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(1)

Fluid Mechanics

Hyungmin Park

Multiphase Flow and Flow Visualization Lab.

Fall 2022, undergraduate course

(2)

Course Introduction

q Fluid Mechanics 001 (M2794.001300, 001) q Prof. Hyungmin Park(박형민)

o Office: 301동 1405호 (Tel: 880-4159) o Email: [email protected]

o Office hour: with appointment

q Goals

o In this course,

• we study the basic theories and concepts of fluid dynamics and derive the governing equations to describe the relevant

phenomena

• to possess the capability of understanding and analyzing the fluid

mechanics phenomena occurring in the diverse industrial and

natural environments.

(3)

Course Introduction

q Textbook o Main

• Fluid Mechanics (F. M. White), McGraw-Hill Higher Education

• Lecture Notes (to be uploaded after each class)

• Supplementary materials – please check “eTL” frequently o References

• Viscous Fluid Flow (F. White)

• Boundary Layer Theory (H. Schlichting)

• ETC.

q Evaluation

o Attendance (10%), Homework (15%), Midterm1 (20%), Midterm2 (20%), Final (35%)

(4)

Course Introduction

q Scope (Schedule) – to be operated flexibly o Ch.1

• Concept of fluid, Continuum, Properties of fluid flow,

Dimensions and units, Basic flow analysis techniques, Flow patterns

o Ch.2

• Pressure and pressure gradient, Hydrostatic pressure o Ch.3

• Basic physical laws of fluid mechanics, Reynolds transport theorem, Control volume analysis

o Ch.4

• Equations for mass and linear momentum conservation -

continuity and Navier-Stokes equation

(5)

Course Introduction

q Scope (Schedule) – to be operated flexibly o Ch.5

• Principle of dimensional homogeneity, Non-dimensional parameters, Pi-theorem

o Ch.6

• Internal viscous flows, laminar vs. turbulent flows, skin-friction drag

o Boundary-layer theory

(6)

TA info

q

여지은([email protected]), 김대일([email protected])

q Lab. Location: 313동 222호 (Tel: 880-9161)

q TA Hour

o Flipped learning (online) – TA video will be uploaded in eTL biweekly o Q&A

o To solve example problems

o To derive theory/equation, not covered in the lecture

o Some stuffs covered in TA hour will be reflected in the exams.

(7)

Fluid Mechanics

q Fluids essential to life

o Human body 65% water

o Earth ’ s surface is 2/3 water

o Atmosphere extends 17 km above the earth ’ s surface

q History shaped by fluid mechanics o Geomorphology

o Human migration and civilization

o Modern scientific and mathematical theories and methods o Warfare

q Affects every part of our lives

(8)

History

Faces of Fluid Mechanics

Archimedes

(C. 287-212 BC) Newton

(1642-1727) Leibniz

(1646-1716) Euler

(1707-1783)

Navier

(1785-1836) Stokes

(1819-1903) Reynolds

(1842-1912) Prandtl

(1875-1953)

Bernoulli

(1667-1748)

Taylor

(1886-1975)

(9)

History

민태기 박사 강연 기계산업경영2

“경계를 뛰어넘은 과학자들”

9월 14일 16:00 301동 118호

(10)

Significance

q Fluids omnipresent o Weather & climate

o Vehicles: automobiles, trains, ships, and planes, etc.

o Environment o Energy

o Biology

o Semiconductor industry

o Physiology, medicine, and virus o Sports & recreation

o Many other examples!

(11)

Boundary-layer flow (경계층 유동)

(12)

Kelvin-Helmholtz instability (Karman vortex street)

(13)

Kelvin-Helmholtz instability (Karman vortex street)

(14)

Flow around a streamlined body

(15)

Diverse flows in industry…

(16)

Vehicles

(17)

Vehicles

(18)

Environment

(19)

Physiology and Medicine

Ventricular assist device

(20)

Physiology and Medicine

(21)

Flows in Nature

(22)

Sports & Recreation

(23)

Energy & Power conversion

(24)

. (

INTRODUCTION

.

1.1

Prime Mary Remote

Fluid mechanism

The

Stay

of

fluid

s

( gas

and

Aid )

other in Motion or

A rest

,

especiaaytemteractiueettetsbetw.eu

① fluid

S -

fluid

and

② fluid

S -

Solid

S .

↳ Approach es

:

Experiment

,

CFD_wmputatonalb.MY

Modeli .

Fluid D

names

)

( theory ng

)

1. 2.

History

and

Score of EM

.

-

Arch

.me des

( 자 5-212

Be

)

:

Law of by

an

g.

