+ All Categories
Home > Documents > -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9...

-494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9...

Date post: 19-May-2020
Category:
Upload: others
View: 6 times
Download: 0 times
Share this document with a friend
37
!"#$%&%' #() *"+,$(-".' /)0$1".' !"#-494 $%. &'(μ)*+ (,-.)*+) /+0+1)2(, 3"! !"#$%&'( )*+,-.% 30 23-"45+6 2015
Transcript
Page 1: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!"#$%&%' #() *"+,$(-".' /)0$1".' !"#-494

$%. &'(µ)*+ (,-.)*+) /+0+1)2(, 3"!

!"#$%&'( )*+,-.% 30 23-"45+6 2015

Page 2: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!"#$%&'(' – )* +,#&-./0µ1 µ,# µ-2/+/

31,4#µ#5,67 81095/+0$#µ,67

:1;4'5,67/)$#&05,67 81095/+0$#µ,67

<"/&/=,95,67 81095/+0$#µ,67

!7"#8#9": Navier-Stokes %"$ ;96(819"+ -96#(< .$" $#6µ359#() -+'

Page 3: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!"#$%&µ" '% $"()'* #+ )(,"-.+ µ.)% /01 µ"'0-"1$12*µ0)'" '1+ 131*'4'"+ '4+ &54+ #+ )(,"-"6+ )(,0$'7)"1+ '%( -8$%(. =)4. >9&-+?µ9 <(" +" "@"<()(9: (+6 -96#(+? <3&: ) 36.1<()($ $, ) ($0?()($ u, ) 359#) p .$" ) >9-µ+.-$#5$ T 951$" #619095: #9 +3+"+@'3+(9 <%.+ -96#(+? dV, <#+ µ".-<: ." $1 951$", .$" $%1++?µ9 (+ %9%+1<: <(" (+ -96#(< $3+(9495($" $3< @"$.-"(A µ<-"$.

!! /012*," 3+%*#456 !7,4+

!"#$%&'(' – )* 6%$/0µ1 µ,# 0">219'

(a) Surface of sphere surroundingobservation point

observation point

(b)

Page 4: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!"#$%&'(' – )+,%95#5' #$%&09'

B" 3+#<()(9: 3+6 µ949(Aµ9 0$-$.()-5C+1($" $3< 4 D$#".E: @"$#(A#9"::

F449: @"$#(A#9": µ3+-+?1 1$ #0)µ$("#>+?1 µ9 DA#) (": 3-&($-0".E::

G$0?()($ u: /+1A@9: SI m/s .$" @"$#(A#9": LG-1

H%.+: V: /+1A@9: SI m3 .$" @"$#(A#9": L3

=?1$µ) F: F=m*a, µ+1A@9: SI kg*m/s2 .$" @"$#(A#9": /LG-2

I78@9: µ: µ+1A@9: SI .$" @"$#(A#9": /L-1G-1 µ =FhAV

µ =kgm ! s

J"1)µ$(".< "78@9: ,: ! =µ"

L2

T="$#(A#9":; /+1A@9: SI; ! =m

2

s

!89$ !

!('46 L

:;1%46 <

=*;µ4- ';$,>$ =

Page 5: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!"#$%&'(' – ?"5,6/"/@'9' "1+@/0 4/7*

Page 6: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

/E>+@+" µ94E():, 39-"%-$K':

2-">µ<: Reynolds

L($(".' -96#(81, M9µ94"8@9": 1<µ+"

!7"#8#9": .51)#):, Navier-Stokes

!75#&#) Bernoulli

!"#$%&'( )*+,-.%

A5>B/, µ#27µ#5/*

Page 7: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

C4>"/, µ1&-5'* "1+@;$ 4/7*

?@4'@"- ;A-&'(

21A46#) +4+.4)-&(".81 97"#8#9&1 @"$('-)#):, 0-)#"µ+3+"81($: µ.)"+ 7 9$%)"::1)'1/.+ ("µE: (&1 µ9($D4)(81.

B&$C4;&'(

!3"4?9" @"$K+-".A "#+C?%"$ @"$('-)#): (&1 >9µ94"&@81 µ9%9>81 (+-µ', µAC$,

91E-%9"$) %"$ ()1 3$-+0' 493(+µ9-9"$.81 3-+D4EN9&1 $1$K+-".A µ9 ()1 #)µ9"$.' $1A46#) (): -+':. 21$@9".1?9" µ)0$1"#µ<

3$-$%&%': -+,.81 39@5&1.

