Chapter 1: Fluid Flow Rules of Thumb for Chemical Engineers, 5th Edition by Stephen all
This Excel workbook includes Visual Basic for Application function subroutines. Macros must be enabled for them to work. The following Text Text Boxes contain the syntax for the functions. Copy them to the worksheet where you want to use the functions for ready reference. Function Subroutines in S! "nits Function #ReS!!" #ReS! !" mu" d" #ptional ro" #ptional Tin" #ptional Mw" #ptional p$ % ! & 'lowrate in kg(h % mu & Viscosity in m)a*s % d & )ipe+, in mm % ro & density in kg(m- reuired for liuid$ % Tin & temperature" deg C reuired for gas$ * default /0 deg C % Mw & molecular weight reuired for gas$ * default /1 % p & pressure" k)a reuired for gas$ * default 2000 k)a
Function FrictionS!epsilon" FrictionS! epsilon" 34e" d$ % epsilon & 5urface roughness is in units m % d & )ipe+, is in units mm Function $%S!!" $%S! !" )in" )out" d" 6" f" #ptional ,ensity" #ptional Tin" #ptional Mw" #ptional 7amma" #ptional +sothermal$ % )ressure ,rop due to friction in a round pipe adiabatic for compressible flow$ % with the following arguments % 5pecify two of the following three8 function will compute the third % ! & mass mass flow flow rate" kg(h % )in & inlet" inlet" or upstream" pressure" k)a % )out & outlet" or downstream downstream pressure" k)a % )ipe properties % d & pipe diameter" diameter" mm % 6 & pipe length" m % f & ,arcy friction factor % 'luid properties % ,ensity optional$ optional$ ** specify specify for liuids" kg(m% Tin optional$ optional$ ** specify for for gas" inlet temperature" temperature" deg C default default to /0$ % Mw optional$ ** specify for gas" molecular molecular weight default to /1 for air$ air$ % 7amma optional$ ** specify for gas" ratio ratio of Cp(C9 Cp(C9 default to 2.:$ % +sothermal optional$ ** any 9alue results in isothermal compressible calc" if missing then adiabatic calc
ChemEng 5oftware sells an Excel template called )+)E5+;E. www.chemengsoftware.com )+)E5+;E si
Function Subroutines in "S "nits Function #Re"S!" #Re"S !" mu" d" #ptional ro" #ptional Tin" #ptional Mw" #ptional p$ % ! & 'lowrate in lb(h % mu & Viscosity in c) % d & )ipe+, in inches % ro & density in lb(ft- reuired for liuid$ % Tin & temperature" deg ' reuired for gas$ * default =0 % Mw & molecular weight reuired for gas$ * default /1 % p & pressure" psia reuired for gas$ * default 22>
Function Friction"Sepsilon" Friction"S epsilon" 34e" d$ % epsilon & 5urface roughness is in units feet % d & )ipe+, is in units inches Function $%"S!" $%"S !" )in" )out" d" 6" f" #ptional ,ensity" #ptional Tin" #ptional Mw" #ptional 7amma" #ptional +s % )ressure ,rop due to friction in a round pipe adiabatic or isothermal for compressible flow$ % with the following arguments % 5pecify two of the following three8 function will compute the third % ! & mass mass flow rate" lb(hr % )in & inlet" inlet" or upstream" upstream" pressure" pressure" psia % )out & outlet" outlet" or or downstream downstream pressure" pressure" psia % )ipe properties % d & pipe diameter" diameter" inches % 6 & pipe length" feet % f & ,arcy friction factor % 'luid properties % ,ensity optional$ ** specify specify for liuids" lb(ft% Tin optional$ optional$ ** specify for gas" inlet temperature" temperature" deg ' default default to =0$ % Mw optional$ ** specify for gas" molecular molecular weight default to /1 for air$ air$ % 7amma optional$ optional$ ** specify specify for gas" ratio of Cp(C9 Cp(C9 default to 2.:$ % +sothermal optional$ ** any 9alue results in isothermal compressible calc" if missing then adiabatic calc
thermal$
$roblem Statement: Calculate pressure drop per 200 m or 200 ft using the shortcut formula 5+ ?nits ?5 ?nits !nputs 'low 4ate Viscosity )ipe ,iameter ,ensity
kg(h m)a*s mm kg(m-
,elta )
Bar(200 m
20"000.0 2./
[email protected] 1=2.>
lb(h c) in lb(ft-
//"000.0 2./ 2.> =0.0
&utput 2.@-
psi(200 ft
@.01
$roblem Statement: Calculate 4eynolds 3umber using VBA function function call.
!nputs )arameter Mass 'low 4ate Viscosity )ipe ,iameter ,ensity Temperature Molecular !eight )ressure
?nits kg(h m)a*s mm kg(mC kg(kgmol k)a" absolute
4eynolds 3umber
dimensionless
6iuid 7as Example 2 Example / 20"000.0 2"/00.0 2./ 0.022
[email protected] /=.= 1=2.0 :0.0 2=.0: /"/00.0
&utput
&34e5+,@",1",20",22$
VA6?E
VA6?E
&34e5+E@"E1"E20""E2/"E2-"E2:$
?5 Customary ?nits ?nits lb(h c) in lb(ft' lb(lbmol psia
6iuid 7as Example 2a Example /a //"000.0 /"=:>.0 2./ 0.022 2.> 2.0: =0.0 20:.0 2=.0: -21.0
VA6?E
&34e?5+@"+1"+20"+22$
VA6?E
&34e?5D@"D1"D20""D2/"D2-"D2:$
$roblem Statement: Calculate ,arcy 'riction 'actor using VBA function function call.