(25)

e

Leonardo da U

Mar

( 1472-1519 ) 1% 녜

:

equation of

mass

Conservation

in 1D

steadyftw.ms#dy:firstf6wuisua1izatm.(sKetch

es

for May Complex

How phe.name

na

)

'

Ed

Me

Mario # ( 1620-1684

)

:

First but

a

어마쨒 ( 풍동 )

and Test d.

-

Issac Newton ( 1642-1727 )

:

Law of Motion

(

Momentan

)

↳ Law of

멱쏄 ( Newton

ian

fluid )

(26)

'

Fiction loss fluid ( theory /

assum

para )

- 18C

Mathematics

ans,

Eden

d

Herbert

,

ange.e.T.devebpedbtdrfferatiala.de#usF(BemouUi 19T 9)

| cnn.piaiabgimmerse.in

africtionlessfluidepeweucesaze.ro

drgforce.unfaliste.ly route ( 수리학

.

수렴할 )

-

My

i

ng

on

te

Application

-

Experimental Oriental

.

(27)

:

Pitottlagen.Poiseu.ie

,

Day

, a . .

↓ produceddataonuanmsflows.ba

they rawformwithodrgardtotefundamentalpys.es

were used in

of flow

.

-

End f De

:

Experimental hydraul.is

+

theoreticdhydrodynamies.Foude.Rylegh.Reynolds.ci (

←iad 一↳ Reyn.ws Number

analysis

CC4.5)

Re

=

9- 나

M~inert_a.li

is

Wait

(28)

a Mean

while

, U isas

flow theory

is a

variable

,

Nai 와 ( 1785-1836 )

,

States

( 189-1903)

too-difficulttosolveforarbitrayf.ws

.

-

Ludwig Prand.tl

. (

1875-1953 )

( publishedthemostimportantpo.pe

((904)

error

write

on EM . "

In

da

y

-

layer theory

" .

Von

Karen

an,

G.

I.

(or, a . . .

-

Second Half of

20C

CFDemerges.tsophisticatedexp.tec.hn

i

que

S.
(29)

1.4

Gap

+

of

a

fluid

,

*

matter / fluid I

reaction

to

an

apple.dshear.la .li

d

(

or

t agent

at

) St

A Solid

Can res

ist

a

der stress by

Mu

du

i

ng

a

State de Formation ( defkc.tn )

13t

, a

fluid Can't !

Any Mean stress apple.la

to a

fluid NG

re

suit

in

Motion of that Head

.

(

and

he Hard

de

Arms

as well

)

( 媤

'

Atom

a,

nofw.i.si

(30)

o

A fluid at rest

is in a

State of

Zero

shears.CThyd.ro static stress condition )

.

T r I

斷 mokcales.it?mEsundergrauiy,formsafree I effect Between of Cohe site fora surface ,

? for

a

My to static

condition

( fluid at rest )

,

te pressure at

a

Point

B

의의

to in aa

"

이에

"

(31)

-79

Rhedogy

.

( 유벤함 )

:

( Study

li

qui

d,

of

in

General

He

How )

,

but of

matter

also

as

stream

flow

.

(

"

soft Plastic

Solid

flow

" . that

Matter response

than with

deformiy.V.slunymixture-asphalt.lead.ms

ist

Sean stress for Short

Time

,

event y dans

and

Show fluid behavior

Over

Long period

,

.

swexist.su Matt per phase critical flow fluid

. :

Two ( 초임계유체

on

More ? phase

(32)

p

a

Critical Point

.

Tiifi distinetanbetweenliq.andgasblurs.ITTTTpho.se digam gas

. --

Only V Single phase

a

its

.

( Super critical fluid )

.

1.5

.

The fluid

as a

mt 邀

fluidsiagregatrm.fm I .eu

.

( gas Y

. :: Warsen

denser.freeymoo.net

each

other

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Q ) How wedefnefluidpwprty.eqdenaity.oiswy.ca?

(33)

For exampe.g.li 怡批

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Most Engineering problem

s are on

and

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/ Physical del

means

Much layer

than

St

1

(34)

denaityisessentyap.int

at

and

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. 6

Di

Monsters and

Unit

-

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: a meansare

by

which a

Physical variable

e used

qua 꺠學

( length

, mass,

tre

,

)

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Unit ( 단위 )

:

aparticalanwayofalteh.rs

a .

number to

te

qaa 깨逃

1 dm 槌 ( metengram.am b)

(35)

'

International stem of Unit (

S

)

:

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M 1kg ]

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he Same

di

Men

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.

(36)

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.

Referensi

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