B&$,-$-&'(

H($1 @91 63A-0+61 @"$>E#"µ$ >9&-)(".A µ+1(E4$, #9 3-8() 3-+#E%%"#) 0-)#"µ+3+"95($" ) @"$#($(".' $1A46#). O-"1 ()1 @"97$%&%' 39"-$µA(&1 ' 3-+#+µ+"8#9&1 0-9"AC9($" 1$ %1&-5C+6µ9 (": .$>+-"#(".E: $@"A#($(9: %9&µ9(-".E: ' K6#".E: 3$-$µE(-+6: (3.0. Re) 8#(9 1$ 94$0"#(+3+")>+?1 +" D$>µ+5 9496>9-5$: (+6 #6#('µ$(+:.

Page 8: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

D1;µ154,67 6#, +0$#µ,67 /µ/,>5'5#

L9 39"-Aµ$($ .$" #9 µ+1(E4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63A-09" %9&µ9(-".' .$" @61$µ".' +µ+"<()($ µ9 ()1 3-$%µ$(".' -+', @)4. 1$ 0$-$.()-5C9($" (+ 39@5+ -+': $3< (": 5@"9: ("µE: (&1 .$>+-"#(".81 $@"A#($(&1 3$-$µ(9(-&1 (3.0. Reynolds number Re, Mach M).

;&% 0,'1/"6µ",0 5.:"'01 *'1 "6,01 :"#µ"'$1/< *µ%10 "<, *5"+ %1 :$0µµ1/.+ 310)'<)"1+ '%( ",*+ 0,'1/"1µ.,%( "6,01 µ10 )'0="$7 0,05%:60 '%( )(,*5%( '#, 0,'6)'%1-#, 310)'<)"#,

'%( 3"&'"$%( 0,'1/"1µ.,%(.

;&% :"#µ"'$1/< *µ%10 0,'1/"6µ",0 5.:"'01 *'1 "6,01 3(,0µ1/< *µ%10 "<, %1 3(,<µ"1+ 9%(

0)/%&,'01 )" 0,'6)'%1-"+ =.)"1+ "96 '#, 3&% 0,'1/"1µ.,#, "6,01 90,'%& µ" '4, 6310 0,05%:60.

D*Aµ*-;&'( 4µ4&1-"-$

B+%$µ&'( 4µ4&1-"-$

y!

U11

2x! 2

2

1

U2

2"

"

p

p

1x!

1y!

Page 9: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

)4,2µ>* Reynolds

FinertialFviscous

=ma!!

"FinertialFviscous

~"L3( ) LT 2( )µU L( )L2

~!UTL2( ) UT( )

µUL=!U 2L2

µUL

"FinertialFviscous

~ !ULµ

= Re

Re = !ULµ

O Reynolds number "6,01 % 5*:%+ '#, 03$0,"10/8, #+ 9$%+ '1+ 3(,<µ"1+ 1>83%(+

<3+6 $ ) 36.1<()($, U (+ µE%9>+: ($0?-()($:, L (+ µE%9>+: (+6 µ'.+6:, µ (+ "78@9:.

(b)

(a)

glass pipe dye streak

laminar transitional turbulent

P"$ Re<<1, 639-"#0?+61 +" "78@9": @61Aµ9":. P"$ Re>>1, 639-"#0?+61 +" $@-$19"$.E: @61Aµ9":. P"$ Re<2000, ) -+' 951$" #(-&('. P"$ Re>4000, ) -+' 951$" (6-D8@):. P"$ Re~2000-4000, µ9($D$(".'.

Page 10: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

E,$'µ#5,67 5;$ 81095F$

•! B" "@"<()(9: (&1 -96#(81 >9&-+?1($" #)µ9"$.E: #61$-('#9": (): >E#): (+6: 4<%& (): >9&-5$: #6190+?: µE#+6 3+6 ($ @"E39"

•! Q1$ #&µ$(5@"+ -96#(+? ($6(+3+"95($" µ9 DA#) (": #61(9($%µE19: (+6 .A3+"$ 0-+1".'

#("%µ' t0, ' $44"8: (": #61(9($%µE19:, x0, y0, z0, +" +3+59: @"$µ+-K81+61 (+ A16#µ$ >E#):.

•! B" #61(9($%µE19: 91<: #&µ$("@5+6 -96#(+? #9 .A3+"$ 0-+1".' #("%µ' t +1+µAC+1($" 0&-".E: #61(9($%µE19:, x, y, z, +" +3+59: @"$µ+-K81+61 (+ 0&-".< A16#µ$ >E#):

!u = !u x, y, z, t( ) = u x, y, z, t( ) x + v x, y, z, t( ) y+w x, y, z, t( ) z! = ! x, y, z, t( )T = T x, y, z, t( )

!R0 =

!R x0, y0, z0, t0( )

!R =!R x, y, z, t( )

Page 11: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

•! O$-$.+4+?>)#) (): 3+-95$: (+6 .A>9 µ9µ+1+µE1+6 #&µ$("@5+6 (+6 -96#(+?, .$>8: $6(< ."195($" $3< .A3+"$ $-0".' >E#) (#$1 1$ (+3+>9(+?µ9 E1$ “(+3".<” #?#()µ$ #61(9($%µE1&1 93A1& (+6).