!nputs
6iuid Example /10.0 2./
[email protected] 1=2.0
)arameter Mass 'low 4ate Viscosity )ipe ,iameter ,ensity Temperature Molecular !eight )ressure
?nits kg(h m)a*s mm kg(mC kg(kgmol k)a" absolute
)ipe 4oughness
m
4eynolds 3umber
dimensionless
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
0.0000:>
&utput
&'riction5+,2=",21",20$
?5 Cus Custo tom mary ary ?ni ?nitts ?nits lb(h c) in lb(ft' lb(lbmol psia
6iu 6iuiid Example -a //"000.0 2./ 2.> =0.0
ft
0.0002>
VA6?E VA6?E
&'riction?5+2="+21"+20$
$roblem Statement: Calculate )ressure ,rop due to 'riction
!nputs
6iuid 7as Example : Example > 20"000.0 2"/00.0 00.0 /"/00.0
)arameter Mass 'low 4ate )ressure in upsteam$
?nits kg(h k)a" absolute
Viscosity )ipe ,iameter Eui9alent 6ength of )ipe ,ensity Temperature Molecular !eight Cp(C9
m)a*s mm m kg(mC kg(kgmol
)ipe 4oughness
m
4eynolds 3umber
dimensionless
VA6?E
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
VA6?E
VA6?E
VA6?E
2./
[email protected] :0.0 1=2.0
0.022 /=.= =0.0
0.0000:>
:0.0 2=.0: 2.-> 0.0000:>
&utput
)ressure #ut" gi9en Mass 'low and )ressure in
&),5+,@",1"",2/",2-",/:",2:$
&),5+E@"E1""E2/"E2-"E/:""E2>"E2="E2$
?5 Customary ?nits ?nits lb(h psia c) in ft lb(ft' lb(lbmol
6iuid 7as Example :a Example >a //"000.0 -"
[email protected] 202.> -21.0
2./ 2.> 2-2.0 =0.0
0.022 2.0: 21.0
ft
20:.0 2=.0: 2.->
0.0002>
0.0002>
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
&),?5+@"+1""+2/"+2-"+/:"+2:$
&),?5D@"D1""D2/"D2-"D/:""D2>"D2="D2$
$roblem Statement: Calculate 'low 4ate gi9en upstream and downstream pressures
!nputs
7as )arameter 7?E55 Mass 'low 4ate )ressure in upsteam$ )ressure out downstream$ Viscosity )ipe ,iameter Eui9alent 6ength of )ipe
?nits kg(h k)a" absolute
Example > 2/00 //00 2-:0 0.022 /=.= =0
Temperature Molecular !eight Cp(C9
C kg(kgmol
)ipe 4oughness
m
4eynolds 3umber
dimensionless
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
m)a*s mm m
:0 2=.0: 2.->
0.0000:>
&utput
Mass 'low" gi9en )ressure in and out
VA6?E
&),5+ "E1"E20"E2/"E2-"E/:"E2:"E2>"E "E1"E20"E2/"E2-"E/:"E2:"E2>"E2="E2$ 2="E2$ ,ifference between 7?E55 and ca calculated ra rate" E@*E/=
VA6?E
?s the tha C 3u 7u
7oal 5eek to find a 9alue for 7uessed flow rate Cell E@$ t euals the calculated flow rate ll E/=$. 3otice that 4eynolds mber is calculated using the ess.
?5 Cust Custom omar ary y ?nit ?nits s
7as 7as
?nits lb(h psia psia c) in ft
Example >a -"0@0.: -21.0 22= 0.022 2.0: 21.0
' lb(lbmol
ft
20:.0 2=.0: 2.-> 0.0002>
VA6?E VA6?E VA6?E
&),?5 "61"620"62/"62-"6/:""62>"62="6 "61"620"62/"62-"6/:""62>"62="62$ 2$ VA6?E
$roblem Statement: Compare pressure drop calculations using e ui9alent length and G*9alue methods for fittings.
!nputs )arameter Mass 'low 4ate )ressure in upsteam$
?nits kg(h k)a" absolute
Viscosity )ipe ,iameter 6ength of )ipe ,ensity Temperature Molecular !eight Cp(C9
m)a*s mm m kg(mC kg(kgmol
)ipe 4oughness
m
Fittings
6iuid 7as Example : Example > 20"000.0 2"/00.0 00.0 /"/00.0 2/.0 >0.0
[email protected] 1=2.0 0.0000:>
0.022 /=.= =0.0 2-.= :0.0 2=.0: 2.-> 0.0000:>
uantity = / / 2
10 deg" welded r(, & 2 TEE" through branch as elbow$ )lug 9al9e" straight 5wing check" Vmin & -> roF0.>
&utput 4eynolds 3umber
dimensionless
VA6?E
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
VA6?E
VA6?E
VA6?E
)ressure ,rop" gi9en Mass 'low and )ressure in
Eui9alent length of fittings
m
2:.@0
.@
)ressure ,rop" eui9 length method
VA6?E
VA6?E
Mass flux Velocity
kg(m/*s m(s
2":2:.2 2.:
>11.@::./>
'itting pressure loss
kg(m/ k)a
VA6?E VA6?E
VA6?E VA6?E
)ressure ,rop" -*G method
VA6?E
VA6?E
)ressure ,rop" Crane method
VA6?E
VA6?E
E 6
6(,$e /0 /0 2@ 200
