A short introduction to Fluid Dynamics , Heat Transfer and CFD

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A short introduction to Fluid Dynamics , Heat Transfer and CFD. Outline. Fluid Dynamics Heat Transfer CFD . Outline. Fluid Dynamics Heat Transfer CFD. Fluid Dynamics. - PowerPoint PPT Presentation

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A short introduction to

Fluid Dynamics,

Heat Transfer and CFD

www.mechcomp.se info@mechcomp.se

Outline

Fluid Dynamics Heat Transfer CFD

www.mechcomp.se info@mechcomp.se

Outline

Fluid Dynamics Heat Transfer CFD

www.mechcomp.se info@mechcomp.se

Fluid Dynamics

Study of fluids in motion, including aerodynamics, i.e. the study of gases (internal and external), and hydrodynamics, i.e. the study of liquids.

A fluid dynamical problem involves calculation of fluid properties, such as velocity, pressure, density and temperature A set of governing equations (conservation laws) are solved

using a numerical method (CFD)

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Fluid Dynamics -governing equations-

Based on conservation laws of mass, momentum and energy

Applied on a small fluid element; control volume (CV) Conservation of mass (continuity eqn):

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dSdVt SV

U CV

the rate of change of mass = net flow through the boundaries of the volume

(the control volume is fixed in space)

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Fluid Dynamics -governing equations-

Conservation of momentum (Navier-Stokes):

Substantial derivative: the rate of change of a property (F) for a CV moving with the fluid

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the rate of change of momentum = net force exerted on the volume

dAdvdvDtD

Aij

vv gU

CV

(the control volume moves with the fluid)

jj xFu

tFF

DtD )()()(

substantial or material derivative local or

Eulerian derivativeadvection

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Fluid Dynamics -governing equations-

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continuity equation

i

i

ii

i

j

ij

ii

xu

xxp

xuu

tu

DtDu

Re1

0

i

i

xu

t

Differential form (valid for arbitrary control volume)

momentum equations

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Fluid Dynamics -Reynolds number-

Most important dimensionless number in Fluid dynamics

For low Re-flows stabilizing viscous forces are dominant laminar flow

For high Re-flows inertia forces are dominant flow is unstable / turbulent

Re is used to determine scale similarity in experiments and simulations

forces viscousforces inertialRe

UL U: velocity scale

L: length scale

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Fluid Dynamics -boundary layer-

A thin layer of fluid, adjacent to the bounding surface, where viscosity is dominant

The treatment of the boundary layer is, due to the present physical processes, crucial Strong shear (wall friction) growth of instabilities, production of

turbulence Separation Heat/mass transfer Dissipation

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U=2m/s

U=10m/s

yU

y

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Fluid Dynamics -laminar flow-

Characterizes a flow in parallel layers In laminar flows

High momentum diffusion Low momentum convection U and P independent of time

The boundary layer in laminar flows is smooth

Smooth (weak) boundary layer low wall friction

Low energy level susceptible for adverse pressure gradients easy separation

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Fluid Dynamics -transitional flow-

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Transition from the laminar to the turbulent state

stable flow

unstableflow

turbulentflow

transit

ion

phase

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Fluid Dynamics -turbulent flow-

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Consists of a large number of vortices, i.e. eddies, of various size (scales) in space and time

Turbulent flows are of a random character

Extremely efficient in mixing processes

Nearly all practical flows are of a turbulent character

Turbulence is three-dimensional

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Fluid Dynamics -scales of motion-

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Turbulent flows are non-linear, i.e. there is transformation of information (energy) between different scales

Energy is supplied at the large scales, by the mean flow (production)

By, so-called, vortex stretching energy is transformed into smaller and smaller scales

Finally, at the viscous scales, energy is transformed into heat (dissipation)

Without production the turbulence decays

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Fluid Dynamics -vortex dynamics-

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Fluid Dynamics -statistical description-

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As turbulence is a non-repeatable random like process, statistical methods are needed to describe the flow

The flow is described by different statistical moments 1st-moment: mean

( ) 2nd-moment (about the mean): variance

( ) 3rd-moment (about the mean):

skewness ( ) 4th-moment (about the mean): kurtosis

( )

kk

k xx /

x2

3

4

n

i ixnx

1

12

std. deviation

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Fluid Dynamics -statistical description-

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0 500 1000 1500 2000 2500 30004

6

8

10

12

14

16

0 500 1000 1500 2000 2500 30004

6

8

10

12

14

16

75.1,10 x 75.1,10 x

63.2,03.0 43 5.1,0 43

Turbulent signal Sinus wave

Probe measurements would identify two identical flows w.r.t. mean and variance (and std. deviation)

Higher order statistics are needed

valu

e

sample sample

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Fluid Dynamics -statistical description-

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4 6 8 10 12 14 160

100

200

300

400

500

4 6 8 10 12 14 160

100

200

300

400

500

Histograms Turbulent signal Sinus wave

“heavy tails”

“high peakedness” symmetric

100

101

102

10310

-6

10-4

10-2

100

102

104

turbulent

sinus

Turbulent: energy concentrated to large scales Sinus: energy “solely” in the dominant frequency

power spectral density

value

sam

ples

value

frequency / wavenumber

psd

/ ene

rgy

Turbulent: distribution close to Gaussian Sinus: distribution heavy in the tails due to the intermittent

“flow character”

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Fluid Dynamics -terminology-

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Vorticity Potential flow Irrotational flow Stokes flow Wake flow Separation

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Fluid Dynamics-from a practical view-

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Outline

Fluid Dynamics Heat Transfer CFD

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Heat Transfer

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Heat Transfer -Prandtl number-

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Heat Transfer -convection heat transfer-

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Heat Transfer -diffusion heat transfer-

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Heat Transfer -radiation heat transfer-

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Heat Transfer -terminology-

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Heat Transfer -from a practical view-

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Outline

Fluid Dynamics Heat Transfer CFD

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CFD -solution strategies-

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CFD -basic criteria-

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CFD -finite difference approach-

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CFD-modeling techniques-

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CFD-terminology-

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CFD -from a practical view-

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