•! O9-"%-$K' (&1 µ9($D+481 (&1 "@"+('(&1 (&1 #&µ$("@5&1 .$>8: $6(A ."1+?1($".

•! B" 97"#8#9": .51)#): 951$" #09(".A $34E:. •! R#(<#+, +" 4?#9": @51+61 µ<1+ #("%µ"$5$

() 0&-".' >E#) (&1 #&µ$("@5&1 -96#(+? (L61(9($%µE19: $197A-()(9: (+6 0-<1+6).

•! S-'#"µ) 3.0 spray, -+' µ9 K6#$45@9: ' #&µ$(5@"$.

G-2/+/, 314,=4#H7* 31+@/0 8/7*

E$F';$%9&$%( (Lagrangian) G*;&F;$C(

?&@*;&$%( (Eulerian) G*;&F;$C(

T3A-0+61 @6+ 3-+#9%%5#9": %"$ 1$ .$>+-5#+6µ9 (": 0&-".E: #61(9($%µE19: 91<: #)µ95+6 µE#$ #9 -96#(<, $1A4+%$ µ9 (+ #?#()µ$ $1$K+-A: &: 3-+: (+ +3+5+ $1A%9($" ) .51)#).

•! 21("#(+"095 #9 #6%.9.-"µE1+ #?#()µ$ #61(9($%µE1&1 #(+ 08-+, #(+ +3+5+ +" "@"<()(9: (+6 -96#(+? µ949(+?1($" &: #61$-('#9": (+6 -$*,%( .$>8: ) -+' 39-1A9" $3< )'0="$.+ 0&-".E: >E#9":.

•! G+ #?#()µ$ $1$K+-A: µ3+-95 1$ 951$" #($>9-< ' 1$ ."195($" µ9 3-+.$>+-"#µE1+ (-<3+ (3.0. 1$ 39-"#(-EK9($").

•! O"+ .$(A44)4) 39-"%-$K' %"$ 3-$.(".+?: 4<%+6:. J6-5$-0) #($ 39-"##<(9-$ 3-+D4'µ$($ -96#(+@61$µ".':.

Page 12: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

1

2! !

2 2 20 0 0" # $ % &

1

!

0 0 0" # $ % &

G-2/+/, 314,=4#H7* 31+@/0 8/7* U µ9($(-+3' µ9($7? (&1 @?+ µ9><@&1 39-"%-$K': (+6 39@5+6 -+': 951$" #61'>&: @?#.+4) #()1 3-A7), .$>8: 3.0. $3< B"49-"$1' #9 V$%.-$1C"$1' >$ E3-939 1$ D-+?µ9 <49: (": (-+0"E: <4&1 (&1 #&µ$("@5&1 3+6 ."1+?1($" #(+ -96#(<!

X

z

y

2

(1)2

X

x

particle path #1

(2)

particle path #2

X(0)1

X1

1(2)X

(1)

X2(0)

typical measurementlocations

x

z

y

E$F';$%9&$%( (Lagrangian) G*;&F;$C(

?&@*;&$%( (Eulerian) G*;&F;$C(

Page 13: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

"!)* “95#2/Iµ1” +0/ &1"5%! G-B4, 5F4# µ,&79#µ1 =,# "4/J&7µ#5# 41095/+0$#µ,67*, +'&. 41095F$ 91 6@$'9'. C@ 90µJ#@$1, =,# 41095% 91 #6,$'9@#;

Page 14: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

"!C, 1.15%K1, ' 95#5,67 5;$ 41095F$;

H ,-$-&'( -A% ;*+,-.% $,#4@*>-$& µ* -" µ*@7-" ;*+,-.% ,* ";*µ>$, I"@. $C4;8 0;4J@(µ$-$ ,-$ 404>$

I*% +08;#*& '>%"," ;*+,-45.

<& ,"µ$>%*& $+-1 F&$ -"% -$#5-"-$ '$& -&6 I&$-µ"-&'76 -8,*&6 (shear stresses)

-4+ ;*+,-45;

Page 15: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!! !K$-µ+%E:; !! !3"34E+1($ ' D6>"#µE1$ #8µ$($, K-A%µ$($, @97$µ91E: .43.

H ,-$-&'( -A% ;*+,-.% 7#*& %1"µ$ µ1%4 F&$ ;*+,-1 04+ &,4;;40*> ,-4 0*I>4

J$;5-"-$6.