'low >0 200 >00 2000 /000 20000 -0000 >0000 0000
Gm
Gi @00 @00 -00 2>00
Gd 0.012 0./@ 0.0@: 0.:=
4egime 6aminar 6aminar 6aminar 6aminar 6aminar Turbulent Turbulent Turbulent Turbulent
: : -.1 :
Total 6(, 2/0 :0 -= 200 /1=
)ressure ,rop" )a Eui9 6 Crane G - *G 0.0=0 0. 0.0:0.0>2 0.2/0 0. 0.0@ 0.20/ 0.>1@ 0. 0.::= 0.>/> 2.21= 0. 0 .1/2 2.0@1 /.-1/ 2. 2 .1=0 /.--2 :2.01 ->.>0@ -@.: /@ /@:.2/1 /> / >.1-: /@.-2> 2 2=./=2 == = =-.12 2>.>/= 2" 2"-/@.1/@ 2" 2 "/:.-02 2"-::./:1
-*G Method total Gf Ex : Ex > VA6?E V VA6?E VA6?E VA6?E VA6?E V VA6?E VA6?E V VA6?E VA6?E VA6?E
?5 Customary Customary ?ni 6iuid 6iuid ?nits Example :a lb(h =-"000.0 psia 202.> c) in ft lb(ft' lb(lbmol
20.0 -.2 -2.> 22/.> 2/.0
ft
0.0002>
- nomina nominall si
Crane ft
Crane G
0.02 0.021/ 1/220.021/ 0.021/220.02 0.021/ 1/220.021/ 0.021/22
/.-2 /.-2 0. 0. 0.=1 0.=1 2.1/ 2.1/ >.=1
VA6? VA6?E E VA6? VA6?E E ,elta )" pipe Velocity f" full full turb turbul ulen ence ce
VA6?E -.00.02 0.02-2: 2:1@ 1@-
6e 10 Ell Branch tee 5wing check )lug 9al9e - x 2 reducer
,elta )" comparison
/ 2 2 2 2
20./>.22 />.> :.=0 @//.=@ @
[email protected]
Crane G -*G 0.=1/>11 VA6?E 0. 0 .-:=- VA6?E 2.-2:1@ VA6?E 0.-22= VA6?E >.1/ >.1/ =2.00 VA6?E VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
2
$roblem Statement: Calculate )ermanent )ressure ,rop Through #rifice =0 m !nputs
6iuid Example = 20"000.0 00.0 2./
[email protected] =0.0 1=2.0
)arameter Mass 'low 4ate )ressure in upsteam$ Viscosity )ipe ,iameter Eui9alent 6ength of )ipe ,ensity Temperature Molecular !eight Cp(C9
?nits kg(h k)a" absolute m)a*s mm m kg(mC kg(kgmol
)ipe 4oughness #rifice ,iameter
m mm
4eynolds 3umber
dimensionless
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
I )/ )-
Expansion factor #rifice discharge pressure )ermanent 6oss
k)a" absolute m(s m(s dimensionless dimensionless r dimensionless k)a" absolute k)a" absolute
VA6?E 20.2
H C
)ressure out downstream$ Velocity through orifice 5onic 9elocity #rifice diameter ratio #rifice Coefficient of ,ischarge
,elta)
)2*)-
k)a
)0
P0
)ipe Jeader at 00 k)a absolute
0.0000:> 21.2
&utput
)2 V2
0.> VA6?E
Stolz equation, Radius Taps
2.0 VA6?E VA6?E VA6?E
4esult G flow coefficient Eui9alent 6ength
dimensionless m
Compare eui9alent length ratio to pressure drop ratio )ipe 6 ( #rifice 6 )ipe )ressure ,rop ( #rifice )ressure ,rop
VA6?E VA6?E
VA6?E VA6?E
Close enough" alt
4#
"
[email protected] mm +,
P2
P1 P3
hough not perfect
$roblem Statement: Calculate )ressure ,rop due to 'riction for !ater*5team !ater*5team Mixture
!nputs
5team*!ater 5team*!ater at 5aturated Conditions Total Mass 'lux kg(m/*s uality Mass 'raction Vapor +nlet )ressure Bar )ipe ,iameter mm Eui9alent 6ength of )ipe m )ipe 4oughness m
Calculations ' $roperty (oo)up )arameter Cross*sectional area Total Mass 'low 4ate +nlet )ressure Temperature Viscosity Molecular !eight ,ensity Cp(C9
?nits m/ kg(h k)a C m)a*s kg(kgmol kg(m-
!ater 2"->=.0 0.> 2.02 >.0 2.0 0.000002> 5mooth Tube Tube & 0.000002> m
Total as 6i Vapor )rops 0.000021=-> 1>.@ 202.0 1.: 0./@ 0.02/
[email protected] 11@. 0.= 2.-2
Mixture
0.0/2./
&utput
20000
2000
4eynolds 3umber
dimensionless
VA6?E
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
VA6?E
)ressure ,rop" gi9en Mass 'low and )ressure in
VA6?E
VA6?E
6iuid ), Multiplier
p hi phiF/
VA6?E VA6?E
)ressure ,rop" /*)hase 'low
k)A
VA6?E
2.02 Bar =.@1 Bar -:.: Bar
[email protected] Bar 20- Bar
200
2-@ Bar 2/ Bar /0 Bar //2./ Ba r
20
2 0
0.2
0 ./
0.-
0.:
0.>
0 .=
0.
0.@
0.1
2
/>0
/00
2>0
7&-1
7&2>=
200
>0
0 0
0.2
0./
0.-
0.:
0.>
0.=
0.
0.@
0.1
2
/>
/0
2>
Awad Dansse n
20
>
0 0
0.2
0./
Property Correlations
0.-
0.:
0.>
0.=
0.
