unidirectional:   

  No body forces cf gravity:  

Hence the Navier-Stokes equation reduces to:

 

 

Unidirectional:

 

Assume 2D problem:

 

Hence take the second integral of

.

To solve, use boundary/initial conditions:

(symmetry  and no slip)

 

 

 

   

Determining constants of integration:

 

 

 

 

 

 

*Note: CHE3167 would express this as

, where

 is half the pipe height

and  is the length of pipe being considered for

which there is a .

Mass Flux:

 

Page 3: Fluids and Related Notes

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Impulsively Started Single Plate for a Semi-

Infinite Fluid:

  Plate moves with speed

 at

 

  Initially,  

  Pressure: Far from the plate,

 and so it must be

constant everywhere

  Assume unidirectional flow

 

  Initial Conditions:

No Slip: Fluid moves at the

same speed as plate (it 'sticks'to it)

 

Far Away Fluid:

 

Example:

Look for a similarity solution such that

       

Assumptions:

  No slip:  

  Far fluid:  

  Constant pressure: (p far away is

constant so it must be constant

everywhere)

  Unidirectional flow

 

No body forces

 

Continuity:

 

No other components to consider as it is

unidirectional

Momentum:

 

 

 

Similarity Solution/Self-Similar Solution: Results

when a space and time variable are tied

together such that      . Solution is of form