?& µ*-$J4@76 -"6 0>*,"6 4C*>@4%-$& ,-4 J8;46 -4+ +0*;'*>µ*%4+ ;*+,-45.

A0$1"F*, /, µ>$1* 5%91,* "/0 0"%4B/0$ 1@$#, /, 6%2151* 6#, /H1@&/$5#,

95'$ /0*," p.

K;$, " -$#5-"-$ *>%$& 0$%-45 µ"I*%&'( '$& I*% +08;#4+% I&$-µ"-&'76 -8,*&6 04+

0$;$µ4;C.%4+% -4 ;*+,-1.

"!C, 1.15%K1, ' 95#5,67 5;$ 41095F$;

H ,-$-&'( -A% ;*+,-.% $,#4@*>-$& µ* -" µ*@7-" ;*+,-.% ,* ";*µ>$, I"@. $C4;8 0;4J@(µ$-$ ,-$ 404>$

I*% +08;#*& '>%"," ;*+,-45.

Page 16: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

H 96")4 9%( 0)/"6'01 09* '% (:$* )" .,0 )4µ"6% '%( )" ?<=%+ h 09*

'4, "91@<,"10, %@"65"'01 )'4, ">#'"$1/7 3&,0µ4 '4+ ?0$&'4'0+ /01 µ*,% ("91'<-(,)4+ g), 345037

)'% ?<$%+ '%( $"()'%& 9%( ?$6)/"'01 (9"$<,#: p(3$=$gh

/I;4,-$-&'( 0>*,"

=*µ*@&.I"6 %1µ46 -"6 /I;4,-$-&'(6

L,+µ0>*,-4 +F;45

H 36.1<()($ $ 951$" 39-53+6 #($>9-'.

p = p0 + !gh

L;#( -4+ Pascal

H !"#$% !&' ($)#"*(+ $*%, #!+-.,#+( #,/0 '12&3 p0 µ#*(4"4#*(+ &µ&+/µ&2-(

#,*/0 ('*&3, !2&0 /5#0 *+0 4+#'63,$#+0 (&,1-)1/0$) )(+ $# /5& *& 7.6&0 *&', (,#8.2*%*( *%0 7(23*%*(0 (45. +6µ7'8+9%91: 4)-'( :

4)-'( +4; <µ=7.7).

Page 17: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

'

(

)

% +%

)) +% +#+"%%

) +#+"

(*

(*

+(

+)

+'

* * * * * * **** * * * * * * * ** * * * * * **** * * * * * * ** * * * * *

*** * * * * * * *

*

! +#+%+"

)">+1,.'

M9&-+?µ9 E1$1 #(+"09"8@) .?D+ -96#(+? #9 )-9µ5$ µ9 $.µE: µ'.+6: dx, dy .$" dz. G+ "#+C?%"+ (&1 @61Aµ9&1 (): 359#): .$" (): D$-?()($: #(": (-9": .$(96>?1#9": (+6 .6D+9"@' <%.+6 94E%0+6 >$ 951$" (>6µ)>95(9 F=p*A):

pxdydz! p

x+dx+"p"xdx

#

$%

&

'(dydz = 0)

"p"x

= 0

pydzdx ! p

y+dy+"p"ydy

#

$%

&

'(dzdx = 0)

"p"y

= 0

pzdxdy! p

z+dz+"p"zdz

#

$%

&

'(dxdy! !gdxdydz = 0)

"p"z

= !g

*

+

,,,

-

,,,

!!F = 0"#

"!p = ! !g"

$p$xx + $p

$yy+ $p

$zz = !gz

pz=%h

% pz=0= !gdz

z=%h

z=0

& = !gh"

p = p0 + !gh

Page 18: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

3#4#+1@=µ# – L1.#µ1$7

G+ #0'µ$ @95019" µ5$ @97$µ91' %9µA() µ9 39-"+0E: 19-+? .$" 6@-$-%?-+6. A*)% "6,01 4 µ0,%µ"'$1/7 91.)4 (gage) )'0 )4µ"60 B, C, C, D; (µ$1+µ9(-".' 951$" ) 359#) #9 E1$ #)µ95+ #9 #0E#) µ9 µ"$ #($>9-' 359#) $1$K+-A: p0, 3+6 951$" #61'>&: ) 39-"DA44+6#$ ' $(µ+#K$"-".' 359#), pµ0,= pabsoluteDp0)

h

DA C

Air

H

B(a)

!"#$%

&'#(

)*#+#,-#.%

pA = pB = pC = !"#!$%gH pD = !"#!$%gh+ !"#!$!%"!&"g H ! h( )