0.@
0.1
2
for all correlations" t & deg C Vapor )ressureK logmm Jg$ & A * B ( tLC$
A 42/ 4// !ater
=.11 .0: @.-2
B
[email protected] @>0.20 2"1@=.>0
C />-.-@ /:>.2@ /=@.:
4efe 4efere renc nceK eK
+)C/ +)C/00 00:* :*/ /2 2
$
Comparison Case 42/ /"000.0 0.1 =.00 >0.0 2.0 0.000002> 5mooth Tube & 0.000002> m$
Total as 6i Vapor )rops 0.0021=-:1>: 2:"2-./ =00.0 //.0 0./0 0.022/0.1 2"-/>./1.= 2.2
?ser in input puts a Temperature" correlation p worksheet$. assume assumed d tha the pressure. Calculations subrou subroutin tines es * subroutines
Mixture
Clicking on t macro that ru ru inputs" based +t seems like for 'igure once" then re recomputing
0.02> -/.@
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E VA6?E VA6?E VA6?E
)hiF/ uality 0 0.00.00.0> 0.0> 0.0@ 0.22 0.22 0.2> 0./ 0./ 0.0.-
2.02 2 :=.:2 :=.:2=:> =:>/1 /12 2 -.--.--//@ //@ 02 02 222.2@::/@: /@: 2:.2@>2 2:.2@>21>01>021-.:0/:/:1./:1.-=>/ =>/>/ >/@> @> ->. ->.=00 =002@ 2@>= >=
0.= 0.= =0.@ =0.@2: 2:/0 /0:> :> 0.@ 0.@ @>./ @>./::2 ::2>= >=-> -> 2 20@.0@1=0>
)hiF/ uality 0 0.2 0.2 0./ 0./ 0.0.0.: 0.: 0.> 0.> 0.= 0.= 0. 0.@ 0.@ 0.1 0.1 2
--1 2 /2.=> /2.=>-:/ -:/>0 >01> 1>
[email protected]@
[email protected]@>0= >0=1: 1:@@ @@ >-.=1 >-.=1- -/@ /@/> /> =@./=@./-@-= @-=== ===/ =/ @/./@ @/./@>:: >::@0 @0/2 /2 1>.1@ 1>.1@=2/ =2/1 10 0 201 201.:/1/@0> @0> 2//.= 2//.=-0 -02@ 2@01 01 2->. 2->.>= >=0 0-> -> 2:@. 2:@.2/2 2/2@> @>/> />
)hiF/ uality 0 0.2 0.2 0./ 0./ 0.0.0.: 0.: 0.> 0.> 0.= 0. 0. 0.@ 0.@ 0.1 0.1 2
//@ 2 -.// -.//>02 >021> 1>=>> =>> >.->.--==/ ==/>2 >2/= /= .-@ .-@==0 ==0-/ -/@-: @-: 1.-1 1.-1@-= @-=0@ 0@1>1 1>1 22.-@: 2.-@:-= -==-= =-=2 2 2-. 2-.->2 ->211=21 =21 2>.-0 2>.-0>1: >1:: :0> 0> 2./: 2./:1- 1-@1 @1>/ >/ 21.2@ 21.2@:>0 :>0-1 1 /2.2 /2.22/1 2/1:2 :2=2 =2
6iuid ViscosityK lnc)$ & A L B ( CLt$
A @.$ @. $ /0.1 /0. 1 :.-: :.:
B >"2-:.>"2-:. :="2:-. :=" 2:-.> > ="1/. ="1 /.-/ -/
Vapor ViscosityK lnc)$ & A L B ( CLt$
C =1-.02 =1.02 /"0=:. /" 0=:.@1$ @1$ 2"--/. 2" --/.--$ --$
1.00$ 1.00$ -.:$ -. :$ :.1/$ :. 1/$
:"=22.@ :"=2 2.@=$ =$ /@. / @.:$ :$ /00.: /0 0.:1$ 1$
2"00@.@ 2"00@ .@$$ /@=.== /@=.== >0/.> >0 /.>$ $
re in 4E, " 9iscosity" and density are determined from rameters in lookup table down at the bottom of the hese are affected by the inlet pressure 9ariable. +t is t the temperature is the saturation temperature at . for 4e" f" and pressure drop a re performed in VBA * other worksheets in this workbook 9erify that those re correct. e 4e*4un All +nputs button at cell 6-> runs a ns the calculation on 9arious combinations of on the charts in +)C/00:*/2. the only way to get a straight line per the reference$ 4ow 2/-$ is to do the friction factor calculations calculate phi for a range of ualities 0 to 2$ without the mixture 9iscosity and density for each uality.
=.@1 2 @.//:=/@=@ @=@2: 2/.=:@-:1/ :1/21
[email protected]@0>1/ >1/2/ /:.1>/2=>=>-@1 -/.=@@@1->@/ :/.0 :/.0> >= =:/ :/-1 -1 =0.2@=0/2= /2=22
-:.: 2 /.:@22@1>/: -.:/--0= -0==1 :.@@0 @0@0@ =.20@-/@ -/@@-.@2@>>2 1.@1 1.@11 11> 1>//-= = 2-.1 -.1/=>=>-2=1
[email protected] 2 2./: /:/01 /.21-2 /.@1 @1@/> -.>>0 >>0/1= :.:/:2@= >.:1 >.:122--: -: .>=> >=>::>
202 2.: 2.:2/ 2/1-=-=2. 2.1: 1:2@/1 /1 /./ /./--@ --@:@10@ 10@ /.=@0/-2 -2: -./=>0:01:: -.1@ -.1@/2 /201 01>2 >2= = >.>.-@0@ @0@/->= ->=
2-@ 2 2.2.-:2/2 2/2:==/ 2.> 2.>=>> >>-0>: 2.@ 2.@1@=/ @=/:2/2 /.// ///>0/@ 0/@ /.=>1=02@/: -.21 -.2121 21-= -=2/ 2/2 2 :./-: /-:=2@:> @:>
2/ 2 2./=> /=>:-==: ==: 2.::0 ::010:>> :>> 2.0/ 0/0-:>= :>= 2.1=0 1=0@>--@ --@ /.-0/=>/./ /./>2 >2/0 /02 22 -.>>= >>=--0@/ 0@/
/0 2 2./2--@22 @22@ 2.->: ->:1-1-@ 1-@2 2.>== >==/@>@ @>@1 2.= =:2>/ 2>/= /.0>>0-@1> /.:0 /.:00= 0=1 1>@ >@ -.0@: 0@:/@>0 >0
//2./ 2 2.2 2.21=1: =1:: 2.2.-/> >> 2.> 2.>/-/ /-/ 2. 2.21 12 2.1=->> /./1 /./1: :/ / /.1 /.1--1: -1:2
22/.2/.- 02 02@@ @@2 2 />. />.:1-:1--1: 1:-= -= 2-.> 2-.>/2 /21@ 1@ 1.:0 1.:0>2 >2>: >:1 1@ @ ./: ./:>2 >2@@ @@@1 @1: : >.1= >.1=1/ 1/-= -=:1 :1 >.0@ >.0@:= :=1= 1=> >: : :.@0 :.@0:2 :2=1 =1 2:=. 2:=.- -2 22/> 2/>/ / -/. -/.11@> 11@>@ @@/ @/ 2.2.- = = 2/. 2/.00== 00==>> >>0= 0= 1.21 1.2120 20// //=2 =2: : .>.>-22-22-1 1 =.-@ =.-@> >> >@/ @/2 2 =.0/ =.0/::-@1 @1 2@0.
