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An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez-Miravete Department of Engineering and Science Rensselaer at Hartford Presented at the COMSOL Conference 2008 Boston

An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

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Page 1: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

An Analysis of Hiemenz Flow

E. Kaufman and E. Gutierrez-MiraveteDepartment of Engineering and Science

Rensselaer at Hartford

Presented at the COMSOL Conference 2008 Boston

Page 2: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

OBJECTIVE

To solve a simple flow field for which an exact solution is available using COMSOL & FLUENT

HIEMENZ FLOW• Planar • Laminar • Viscous • Incompressible• Close to a stagnation point x

y

x

y

Page 3: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

BACKGROUND

• Exact Solution Exists for Hiemenz Flow• Viscous Solution is Derived from the Inviscid Solution

Viscous

jxayfixafV ˆ)('ˆ)( +−=

( )[ ]yFxapp +=− 2221

0 ρ

jayiaxV ˆˆ +−= Inviscid

( )22221

0 yxapp +=− ρ

Page 4: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

HIEMENZ SOLUTION

• Substitute into 2D Incompressible Navier-Stokes Equations

•Similarity Solution Yields Hiemenz Equation

•Boundary Conditions

•Solve Using Shooting Method

01'''''' 2 =+−+ φφφφ

( ) ''''''22 axfxpgfffxa x µρρ +∂∂

−=− '''2 afypgffa y µρρ −∂∂

−=

0)0(')0( ==φφ

1)(' =∞φ

Page 5: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

Velocity Profiles

Wall

Flow Direction

Inviscid and Viscous Hiemenz Flow: Velocity

Symmetry Line

Page 6: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

Inviscid and Viscous Hiemenz Flow: Pressure

Pressure Contours

Wall

Flow Direction

Page 7: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

•Inviscid heat flux at the wall is ~ 2X Viscous

Inviscid and Viscous Hiemenz Flow: Temperature

Page 8: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

Exit Pressure

0

1

2

3

4

5

6

60 70 80 90

Pa

m

COMSOL & FLUENT: Case Study - Inputs

• Compare Analytical Solution to Computational Results

• Density = 1 kg/m3

• Viscosity = 1 kg/ms• Conductivity = 1 W/moC

Material Properties

Similarity Factors• η = y/1•ϕ = f/1

• Set up Dimensional Problem for Easy Comparison

Flow Field Scale Factor• a = 1 s-1

Computational Domain• 6 meters by 6 meters

Inlet Velocity:(u, v) = (x, 5.3521)Inlet Temperature: T=100Inlet

Exit

Wall: T=1000

Symmetry

(0,0)

(0,6)

(6,0)

(6,6)

Boundary Conditions• Consistent with analytical solution at boundaries• Assume stagnation pressure of 100 Pascals

Page 9: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

COMSOL Mesh

FLUENT Mesh

COMSOL Velocity

FLUENT Velocity

COMSOL Pressure Field

FLUENT Pressure Field

COMSOL & FLUENT: Case Study - Results

Page 10: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

Pressure Profile at Symmetry Plane (X=0)

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

98 99 100 101 102

Pressure (Pa)

Y co

ordi

nate

(m)

COMSOL FLUENT

Hiemenz Inviscid

Pressure Profile at Symmetry Plane (X=0)

0

1

2

3

4

5

6

80 85 90 95 100 105

Pressure (Pa)

Y co

ordi

nate

(m)

COMSOL FLUENT Hiemenz Inviscid

Wall

Inlet

Flow Direction

COMSOL & FLUENT: Case Study – ResultsStatic Pressure Along Symmetry Plane

Page 11: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

Temperature Profile

0

1

2

3

4

5

6

0 0.2 0.4 0.6 0.8 1

Normalized Temp (T-Twall)/(Tinf-Twall)

Y co

ordi

nate

(m)

COMSOL FLUENT Hiemenz Inviscid

COMSOL Temperature Distribution

FLUENT Temperature Distribution

COMSOL & FLUENT: Case Study – ResultsTemperature

Page 12: An Analysis of Hiemenz Flow - COMSOL Multiphysics · An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez -Miravete Department of Engineering and Science Rensselaer at Hartford

CONCLUSIONS

• Both COMSOL and FLUENT have been shown to reliably reproduce the flow field

• Velocities, Pressures and Temperatures match the analytical predictions closely

•Selection of appropriate boundary conditions and adequate domain size are critical to accurately predict flow field