Page 19: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

3#4#+1@=µ# – A;&7$#*

G+ #0'µ$ @95019" E1$ #&4'1$ 3+6 39-"E09" 19-< .$" 6@-A-%6-+. A*)% "6,01 4 µ0,%µ"'$1/7 91.)4 (gage) )'0 )4µ"60 B, C, C, D, E; 26(' () K+-A, @91 µ3+-+?µ9 1$ #6#09(5#+6µ9 (": 3"E#9": µ9 ()1 $(µ+#K$"-".' 359#), @9@+µE1+6 <(" @91 63A-09" $1+"0(' 93"KA19"$ #()1 $(µ<#K$"-$. 21( '$6(+?, >$ #6#09("#(+?1 &: 3-+: ()1 359#) #(+ #)µ95+ O, 3+6 #6µD+45C9($" p0.

pA = p0 + !"#!$%gapB = p0 ! !"#!$%gbpC = p0 + !"#!$%gc

pD = pC + !"#!$!%"!&"g d ! c( ) = ;

pE = pD ! !"#!$!%"!&"g d + e( ) = ;

Oh

(b)A D

a dc

e

E

b

B

C

Mercury

Water

!"#$#%&#'(

)*#+

Page 20: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

3#4#+1@=µ# – LI5'*

A*)4 96")4 01)=<,"'01 % 3&'4+ )'0 30 m ?<=%+;

pµ!" ,2 = #"$#%&gH = 998 kgm3

!

"#

$

%& 9.81

ms2

!

"#

$

%& 30m( )

= 293.711kPa 1atm101.325kPa!

"#

$

%& ' 2.9atm

pabsolute,2 = pµ!" ,2 + patm = 2.9atm+1atm = 3.9atm

$

!""#$%

!

&$

$ $

30 m

E9<$-"1 /6,3(,%+ /0'< '4, 09*'%µ4 "90,0@%$< '%( 3&'4 )'4, "91@<,"10;

P1V1 = P2V2V1V2

=P2P1=3.9atm1atm

! 4

;<µ+: (+6 Boyle %"$ "#+>9-µ+.-$#"$.E: µ9($D+4E: (): 359#)::

!A1 .$195: .-$('#9" ()1 $1$31+' (+6 .$(A ()1 93A1+@+ #()1 93"KA19"$ (): >A4$##$:, + <%.+: (&1 3196µ<1&1 #09@<1 >$ (9(-$34$#"$#>95 µ9 $3+(E49#µ$ ()1 9µD+4' .$", 91@90+µE1&:, (+1 31"%µ<.

Page 21: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

K%A," L;#76 -4+ L;#&µ(I"

1" $;#(

F 0,#)'1/7 3&,0µ4 9%( 0)/"6'01 )" .,0 ?(=1)µ.,% )8µ0 1)%&'01 µ" '% ?<$%+ '%( (:$%& 9%( "/'%962"1, .-"1 /0'"&=(,)4 9$%+ '0 "9<,# /01 )4µ"6% "@0$µ%:7+ '% /",'$%"13.+ '%( "/'%912*µ",%( *:/%(.

2" $;#(

G8µ0 9%( "9195."1 "/'%962"1 9%)*'4'0 '%( 9"$1?<55%,'%+ $"()'%& 6)4 µ" '% ?<$%+ '%(

)8µ0'%+. (V$µDA19($" 63<N) µ<1+ E1$ .4A#µ$ (+6 #61+4".+?

<%.+6 (+6 #8µ$(+:, 3+6 $1("#(+"095 µ9 (+ 3+#+#(< .A(& $3< ()1 93"KA19"$ (+6 6%-+?.)

F 3&,0µ4 '4+ <,#)4+ "6,01 4 /0'0/*$(@4 3&,0µ4 9%( 3.-"'01 )8µ0 9%( "9195."1 7 "6,01 ?(=1)µ.,%, 5*:# '4+ 310@%$<+ '4+ (3$%)'0'1/7+ 96")4+ µ" '% 9"$1?<55%, $"()'*.

FA = ! fluidVg

Page 22: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

"

$$

$$

#

232 2

#

232 22

32 22

32 2

!"#$ %&' (%)%*+()

!"#$ %&' $),-(./$) (&'0+/(-1

%*('2/3/1/$)

!"#$ %&' 4'5.6(/$)

78-3

!","&-/$5#, #,;4/Iµ1$# 6#, J02,K>µ1$# 9Fµ#5#

$body < $fluid

G+ #8µ$ 93"34E9"

$body = $fluid

G+ #8µ$ $"&-95($"

$body > $fluid

G+ #8µ$ D6>5C9($"

FA = ! fluidVg

Page 23: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!F!"#"!$%&'( = FA "FW = 0

FA = %)*%$& 34 h

3g

FW = %!&+$&h3g

#

$%

&%%!&+$& =

34%)*%$&

•! H #61+4".' .$($.<-6K) @?1$µ) "#+?($" µ9 (+

DA-+: (+6 6%-+? 3+6 9.(+35C9" (+ #8µ$:

3#4%+1,=µ#

M9&-+?µ9 E1$1 .?D+ 3496-A: h 3+6 93"34E9" #9 19-<, µ9 µ<1+ (+ W (+6 µ'.+6: (+6 3A1& $3< ()1 93"KA19"$. A%1< "6,01 4 9(/,*'4'0 '%( /&?%(;

•! U #61+4".' +-"C<1("$ @?1$µ) 3+6 6K5#($($" (+ #8µ$ 951$" µ)@E1 ("#+--+35$ @61Aµ9&1):

!F!"#$!%&#' = 0

g

FW

F

1

b

hh4

!