[email protected]= 0=21 210 0:2 :2 :0. :0.:/0@ :/0@-1 -12/ 2/ /2.2 /2.2@@-= = 2:. 2:.>0= >0==/ =/@: @: 22.20 2.20==-22->= >= 1.0= 1.0=1 11> 1>-: -: .== .==0 0>1 >1/2 /2 .// .//> >1 1
5onic Velocity
U
max
2->= 2 //.12=:>22> :/.0>=:/-1 =0.2@=0/2=22 .@->-@2-@ 1>.211@=/=>: 22/.-02@@2 2/1.://>>@-1 2:=.-22/>/ 2=-./:>=->/>
[email protected]=210:2
>:/: Mass 'lux , ,e ensity 2 11@.== /:.>//2:-@= >.@ :=.:21/10:= /.1: =.@=:0/-2@ 2.1= @1.20211: 2.: 220./-110=2 2.2@ 2-2.-0:/=// 0.1@ 2>/.-//@0.@: 2-.-0@:> 0.: 21:./0>>:1 0.== /2>./2-@-0.>1
=
√
Z γ R T M
)ipe flow area Velocity" m(s --1 0.-: >.> 22>.2 2/.>@ /-0.00 /@.:2 -::.@:0/./: :>1.== >2.0 >:.:@
:@1.:1 :@1.:1@// @// m(s
0.000021=-> m/ 2->= 2.-= //-2.0/ :=0.= =10.-121.11 2"2:1.=> 2"-1.-0 2"
[email protected]= 2"@-@.=/ /"0=@./@ /"/1.1:
>:/: kg(m/*s >.:1/:.0= IE66#! 2"@:/.=1 4E, N Ma /"=2.--"=1.1= :">1@.>1 >">2.// =":->.@> "->:.:@ @"/-.22 1"212.:
Mass 'lux 2 >.> @ 1.> 22.>
,ensityK kg(m- & m t L b
m -.01$ -.0 1$ -./ ./0$ 0$ 2.> 2 .>=$ =$
b 2"-12" -1-.: .:0 0 2"/1 2" /1..-2"2>0 2" 2>0.: .:/ /
,ensityK lb(ft- & m t L b
m 0.2 0 .21$ 1$ 0./ 0 ./0$ 0$ 0.0 0 .0=$ =$
b @=.11 @=.11 1.@ 1. @ =:./: =:. /:
Molecular !eight 2/0.1 2/0 .12 2 @=.:@ @=. :@
[email protected] 2@. 00
Cp(C9 2.20 2.20 2./>0 2. />0 2.-20 2. -20
N Mach 0.h2
$roblem Statement: Calculate )ressure ,rop due to 'riction for 42/ at 5aturation
!nputs
5team*!ater 5team*!ater at 5aturated Conditions Total Mass 'lux kg(m/*s uality Mass 'raction Vapor +nlet )ressure Bar )ipe ,iameter mm Eui9alent 6ength of )ipe m )ipe 4oughness m
Calculations ' $roperty (oo)up )arameter ?nits Cross*sectional area m/ Total Mass 'low 4ate kg(h +nlet )ressure k)a Temperature C Viscosity m)a*s Molecular !eight kg(kgmol ,ensity kg(mCp(C9 Velocity assuming a9g density$ m(s Critical Velocity m(s &utput 4eynolds 3umber dimensionless ,arcy 'riction 'actor
dimensionless
)ressure ,rop" gi9en Mass 'low and )ressure in 6ower Bound ?pper Bound A9erage . m ' a $ + t n e i d a r g e r u s s e r p l a n o i t c i r f
200"000
20"000
42/ 200.0 0.> 1.:0 20.0 2.0 0.000002> 5mooth Tube Tube & 0.000002> m
6iuid .@>-1@/E*0> 2:.2 1:0.0 -1./ 0.2 2/0.1 2"//.>
2:.2 1:0.0 -1.2= 0.02: 2/0.1 :-.@ 2.2 2.2@ 2>@.0
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
0.20.-: k)a & )a
Vapor
0.//-2.@-
2"000
200
20
2 20
2 00
mass flu* +)g'm,-s.
2000
4efe 4efere renc nceK eK +MEC +MECE/ E/00 00>* >*@2 @2:1 :1-
$
Comparison Case 42/ /"000.0 0.1 =.00 >0.0 2.0 0.000002> 5mooth Tube & 0.000002> m$
6iuid 0.0021=-:1>: 2":2-. =00.0 //.0 0./0 2/0.1 2"-/>.-
Vapor 2/"/-.> =00.0 //.0> 0.022/0.1 /1.= 2.-2 =2.0> 2=-./=
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
.= 2/.1: 20.-0
uality
0.>
Mass Mass 'lu 'lux x 6ower 6ower /0 @ @0 @= /00 :/> :00 2": 2":-2 =00 /"1 /"101 2000 2000 "2 "22/
5onic
A9erage 2: 2> @0 /"=/>"--2-"0-
?pper
2>@.02=
,ensity Velocity Velocity"" m(s /0 @:.= @:.=/ / 0./0./-==-/1 /1 //@ 0.1:>-2 2"2-: /.-=-/1/ -"@2> :./=>@> ">= .0@1@ 2@"1=/ 22.@2=:=
$roblem Statement: Calculate )ressure ,rop due to 'riction for 42/ at 5aturation
!nputs
5team*!ater 5team*!ater at 5aturated Conditions Total Mass 'lux kg(m/*s uality Mass 'raction Vapor +nlet )ressure Bar )ipe ,iameter mm Eui9alent 6ength of )ipe m )ipe 4oughness m
Calculations ' $roperty (oo)up )arameter Cross*sectional area Total Mass 'low 4ate +nlet )ressure Temperature Viscosity Molecular !eight ,ensity Cp(C9
?nits m/ kg(h k)a C m)a*s kg(kgmol kg(m-
42/ 200.0 0.> 1.:0 20.0 2.0 0.000002> 5mooth Tube Tube & 0.000002> m
6iuid .@>-1@/E*0> 2:.2 1:0.0 -1./ 0.2 2/0.1 2"//.>
Vapor
2:.2 1:0.0 -1.2= 0.02: 2/0.1 :-.@ 2.2
&utput 4eynolds 3umber
dimensionless
VA6?E
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
VA6?E
)ressure ,rop" gi9en Mass 'low and )ressure in
VA6?E
VA6?E
dp(d<
)a(m
VA6?E
VA6?E
'itting parameter
p
Total pressure drop
k)a(m
0.@ VA6?E
4efe 4efere renc nceK eK +MEC +MECE/ E/00 00:* :*=2 =2:2 :20 0
$
Comparison Case 42/ /"000.0 0.1 =.00 >0.0 2.0 0.000002> 5mooth Tube & 0.000002> m$
6iuid 0.0021=-:1>: 2":2-. =00.0 //.0 0./0 2/0.1 2"-/>.-
k)a(m
Vapor 2/"/-.> =00.0 //.0> 0.022/0.1 /1.= 2.-2
water 4eference article" 'igure !ater*Air >12.0 0.0-> 2.-0 /.0 2.0 0.000002> 5mooth Tu
6iuid 0.000>/>= 2"21.= 2-0.0 /0.0 0.-1
[email protected] 2"221.2"221.-
Vapor /0.= 2-0.0 /0.00 0.0/0 /1.0 2.>> 2.:0
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
0.- This method depends on fitting parameter" p VA6?E
0./> This metho VA6?E VA6?E
2
be & 0.000002> m$
depends on fitting parameter" parameter" p
$roblem Statement: Calculate )ressure ,rop due to 'riction for !ater*5team !ater*5team Mixture
!nputs
5team*!ater 5team*!ater at 5aturated Conditions Total Mass 'lux kg(m/*s uality Mass 'raction Vapor +nlet )ressure Bar )ipe ,iameter mm Eui9alent 6ength of )ipe m )ipe 4oughness m
Calculations ' $roperty (oo)up )arameter Cross*sectional area Total Mass 'low 4ate +nlet )ressure Temperature Viscosity Molecular !eight ,ensity Cp(C9
?nits m/ kg(h k)a C m)a*s kg(kgmol kg(m-
water 220.= 0.2 2:.@
[email protected] -0.> 0.0000:>
6iuid 0.0022:0012@ -1/. 2":@/.@ 21. 0.2
[email protected] @:/.:
Vapor
=2.2":@/.@ 21.0 0.02:
[email protected] =. = .@ 2.:0
&utput 4eynolds 3umber
dimensionless
VA6?E
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
VA6?E
)ressure ,rop" gi9en Mass 'low and )ressure in
VA6?E
VA6?E
6ockhart and Martinelli Method O dimensionless )hi*liuid dimensionless
VA6?E VA6?E
Total )ressure ,rop" /*phase
m r e p a $ ) , p 0.20 o r %
k)a psi(200 ft
VA6?E VA6?E BrananK 0.:1 psi(200 ft 4ukanK 0./@ psi(200 ft
Comparison of o f Two-$hase Two-$hase /odels R1 R1, 0 ar pressure, 122 )g'm-s in 52 mm s
r . u s s e r 0.0@ $
0.0 0.0= 0.0> 0.0: 0.00.0/ 0.02 * 0
0.2
0./
m r e p a $ ) , p 2=0 o r % e r u 2:0 s s e r $
0.-
0.:
0.> 3uality
0.=
0.
0.@
Comparison of Two-$hase Two-$hase /odels R1, 0 ar ar pressure, 5222 )g'm-s in 52 mm mm s
2/0 200 @0 =0 :0 /0 * 0
0.2
0./
0.-
0.:
0.> 3uality
0.=
0.
0.@
4efere 4eference nceKK Branan Branan"" 4ules 4ules of Thum Thumb" b" :th Edit Edition ion
Comparison Case 42/ /"000.0 0.1 =.00 >0.0 2.0 0.000002>
6iuid 0.0021=-:1>: 2":2-. =00.0 //.0 0./0 2/0.1 2"-/>.-