Page 24: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

M+,-82&$ 0@A-.% ,Aµ8-A%

F 9"$1)'$%@1/7 "()'<="10 95#'8, )#µ<'#, ">0$'<'01 09* '4, )-"'1/7 =.)4 '%( /.,'$%( ?<$%(+ G /01 '%( /.,'$%( <,#)4+ B.

•! G .$($.<-6K$ .A(& $3< (+ *: 9<,'0 "()'<="10 •! G ($6("C<µ91+ µ9 (+ *: %(3.'"$4 "()'<="10 •! G .$($.<-6K$ 93A1& $3< (+ *: 0)'<="10 (9* )(,=7/"+ (µ9 .$(A44)4) #($>9-+3+")(".' -+3' µE#& (): µ9($.51)#): (+6 .E1(-+6 A1&#):) G vs B

#

%

!"#$

%&#'(

%&#'(

)*+,&-./0 1*23,.#4 .*+,&-./0 5+,&-./0

#

%

!"#$%

&$'( )'*+*,$#"%

Page 25: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!"#$%& '()*+ ,-) ./)'01234% (5+&

6/5,788%4%4235()-,59 4'(#:-'5&

;'.<-3)-=- (5+

-=:-'5& u

"!Let the flow begin! E@$'9'!

Page 26: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!.,9F91,* 6@$'9'* 41095F$

B&$-(;"," !89$6 – MN>,A," 3+%7#*&$6

B&$-(;"," ?;µ(6 - Navier-Stokes equation

B&$-(;"," M%7;F*&$6

!.(<: $3< ()1 T3<>9#) L6190+?: /E#+6 3+6 $1$KE-$µ9 '@), 63A-0+61 (-9": .?-"9: K6#".E: "@E9: 3+6 $3+(94+?1 () DA#) (): @61$µ".': (&1 -96#(81:

1

2

3

Page 27: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

1

!! L;#( I&$-(;","6 -"6 µ89$6 F )(,%51/7 µ<20 m ",*+ $"()'%& 310'4$"6'01 )'0="$7. =)4. + -6>µ<: µ9($D+4': (): µAC$: (+6 -96#(+? 3-E39" 1$ 951$" µ)@E1.

H3+6 R(t) µ"$ (60$5$ 39-"+0' 3+6 39-"E09" #6%.9.-"µE1) µAC$ m (+6 -96#(+?. U 36.1<()($ $ 935#): µ3+-95 1$ 951$" 0-+1".A µ9($D$44<µ91).

L,#574'9' µ%K#* – !.@9;9' 90$-B1,#*

dmdt

=ddt

! dV = 0R(t )!

•! P"$ $#6µ359#() -+' ) 36.1<()($ $ >9&-95($" #($>9-', @)4.

.$" #61938: ) !75#&#) L61E09"$: %519($":

!! !t = 0!"!u = 0

!!!t+"# !

!u( ) = 0230,4," 5+%6#*&$7 (Continuity Equation)

! =""xx + "

"yy+ "

"zz

#

$%

&

'(

Page 28: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

G(,%51/7 "91'<-(,)4 = "91@0,. 3(,<µ"1++ ">#'"$1/.+ 3(,<µ"1+ !

{H(=µ*+ µ"'0?%57+ '4+ %$µ7+} = {I=$%1)µ0 3(,<µ"#,} !

2

!! B*5-*;46 O1µ46 -4+ O*5-A%$ F )(,%51/7 3&,0µ4 F 9%( 0)/"6'01 )" .,0 $"()'* "6,01 6)4 µ" '% $(=µ* µ"'0?%57+ '4+ %$µ7+ '%(.

L,#574'9' /4µ7* – Navier-Stokes equation

d m!u( )dt

=!F

!DDt

!R t( )" !udV =

!FSS t( )" dA +

!FBR t( )" dV

G(,%51/7 "91'<-(,)4 = F96")4+ + F1>834+ + F?0$&'4'0+ !