Vapor 2/"/-.> =00.0 //.0> 0.022/0.1 /1.= 2.-2
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E
VA6?E VA6?E VA6?E
ooth pipe
!allis
)hiF/" lo )hi" lo
/0.@1-0>2 :.>0@12 VA6?E
/ass Flu* 3u 3uality 4elocity omog Split 200 0 0.0> 0. 0.00 200 0.2 0.:0= 0.02 200 0./ 0.- 0.02 200 0.2.0=@ 0.0/ 200 0.: 2.-11 0.0/ 200 0.> 2./1 0.0200 0.= /.0=0 0.0-
0.00 0.02 0.0/ 0.00.00.0: 0.0>
Jomogeneou s 5plit Asymptotic Asymptotic 6ockhart
0.1
2
ooth pipe
Jomogeneou s 5plit Asymptotic Asymptotic 6ockhart
0.1
2
200 200 200 200 20 >0 200 /00 -00 :00 >00 =00 00 @00 2000 2000 2000 2000 2000 2000 2000 2000 2000 2000 2000 2000 /000 /000 /000 /000 /000 /000 /000 /000 /000 /000 /000 >000 >000 >000 >000 >000 >000 >000 >000 >000 >000 >000
0. 0.@ 0.1 2 0.> 0.> 0.> 0.> 0.> 0.> 0.> 0.> 0.> 0.> 0.> 0 0.2 0./ 0.0.: 0.> 0.= 0. 0.@ 0.1 2 0 0.2 0./ 0.0.: 0.> 0.= 0. 0.@ 0.1 2 0 0.2 0./ 0.0.: 0.> 0.= 0. 0.@ 0.1 2
/.-12 /.// -.0>/
[email protected]>1 0.1> 2.>10 -.21 :.=1 =.->1 .1:@ 1.>-@ 22.2/@ 2/ 2/.2 2>.@1 0.>> :.0=/ .-0 20.=@ 2-.1@= 2./1: /0.=02 /-.101 /./2 -0.>/> --.@-2.>01 @.2/> 2:.:0 /2.->= /.1/ -:.>@ :2./0:.@2@ >:.:-: =2.0>0 =.==> -./0.-2/ -=.@>2 >-.-10 =1.1/1 @=.:=@ 20-.00 221.>:= 2-=.0@> 2>/.=/: 2=1.2=-
0.0: 0.0: 0.0: 0.0> 0. 0.000. 0.0>2 0. 0.2= 0. 0.=22. 2./@> /. /.2@: -. -.-0: :. :.=:2 =.21: .1=2 2/ 2/.2-0 2 2 2 / / / : 0 / > = 1 20 22 22: / 22 21 /@ -= :: >/ =0 =@ =
0.0> 0.0> 0.0> 0. 0.00> 0. 0.0@: 0. 0./@: 0. 0.1>: 2. 2.1:0 -. -./01 :. :.:/ =. =.>/: @.>:> 20.1: 2> 2 >.1>2 0 2 2 / / / 0 / : > = @ 1 20 20 20 / 22 2@ /> -/ -@ ::@ >2 >2
symp 0.02 0.0/ 0.00.00.0: 0.0>
(oc)hart 0.0/ 0.00.0: 0.0> 0.0= 0.0
Fluid 42/ 42/ 42/ 42/ 42/ 42/ 42/
!nlet $res $ipe %iam E6ui7alen $i $ipe Roughne =.00 >0.0 2.0 0.000002> =.00 >0.0 2.0 0.000002> =.00 >0.0 2.0 0.000002> =.00 >0.0 2.0 0.000002> =.00 >0.0 2.0 0.000002> =.00 >0.0 2.0 0.000002> =.00 >0.0 2.0 0.000002>
0.0> 0.0= 0.0=
0.0@ 0.01 0.0@
0.00 0.0= 0.// 0.1:0 2.1:> -./:.12=.@>1 1.20> 22.=:@ 2.=2-
0.022 0.2/: 0.::2.>/ -.2> >.-22 .1=1 22.2/2:.=/ 2@.@@/ /@.>:/
2 2 / / : : :
2 / : : > = = =
/ : = @ 20 2/ 2: 2> 2=
: 20 22= 21 // /: /:
2: /: -> := >@ =1 1 @@ 1:
/> :2 >@ = 1222 2/= 2-@ 2:2
42/ 42/ 42/ 42/ 4// 4// 4// 4// 4// 4// 4// 4// 4// 4// 4// 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/ 42/
=.00 =.00 =.00 =.00 1.20 1.20 1.20 1.20 1.20 1.20 1.20 1.20 1.20 1.20 1.20 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00 =.00
>0.0 >0.0 >0.0 >0.0 20.0 20.0 20.0 20.0 20.0 20.0 20.0 20.0 20.0 20.0 20.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0 >0.0
2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0
0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002> 0.000002>
ss
Jashi
0.: />0 2
m r e p a $ ) , p o r % e r u s s e r $ l a n o i t c i r F
R1, 0 ar C
=
>
:
-
/
2
*
0
m r e p a $ ) , 200.000 p o r % e r u s s 20.000 e
0.2
0./
0.-
0.
R, 891
$
2.000
0.200
0.020
0.002
20
Comparison of Two-$hase /odels ressure, ressure , 1222 )g'm-s in 52 mm smooth pipe pipe
0.> 3uality
0.=
0.C
0.@
0.1
Comparison Comparis on of Two-$hase /odels r pressure, 295 3uality 3uality in 12 mm smooth tube
200 ass Flu*, )g'm-s
2000
6ockhart Asymptotic Asymptotic 5plit Jomogeneou s
2
6ockhart Asymptotic Asymptotic 5plit Jomogenous Jashi
$roblem Statement: Calculate )ressure ,rop Through an Elbow for ,ifferent 5team ualities
!nputs
5team*!ater 5team*!ater at 5aturated Conditions Total Mass 'lux kg(m/*s uality Mass 'raction Vapor +nlet )ressure Bar )ipe ,iameter mm Eui9alent 6ength of )ipe m )ipe 4oughness m
Calculations ' $roperty (oo)up )arameter Cross*sectional area Total Mass 'low 4ate +nlet )ressure Temperature Viscosity Molecular !eight ,ensity Cp(C9
?nits m/ kg(h k)a C m)a*s kg(kgmol kg(m-
!ater 2"->=.0 0.2 =.00 >0.0 2.0 0.000002> 5mooth Tube Tube & 0.000002> m
Total as 6i Vapor )rops 0.0021=-:1>: 1">@>.0 =00.0 2>@.0./2 [email protected] 10-. -.0