Page 29: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

2 L,#574'9' /4µ7* – Navier-Stokes equation

! !"!u"t+ !!u #$!u

R t( )% dV =!FSS t( )% dA +

!FBR t( )% dV

J10 K"('8,"1%, 0)(µ96")'% $"()'*:

! !"!u"t+!u #$( )

!u%

&'

(

)* = +$p + µ$2 !u + !g

! =""xx + "

"yy+ "

"zz

#

$%

&

'(

Navier-Stokes equation

!DDt

!R t( )" !udV =

!FSS t( )" dA +

!FBR t( )" dV

G(,%51/7 "91'<-(,)4 = F96")4+ + F1>834+ + F?0$&'4'0+ !

{H(=µ*+ µ"'0?%57+ '4+ %$µ7+} = {I=$%1)µ0 3(,<µ"#,} !

Page 30: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

T% 05:"?$1/* <=$%1)µ0 *5#, '#, µ%$@8, ",.$:"10+ )" .,0 $"()'* 310'4$"6'01 )'0="$* µ" '4, 9<$%3% '%( -$*,%(. T3A-0+61 3+44+5 @"$K+-9(".+5 (?3+" 91E-%9"$: (3.0. 9#&(9-".', ."1)(".', @61$µ".<, 0)µ".'), 3+6 µ3+-+?1 1$ .$($#('#+61 ()1 9K$-µ+%' (+6: #(+ >98-)µ$ 3"+ 39-534+.). R#(<#+, #601A µ$: 91@"$KE-9" µ<1+ #9 E1$: (?3+: (): µ9($K+-A: 91E-%9"$: (3.0. µ9($K+-A >9-µ<()($:). <3+6 Q 951$" ) 9#&(9-".' 91E-%9"$ and W 951$" (+ E-%+ $3< (+ #&µ$(5@"+ -96#(+?.

3 L,#574'9' 1$-4=1,#*

d(E)

dt=

dQ

dt−

dW

dt

dEsys

dt=ddt

!ECV! dV + !"

!ur # n( )dSCS!

Page 31: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!.,9F91,* 6@$'9'* 41095F$

!.(<: $3< ()1 T3<>9#) L6190+?: /E#+6 3+6 $1$KE-$µ9 '@), 63A-0+61 (-9": .?-"9: K6#".E: "@E9: 3+6 $3+(94+?1 () DA#) (): @61$µ".': (&1 -96#(81:

!!!t+"# !

!u( ) = 0

!!!u!t+!u "#( )

!u$

%&

'

() = *#p + µ#2 !u + !g

1

2

3 dEsys

dt=ddt

!ECV! dV + !"

!ur # n( )dSCS!

Page 32: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!.,9F91,* 6@$'9'* 41095F$

H49: +" 97"#8#9": .51)#): µ3+-+?1 1$ 9.K-$#(+?1 µ$C5 #()1 $.<4+6>) µ+-K': <3+6:

∂tU +

∂xFx +

∂yFy +

∂zFz =

∂xGx +

∂yGy +

∂zGz

U =

ρ

ρu

ρv

ρw

ρE

, Fx =

ρu

ρu2 + p

ρuv

ρuw

ρuH

, Fy =

ρv

ρvu

ρv2 + p

ρvw

ρvH

, Fz =

ρw

ρwu

ρwv

ρw2 + p

ρwH

Gx =

0

σxx

σxy

σxz

(σ · u)x + kTx

,Gy =

0

σyx

σyy

σyz

(σ · u)y + kTy

,Gz =

0

σzx

σzy

σzz

(σ · u)z + kTz

(σ · u)x = uσxx + vσxy + wσxz

(σ · u)y = uσyx + vσyy + wσyz

(σ · u)z = uσzx + vσzy + wσzz

σij = µ

[(

∂ui

∂xj+

∂uj

∂xi

)

− 23δij(∇ · u)

]

Page 33: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!.,9F91,* 6@$'9'* 41095F$

B" 97"#8#9": Navier-Stokes 951$" µ) %-$µµ".E: .$" 39-534+.9: %"$ 1$ 46>+?1. P"$ ;96(819"+ (@)4. µ #($>9-<) .$" $#6µ359#(+ (@)4. $ #($>9-<) -96#(<, 0&-5: 97&(9-".E: @61Aµ9":, +" Navier-Stokes µ3+-+?1 1$ 9.K-$#(+?1 &::

!!!u!t+ !!u "#( )

!u = $#p + µ#2 !u

!"!u = 0

P"$ &N.I" ;4( – Stokes Flow (Re<<1), +" <-+" 93"(A061#): µ3+-+?1 1$ $%1+)>+?1.

!"!u = 0

µ!2 !u "!p = 0

P"$ 8-;&J" ;4( (<3+6 +" @61Aµ9": (-"D': 951$" µ".-E:, @)4. - #61'>&: µ$.-"A $3< #(9-9E: 93"KA19"9:).

!!!u!t+ !!u "#( )

!u +#p = 0

!"!u = 0

µ! 0

Page 34: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!.@9;9' Bernoulli

F )(,%51/7 96")4, pT "6,01 )'0="$7 )" µ10 H%L/7 J$0µµ7 (streamlne) *'0, 4 $%7 "6,01: 1.! )'0="$7,

2.! 0)(µ96")'4,

3.! <'$1?4 (µ43",1/* 1>83"+),

4.! 3", 0)/"6'01 .$:% )'% $"()'* (9.-. 09* ">#'"$1/7 94:7),

5.! 3", (9<$-"1 µ"'0@%$< ="$µ*'4'0+.

pT = p+12!u2 + !gz

Page 35: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

3#4%+1,=µ# – 8/7 #"> #64/HI9,/ +1.#µ1$7*

F 3">0µ",7 '%( )-7µ0'%+ "6,01 :"µ<'4 µ" ,"$*, /01 .-"1 "µ?03*, "91@<,"10+ B1 /01 .,0 µ1/$* 0/$%@&)1% "µ?03%& B2 )" ?<=%+ h 09* '4, "91@<,"1< '%(. A%1< "6,01 4 '0-&'4'0 '4+ $%7+ 09* '% 0/$%@&)1%;

21 ) 93"KA19"$ (): @97$µ91': 951$" #9 ?N+: z1 (<(9 ) #61+4".' 359#) #()1 93"KA19"$ 951$":

<3+6 pA ) $(µ+#K$"-".' 359#). L(+ $.-+K?#"+, ) 359#) 951$" 935#): pA, (+ ?N+: 951$" z2=z1-h .$" ) ($0?()($ u2:

26(A ($ 2 #)µ95$ µ3+-+?1 1$ #61@9>+?1 µ9 µ"$ -+I.' %-$µµ' .$" A-$

pT1 = p! +12!u1

2 + !gz1

pT 2 = p! +12!u2

2 + !gz2

pT1 = pT 2 ! u22 "u1

2 = 2g z1 " z2( ) = 2gh/9 DA#) () @"$('-)#) µAC$:, + -6>µ<: µ9($D+4': #()1 93"KA19"$ u1A1 951$" 5@""+: µ9 (+ -6>µ< µ9($D+4': #(+ $.-+K?#"+ u2A2.

u22 − u2

1 = u22

1 −A2

2

A21

= 2gh ⇒ u2 =

2gh

1 − A22/A

21

≈�

2gh,

T3+>E(+6µ9 <(" ) -+' 951$" #($>9-', (+ 19-< 951$" $#6µ359#(+ .$" $%1++?µ9 935@-$#) "78@+6: .$>8: .$" >9-µ".E: 93"@-A#9":. R: 9. (+?(+6, +" <-+" (): Bernouilli 951$" ".$1+3+")µE1+".

Page 36: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

3#4%+1,=µ# – A;&7$#* Venturi

M,0+ )#57,0+ Venturi 0,0:/<2"1 '% $"()'* ,0 9"$<)"1 09* µ10 )'.,#)4 (-#$6+ /0µ60 0985"10 ",.$:"10+). C$"6'" µ10 ./@$0)4 :10 '4, 96")4 P2 ",'*+ '4+ )'.,#)4+, 8+ 9$%+ '4, 9(/,*'4'0 $"()'%& $, '0 "µ?03< B1 /01 B2 /01 '4, '0-&'4'0 $%7+ U1 /01 96")4+ P1 )'4, "6)%3%.

!K$-µ<C+1($: ()1 975#&#) Bernoulli ($%1+81($: () D$-?()($ .$" >9&-81($: $#6µ3"9#(<()($) E0+6µ:

P1 +12!U1

2 = P2 +12!U 2

2

/9 DA#) () @"$('-)#) µAC$:, + -6>µ<: µ9($D+4': #()1 93"KA19"$ u1A1 951$" 5@""+: µ9 (+ -6>µ< µ9($D+4': #(+ $.-+K?#"+ u2A2.

U1A1 =U2A2 !U2 =U1A1A2

P2 = P1 +12!U1

2 !12!U 21A

21

A22"

P2 = P1 +12!U1

2 1! A21

A22

#

$%

&

'(

Page 37: -494 !#$%&'( )*+,-.% · 2015-05-26 · d1;µ154,67 6#, +0$#µ,67 /µ/,>5'5# l9 39"-aµ$($ .$" #9 µ+1(e4$ 3-+#+µ+5&#): 93">6µ+?µ9 1$ 63a-09" %9&µ9(-".' .$" @61$µ".' +µ+"

!0B#4,95F! [email protected]


Recommended