Mixture
0.0@: /1./
&utput 4eynolds 3umber
dimensionless
VA6?E
VA6?E
,arcy 'riction 'actor
dimensionless
VA6?E
VA6?E
)ressure ,rop" gi9en Mass 'low and )ressure in
VA6?E
6iuid ), Multiplier
p hi phiF/
VA6?E VA6?E
)ressure ,rop" /*)hase 'low
k)A
VA6?E
5onic Velocity
U
max
uality 0 0.02 0.02
=
√
Z γ R T M
:>.=
)ipe flow area 0.0021=-:1> Velocity" m(s ,ensity >:/: kg(m/*s 10-. 10-.> > =.00 =.00 //=.:0 //=.:0 /-.1= /-.1= IE66#! IE66#! & N Mach Mach 0.-
0.0/ 0.0/ 0.00.00.0: 0.0: 0.0> 0.0> 0.0= 0.0= 0.0 0.0 0.0@ 0.0@ 0.01 0.01 0.2 0.2 0.2 0.22 0.2/ 0.2/ 0.20.20.2: 0.2: 0.2> 0.2> 0.2= 0.2= 0.2 0.2 0.2@ 0.2@ 0.21 0.21 0./ 0./ 0./2 0./2 0.// 0.// 0./0./0./: 0./: 0./> 0./> 0./= 0./= 0./ 0./ 0./@ 0./@ 0./1 0./1 0.0.0.-2 0.-2 0.-/ 0.-/ 0.-0.--
2/1.:2 2/1.:2 10.= 10.=0 0 =1.= =1.=1 1 >=.= >=.=:.= :.=1 1 :2.2 :2.21 1 -=./ -=./: : -/.-/.-= = /1./ /1.//=.= /=.=> > /:.: /:.:1 1 //.= //.=> > /2.0 /2.0 21. 21.0 0 2@.: 2@.:1 1 2.: 2.:2=.: 2=.:@ @ 2>.= 2>.=/ / 2:.@ 2:.@= = 2:.2 2:.2= = 2-.> 2-.>2/.1 2/.1> > 2/.: 2/.:2 2 22.1/ 2.1/ 22.: 2.: 22.0> 2.0> 20.= 20.== = 20.20.-0 0 1.1= 1.1= 1.=: 1.=: 1.-: 1.-: 1.0= 1.0=
:2.12 :2.12 4E, 4E, N Mach Mach 2 >1.@ >1.@ .@.@1>.@ 1>.@ 22-.: 2-.: 2-2.= 2-2.=1 1 2:1.= 2:1.=> > 2=.= 2=.=2 2 2@>.> 2@>.>= = /0-.> /0-.>/ / //2.: //2.: /-1.: /-1.:/>./>.-1 1 />./>.-: : /1-./1-.-0 0 -22. -22./> /> -/1./ -/1./2 2 -:.2 -:.2 -=>.2 -=>.2/ / [email protected] [email protected]@ @ :02.0 :02.0:[email protected] :[email protected] 1 :-=.1 :-=.1> > :>:.10 :>:.10 :/.@= :/.@= :10.@2 :10.@2 >0@. >0@. >/=. >/=.>::. >::.=@ =@ >=/.= >=/.=: : >@0.> >@0.>1 1 >1@.> >1@.>> >
Property Correlations
for all correlations" t & deg C Vapor )ressureK logmm Jg$ & A * B ( tLC$
A 42/ 4// !ater
=.11 .0: @.-2
B [email protected] @>0.20 2"1@=.>0
C />-.-@ /:>.2@ /=@.:
$
Gm @00
m(s
m/
G
VA6? VA6?E E k)a VA6?E
Gi 0.012
VA6?E elbow
Gd :
VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E VA6?E
2/.00
20.00
@.00
=.00
:.00
/.00
*0.2
* */.>>>>=2>=/@1E*2
0.2
6iuid ViscosityK lnc)$ & A L B ( CLt$
A @.$ @. $ /0.1 /0. 1 :.-: :.:
B >"2-:.>"2-:. :="2:-. :=" 2:-.> > ="1/. ="1 /.-/ -/
Vapor ViscosityK lnc)$ & A L B ( CLt$
C =1-.02 =1.02 /"0=:. /" 0=:.@1$ @1$ 2"--/. 2" --/.--$ --$
1.00$ 1.00$ -.:$ -. :$ :.1/$ :. 1/$
:"=22.@ :"=2 2.@=$ =$ /@. / @.:$ :$ /00.: /0 0.:1$ 1$
2"00@.@ 2"00@ .@$$ /@=.== /@=.== >0/.> >0 /.>$ $
0./
0.-
,ensityK kg(m- & m t L b
m -.01$ -.0 1$ -./ ./0$ 0$ 2.> 2 .>=$ =$
b 2"-12" -1-.: .:0 0 2"/1 2" /1..-2"2>0 2" 2>0.: .:/ /
,ensityK lb(ft- & m t L b
m 0.2 0 .21$ 1$ 0./ 0 ./0$ 0$ 0.0 0 .0=$ =$
b @=.11 @=.11 1.@ 1. @ =:./: =:. /:
Molecular !eight 2/0.1 2/0 .12 2 @=.:@ @=. :@ [email protected] 2@. 00
Cp(C9 2.20 2.20 2./>0 2. />0
$roblem Statement: Compare the )anhandle and !eymouth formulas with the +sothermal gas calculation
!nputs
5+ ?nits 7as molecular weight Temperature C )ipe diameter mm )ipe length km +nlet pressure k)a abs #utlet pressure k)a abs Ele9ation difference m Efficiency A9erage compressibility compressibility factor
Value
?5 ?nits
2.: -.@ 20/ -/./ 2-"00 20"-00 -0.> 2 2
' in miles psia psia ft
Value
2.: 200 :.0/= /0 /"000 2">00 200 2 2
Constants Base temperature Base pressure )ipe roughness Calculations Isothermal Gas Calculation 4eynolds 3umber 'riction factor 'low 4ate 5tandard 9olumetric rate Intermediate Calcs 7as specific gra9ity A9erage temperature A9erage pressure Jead correction
C k)a abs m
kg(h MM m-(day
G k)a abs k)a
Weymouth 5tandard 9olumetric rate
MM m-(day
Panhandle A 5tandard 9olumetric rate
MM m-(day
Panhandle B 5tandard 9olumetric rate
MM m-(day
* 200 0.0000:>
/00"000 VA6?E VA6?E VA6?E
0.=0 -22 2/"0@0 :1
' psia ft
lb(h MM ft-(day
4 psia psi
=0 2:. 0.0002>
/00"000 VA6?E VA6?E VA6?E
0.=0 >=0 2"=/
MM ft-(day
20"2>2
:0/
MM ft-(day
2>"220
:/@
MM ft-(day
2="0-: