UNCLASSIFIED UNCLASSIFIED DEFENSE DOCUMENTATION CENTER SCIENTIFIC AND TECHNICAL INFORMATION FOR CAMERON STATION, ALEXANDRIA, VIRGINIA
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1 UNCLASSFED AD DEFENSE DOCUMENTATON CENTER FOR SCENTFC AND TECHNCAL NFORMATON CAMERON STATON ALEXANDRA VRGNA / UNCLASSFED
2 NOTCE: When government or other drawlngb specifications or other data are used for any purpose other than in connection with a definitely related government procurement operation the U. S. Government thereby incurs no responsibility nor any obligation whatsoever; and the fact that the Goremment may have fonnulated furnished or in any way supplied the said drawings specifications or other data is not to be regarded by implication or otherwise as in any manner licensing the holder or any other person or corporation or conveying any rights or permission to manufacture use or sell any patented invention that may in any way be related thereto.
3 AEDCTDR63190 ECSSSSSCSö MOLLER DAGRAM FOR AR S D D ; ' ^ ' '«* By A.nr.T T '963 Wanda J. Littie von KaVman Gas Dynamics Dynai Facilitf ARO nc. TECHNCAL DOCUMENTARY REPORT NO. AEDCTiR63190 September 1963 Program Element /8951 Task (Pr.portd und.r Contract No. AF 40(600)1000 by KRO nc.. MMMd «^ rofof of AEDC Arnold Air Fore» Stotitn Tonn) ARNOLD ENGNEERNG DEVELOPMENT CENTER fwn 1 AR FORCE SYSTEMS COMMAND UNTED STATES AR FOtCi
4 g < a M S 3 > O a 35 Ov a = W U Pi % < gs a y od ^ Q < g w 5V^9 ^//^ ^^ nr
5 ' 8 6
6 MOLLER DAGRAM FOR EQ «) 42 SOÜO 0 K ^* K l30oo o K "K K
7 1 FOK EQUTTJB Rii > JM AR 14 rn 1 {n t > 1 ^^5 ^^ iz^zz^^z^z^zis
8 R i ;!! ; ^ i j i ; : i U i i 1 j i! : : i! : j 1 \: : [: [ii : i i :i \\ : i ' '
9 n
10 :.;.:;: 10^ J i : : HOC \4
11
12
13 l800 o K
14 ^^ 9000 o K ^ ^ /.. 1 ' '. 1 ^.. ^ Ml S/R MOLLER DAGRAM FOR EQULBRU PRK'ARKD»V Ml SAH ()» VON KARMAN <.AS DYNAStK FACLTY. ARO. NC. CONTRACT ()>1 RATORS OF ARSO.D! cnnf.hrnc DKVKl.O'MFN CFNTFR. NnFl) S Al S Al FORCK. ARNOLD AR POKE STATON. TNNFSS1 luntbd f THF. 1'ARTHNON PRvSS. NASHV NN SS 1. MARl H Hj This chart is a composite of sectional parts given hy Wamla. Little " Air'* AEDCTÄ63190September 1963.The ilata tor it are derived «m
15 S/R )AGRAM FOR EQULBRUM AR D BY THK STAFF OF VON KARMAN (ias DYNAMCS ARO NC. CONTRACT Ol'KRATORS OF ARNOLO EH NG DEVELOPMENT CENTER UNTED STATES AR RNOLD AR FORCE STATON TENNESSEE. PRNTED BY LTHENON PRESS NASHVLLE TENNESSEE MARCH 19M. e of sectional parts given by Wanda ]. Little "Mollier Diagram for ^rtrrnwr WM The data for it are derived from Hilsenrath
16 _
17
18 JO # K
19 «QOK 10' 240 o lt 220 o K 260 "K ZOO^K '
20 utiwwnno DFVF.OPMFNT CFNTFR. fntttt 5TATTS ATR FORCE. ARNOLD AR POME STATON. TF.NNKSSF. 'RNTF) BV THE PARTHENON PRESS. NASHVLLE. TENNESSEE. StARCH 1*4. This chart is a composite of sectional parts given hy Wanda. Little. "Mollier \4 Air" AEDCTDR63190 Septemher»63. The data tor it are derived from and M. Klein. "Tables of Thermodynamic Properties ol Air in Chemical Ed eluding Second Virial Corrections from 1500 to 15000%" AEDCTDR and from R. L. Humphrey and C. A. Ned " Tables of Thermodvnamic Air from 90 to 1^00"K; AEDCTR61103 August The latter lahle«. are io 3 on. Hilsenr.uli. C. W. Beckett et al.. Tables oj Thermal Piufirtki of Cue* NovemlKr 1955 and on F. Din Thermodynanin hum lions of Gases. V worths London The tables of Din als.) provide data for the saturation sures above one atmosphere. At pressures below one.umosphere. the approx tion line is basal on C. T. Furukawa and R. E. McCoskey. "The Condensatior and the Heats of Vaporization of Oxygen and Nitrogen." XHSTeehiiKa! Rep gust and on W. 1). Krickson and 11. E. Creekmore. "Suulv d EqidKbrij Effects in Hvpersonic Air Nozzles ncluding Charts ol ThermcHlynamic Propc. librium Air" \ASATNi)231. April 19((). The vertical coordinate is the enthalpv luikiion 1 l/r expressed in urn Kelvin. ts values are obtained by multiplving the dunensionless luiuiion 1 temperature. The horizontal COOfdlMtr is the dmunsionless emfop) luneti. temperature T ts measured in degrees Kelvin. The pressure p is given m aim. the density p in unagat units based on the densitv ot.ur at (V'C and a pressure. phere. The logarithms are common logarithms to base ten. For air one amagat is the equivalent of "' grams per cubic eentmul pounds per cubic foot. Enthalpy in calories per gram is equal to /R( K) i and in British thermal units per pound it is equal to 1 l/r( K ) multipl«the specific enthalpy in fectsquared per secondsquared is equal to H/R("K by and in meterssquared per secondsquared to H/R("K) multiphe«t8 10 2
21 GNEERNG DEVELOPMENT CENTER. UNTED STATES AR FORCE ARNOLD AR FORCE STATON. TENNESSEE. PRNTED BY THE PARTHENON PRESS. NASHVLLE. TENNESSEE. MARCH 9M. This chart is a composite of sectional parts given by Wanda. Little "Mollier Diagram for Air" AE1X rdr63190 September The data for it are derived from. Hilsenrath and M. KU""Tables of Thcrmodynamic Properties of Air in Chemical Kquilibrium ncluding Second Virial Corrections from 1500 to 15000"K" AEDCTDR63161 August 1963 and fn m R. L. Humphrey and C. A. Neel "Tables of Thermodynamic Properties of Air from 90 Ml 500 K" AEDCTR61103 August The latter tables are based mainly on ]. HilseiH ith C. W. Beckett et al.. Tables of Thermal Properties of Gases. NBS Circular 564 November 1955 and on F. Din Thernioclynamic Functions of Clases Vol. 2 Butterworths. London The tables of Din also provide data for the saturation line at pressures above one atmosphere. At pressures below one atmosphere the approximate saturation Jint is based on C. T. Furukawa and R. F. McCoskey "The Condensation Line of Air and the 1 leats of Vaporization of Oxygen and Nitrogen" NBS Technical Report 1775 August 1952 and on W. D. Frickson and H. F. Creekmore "Study of Equfllbriuni RealGas Effects in llvpersonic Air Nozzles ncluding Charts of Thermodynamic Properties ot Fcjuilibrium Air" NASATND231 April The vertical coordinate is the enthalpy function ll/r expressed in units of degrees Kelvin. ts values arc obtained by multiplying the dimensionless function 1 l/rt bv the temperature. The horizontal coordinate is the dimensionless entropy tunction S/R. The temperature is measured in degrees Kelvin. The pressure p is given in atmospheres and the density p in amagat units based on the density of air at 0"C and a pressure of one atmosphere. The logarithms are common logarithms to base ten. For air on» amagat is the equivalent of grams per cubic centimeter or pounds per t; )ic foot. Enthalpy in calories per gram is equal to H/R("K) multiplied by and in British thermal units per pound it is equal to H/R("K) multiplied by The specific. ithalpy in feetsquared per secondsquared is equal to H/R("K) multiplied by and in meterssquared per secondsquared to H/R("K) multiplied by
22 AEDCTDR63l90 MOLLER DAGRAM FOR AR By Wanda J. Little von Karman Gas Dynamics facility ARD nc. TECHNCAL DOCUMENTARY REPORT NO. AEDC.. TDR September 1963 Program Element /8951 Task (Prepared under Contract No. AF 40(600).1000 by ARO nc. contract operator of AEDC Arnold Air Force Station Tenn.) ARNOLD ENGNEERNG DEVELOPMENT CENTER AR FORCE SYSTEMS COMMAND UNTED STATES AR FORC AF 40(600)1000
23 AEDC. TDR ABSTRACT A Mollier diagram for air including the effects of dissociation and ionization as well as of intermolecular potentials to the second virial correction. is presented. The range of temperatures extends from the saturation line to 15 OOooK and the range of densities from 10 7 to approximately 200 amagats. PUBLCATON REVEW This report has been reviewed and publication is approved.. ;9$T L D. Fit{{erld Capt USAF Aerospace Sciences Division DCS/Research USj al} R. Eastman Jrr" DCS/Research. ii
24 A EDC. TDR COl'nEHTS ABSTRACT... NOMENCLA TURE NTRODUCTON. REFERENCES. APPENDX... Page ii iv LLUSTRATOHS Figure 1. ndex Sheet. 233 Air Mollier Diagram iii
25 NOMENCLATURE H/R log P R S/R T p/po Enthalpy in ok obtained by multiplying the dimensionless function H/RT by the temperature in ok Common logarithm to base 10 Pressure atm Gas constant Entropy dimensionless Temperature ok Density in amagats based on Po at O C and one atm of pressure iv
26 AEDCTDR=63= NTRODUCTON This air Mollier diagram was prepared for the purposes.of data reduction in the operation of wind tunnels at the Arnold Engineering Development Center (AEDC) Air Force Systems Command (AFSC) USAF. This diagram represents the most recently available information on the thermodynamic properties of air. including the effects of dissociation ionization and of intermolecular potentials to the second virial correction. The diagram covers the range of temperatures from the saturation line to 15 OOooK and the range of densities from 10 7 to from 200 to 250 amagats. Above 1500 o K the plotted data are taken from the tables of Hilsenrath and Klein (Ref. 1) whereas the data below K are derived from the tables of Humphrey and Neel (Ref. 2) which combine information from various sources notably the tabls of Din (Ref. 3). Data below 90 o K as well as all data at densities below 107 amagat were generated mainly by extrapolation using the method described in Ref. 4. The tables of Din (Ref. 3) provide explicit data for the saturation line at pressures from one atmosphere upwards. At pressures below one atmosphere the saturation line is based on the work of Furukawa and McCoskey (Ref. 5) and of Erickson. and Creekmore (Ref. 6) the latter being based on vaporpressure data for pure nitrogen and oxygen. Enthalpy expressed as H/R having dimensions of degrees Kelvin is plotted vertically on a logarithmic scale through four decimal orders of magnitude. The dimensionless entropy S /R is the other basic variable. Lines at constant density are identified by their values of log P / Po' in which the ratio p / Po is the density in amagats. The constant pressure lines are marked in atmospheres and the constant temperature in degrees Kelvin. The appendix contains a short list of useful conversion factors. REFERENCES 1. Hilsenrath J. and Klein M. "Tables of Equilibrium Properties of Air ncluding Second Virial Corrections. AEDCTDR September Humphrey R. L. and Neel C. A. "Tables of the Thermodynamic Properties of Air from 90 to 1500 o K." AEDCTN61103 August Manuscript received August
27 AEDC.TDR Din F. Thermodynamic Functions of Gas es. Vol. 1 Butterworths Scientific Publications London Humphrey R. L. Little W. J. and Seely L. A. "Mollier Diagram for Nitrogen. 11 AEDCTN6083 May Furukawa G. T. and McCoskey R. E. l1the Condensation Line of Air and the Heats of Vaporization of Oxygen arid Nitrogen. 11 National Bureau of Standards Technical Report August Erickson W. D. and Crekmore H. S. l1a Study of Equilibrium RealGas Effects in Hypersonic Air Nozzles ncluding Charts of Thermodynamic Properties of Equilibrium Air." NASA TN D231 April
28 APPENDX Conversion Factors To Change To With Units of Multiply by H H 1 None R RT T (OK) H R or 1.8 H S S R ft2 sec2 Btu lb cal gm ft2 sec2 K ft 2 sec2 R Btu lbor Btu lbok cal gmok ( 10) (10) (10) (10) (10) (10) (10) (10)2 L P (10) 3 cm3 Po b in. 3 lb ft (10) (10)2 3
29 flo 1ft 1 i " 0 '=' 1 :z lie l i 1i :: C... f!... A.....c.. r. V) )(.".:.....b 4
30 10 4 AE DC. TO R ' J 'J ' 1'1.'1/ r>. lil [ SR t Ll JiV 1/ B' ; Fig.2 Air Mollier Diagram 5
31 9 'Hs u; OZ L t1 G01 1'<1 e 11 btd.l. V j{ ) 1\ 11 1\ l _. j t '}o ''H/H t= t= t= 801
32 :c::::. AEDC.TDR " t +. L_ f 0 C ll r... / f. V / ;1.3Pl L V 71/ 24 SR V / V r; /. / / / 1/ / / V V / " 1/ / / 't / 01/ OD V 1.1. V i: /.i/ V " 1 V 2 Q V V vy o/.. o ". / 1 / V /! l V Ll / / / 1/ " V Fig. 4 Air Mollier Diagram 7
33 AEDC. TDR [/ 1.1. V ' ' V 19 V '/ J 'll '/ 1/ ' [/!7 1 1/ l. V V:V V 22 r.j 111/ 1/ V :; 'V v V 1/ V V VV V 23 " L L til i } 'L / V ) r t.: 1.1 j / 'l D 1/ V '!.ll ') f V!j P ' 1.1 V V V V V." ' ' ' :; /. / / V' it VAl 1/1 ' ' V 1 v i bf 1/11' L r'i '/ V ' r:.;.1 1 P V [ / '/ SR Fig.5 Air Mollier Diagram 8 ")i " l') 1 A l ll ' 1/ j. / \ V V V ' V lot it V. )"11 J... :' t V' / \t 1 ' 1) 1/ V 1 r' '/ t: b' 10. v' V 1/1 '/ V V V V V t 1/1' J 1/ V V V
34 AEDC TDR ;... f. r rl ' ) 16 / il i'1'l 17 J ) :l f 110 i.e " fi' F p' 11 1 Jl 102 wwwwww SR Fig.6 Air Mollier Diagram 9
35 AEDC.TDR J 'f V ' ' 1/ ' 1.11' 1 il' f' ; 1 / 1 1/ r i.' il ' V 1/ ' V ' ' ' /r l ' ' / J ' V ' ' / li ' / 'f 1/ V 'V ;/ ' '" " 1/ V 1/... " t: L ' ' i' " [."? a. 1/ '" 1/ V' '" J '" " v 1/ ' 1 V V. )(V '" 1/ V ;t l..: '" k" ' ; " l{ '.. "f 1/ '" V 'V ' iii' ' 1/11 ' ' 1/ V' 1/ V' 1'1/ '' 'J [ 1/ // Ji' ' V /V [S V' t)# 1.1' 1/ V [ V ly ' 1 V ' 81' ' ' V tt ll V ' V 1/ V V 1 V 19 V '" ' 1/ [' /.VV V 1' j t' rn L '" SR Fig.7 Air Mollier Diagram
36 AE DC. TD R :=..... _t. '71/ f \ '.. 1/ 1/. "' l&' J rt [j 1/ / '(J 1/ 1/ V 1/ ) 1/ 1 i1 / / V ) 1/ 1/ 1/ rj 1/ V 1/ 1/1) 29 J 1/ / 1/11 / / L / [ 1/ ) ' 1/ 12 V ' ' 1/ ' ' 1/ 1/ V V J 1/ iii i / li 1/ 1/ / Ll! ti' 1/ ' 1/ 1/ r; /11 30 V t:. 1.1 [) L V/ 1/ 1/ ' V 1/ rj V./ 1/ 1/ 1/ 01/ 1/ ii ' V V LrL SR Fig.8 Air Mollier Diagram 11 A. So '/1 i" " ' 1/ " ) ;. 19 1/ 1/ V 1/ 1/ i/ :i" '4" ltv 1/ 1/ 1/ / V lw / /t 1// i 1/ " ls '" 1/ 1/ 1 iii 1/. f1 V <V :..4 1/ 1/ V / 1/ 1/ b J l:" llll L V r/ / 1/ j l
37 AE DC. TDR H/R <>x V 1/ 1/ 1/ V tf "" 1/ s. j V 1/ ' 1111 L 1/ Li" f\.j0' 1/ V 1/ / 1/ V V V / L L Y J 1/ ' V 11/ 1/ V V " V 1/ V V '1' r.c' V 1<2' i' ' 1/ V 'l VV 1/ to J 1/ t 1/ 1/ 1/ 1/ 1/ V " " '' J 1'1 foil 1/ " / :; / V / J V V u: 1/ l V i ) i 1/ 1/..l 1 /. ) A " 2f;i"i.2' "" il i/y V/ 1/ rj ) i fz"r. 1/ '/ 1/ 1/ r i 1/ o ) r TT T SR Fig.9 Air Mollier Diagram 12
38 10 6 AEDC TDR ! 'i"'r v l J.. f.' ' J...; v e:: "" ::: v 6!:!i "" ""' 10 J..!jo.; j..oli:l '.i l io > i=i= 1; SiR Fig.10 Air Mollier Diagram 13 j... ri p. "" k "io' k: ".." 10 ""r= P ""F. 1:::"" : '"' p"' r;; t;ij.: [Q[Q. "FF'!= i: D 11' "" 1lr1' 1::1:= ' 1:::= r.::'" c' J "" :::= ""t;
39 . AEDC.TDR E:: f'i t;>. r :.. r. ;;;: Y Y ' i' V V V Y V V v oo' yo 11 b V V... V y y v V v 1/11' '" V V.; 11 V '/ " V 'll '" '/ V' 'rl 1/? 1/ 1/ / 36 y V '" V f:;!c.: t. V J...:: V V V t. t. V. v r:: f'l. V V po 37 V b V v V V "'v v v v vv' r;.. V "' v!.o v 1/1'/ V 1/1." l"1/ V lilt c.it' 1t>1' V ] bl. 1/ 1/ 1/ 11'1/ 17 1/ Fig. 11 SiR Air Mollier Diagram 14.; ii Y.: ): V:. V V jo/ Q t. V Tl' il>" v V { j y jill!'" L" V V "'" f V Y V t&? rj b V [;; tt V 11. t. i' 0 V t( e V 1::'" 17 1:1. i1v. 1/ ; 1/ d: 1v Ji V' 11 k:! J. br'1v V V ' b': /' v.; V' Ji1:p 1/ 11 ; i)\> '" 1/ 1110 v vi/ v/.y 1 v' th F k'
40 AEDC.TDR V tl ". ll) rj 1/ rt' 1/ 1/ 1/ V 1/ J l" t / / / / Gil rj i!hi V V V / / V V / V V >' / oj 1/ VOl 1/ V / / illy / 1/'4 1/ '/ ' 1/ /'1 ' ' 1/11 ''!/ ' ' V V V V 1/ fl V V 11/ V 1111 l? 1(1/ 1/ V / V ; L / 1/ ' i / V 1/ 14 1/ V 1/ V 1 V ' 1/ 1/ V) / 1/ V ' )" ll" V r! i 1/ 1/ ' / ")0 '" il 1/ j 1/[1 1/ 1/ 1/ '/ 1/11 / VV!e" SR Fig. 12 Air Mollier Diagram 15 '" 'L
41 AEDC.TDR '.. _. r 1. H/R /. f V L 1.( 1/ V 1/ 1/ V V / '. /: 1/ 1/ L ' f JJ V' 11 i 1/. 1/ 1/ JJ 1/1/ 1/ V 1/ 1/ t 1/1/ 1/ 1/ i J. :\ L [J... ' U.J.. 'J 7 1/ 1/ V' A ' V 1/ V' l/ 'J / V V 1/ 1/ ' 1/ Y 1/1/ 1/ V V V 1/ 1/ 1/!.1? J; tjll J 1/ 1/ ' 1/ 01/ 1/ i.tv ill 1/ VlW.W ti /) 1/ 1/ ij A 1& 1/11 1/ 1/11 ) V 1/1/ 1/ 1/ 1111 ii' 1\ / i) i i' V? 111) 1/ J r i' 1/ :/ 1/ j rj /) ii. 1/1) 1/ 1/ 1/1\ 17/ SR Fig.13 Air Mollier Diagram 16
42 10 6 AEDC.TDR ;::= :::;. i=:: l' '" '" 1'.. :::::... "';;. ;;:; > F== '9 D i'" b:: i"f= ::::... E::;:? PO::::... :;; F'''' ;::: P ". f :::F'? ""... "'f:'r "" 1''''' i';> 0 ". 9 p::: f ::! 1'; ;:;::::Fi=i :... :::. ;... "'" io'" :::: "" "1== SiR Fig. 14 Air Mollier Diagram 17 l;:: f f"" i" "" f" " i'" f fi'".. ij::.. :'''' fi"!5i'" i:! ::trt.' f ::io; 1 \. :;: i"" H'".. F
43 AEDC.TDR _'" i"'" : r._.! r i" i" ': ; ;....;.;....; '. SR Fig. 15 Air Mollier Diagram 18
44 AEDC. TDR uullllllllllu SR Fig.16 Air Mollier Diagram 19
45 AEDC.TDR =tt: :.l H=! 1±±_4=: ; 1 l=t:+. +t+ ::: j.. 1 i+..i. r= l t:t+tt:t:t::tl=t:1 tt:t=t::t+==1=t=:: :: J: t: L. ::i( $t.1.r:.i: +:! 11. f + l l:.1=1 tf t.l LHHH.. i1'++1+1 f it: + + i r!.. +itchtcltr 1ffhf'+cLh.f+l.li i ' + H++H+++H+t+H++++'+t++++jl+t+H+f++H f'r '1 f ( jt+t+hh+tjjt+++++h+th+++++h+h AHvlH.:4i'J t : T jittt+itlllti+i+ tit1t:it H! HithH+tjjHt +++++t++ fi J:Flt. =ti +=++++H HtitHi J+L +vl. PT_'H++t+HH.t _.i' t H+i+H+ ttttttttt=h+r 1 _L.l_..!! i _l tt ++++HHt+HH +Hf++H++HH+H+++++tH+++++H++Hl :.1 1 +l++++++l ' ihl+++tcitltt+t+1++t+tt+ith lhh1+l SR Fig. 17 Air Mollier Diagram 20
46 10 6 f+ r' )1 t =r 1=1=it=i 1 H rr =j= AEDC.TDR 63 ]90 r H 1'' L ' T i +._. ::t= =i= L " r " po l "'" p 11 1oo!::= 100 ;..1 l 1'''" j...; j..oo l l"" i" 1::::1:::: l '" j.::: 1/ lt':1. ti O 1 l l " ' i:: 0 r "" l 10:.: 11 " &:: o f1... k l r l! '" ' 10 l td 101. r: z:' i"l'id. F l ""E! loop. '" l... :::: t::::t:= r..t:: \1 Jt' S \ SR Fig. 18 Air Mollier Diagram 21
47 AEDC.TDR f"... ttf::.io"'b."'1fl1...j..h.. irv';" "f A.. ii' '".. 0'"! j:vt"oh:l...llj... HHj ++++f lhh+f+llhhhl v rr++tttttrrrhyh++++++rlht++++++?vbvhhhi++rrhh++++hy w SR Fig. 19 Air MoWer Diagram 22
48 AEDC.TDR '.. jj 0 F :::: u: :::: ;:: "lor".' ;:: ::::::::? ;:: i.:: 'r' f" 0 :: 7$ f1: '" ::::.... f f p... f""'" ::::. ;r SiR Fig. 20 Air Mollier Diagram.p.::. 1'\... i:::"1r 1:::=== 0 f.o l.. ;:: 4....!t l.s... r:::: :::: ;:: " ::: :::: 'il " 2.3
49 AEDC. TDR SR Fig.21 Air Mollier Diagram 24
50 . A E DC. TO R "" j = " t j o k " f '; i== f... F*='F" f' ' ro" '" 11 ::l. 1:= F l "'. i:! 1oOf... j:::: 111 F:: k:f ;;;!tl F: hide 11 btl. l + t f H ::: PF::! & i=' 101== t:::.. :t. F= f' t"l f lo" b 10"1"". lq: F6 t:t1. ; +l SR Fig. 22 Air Mollier Diagram 2!1
51 AEDC.TDR SR Fig.23 Air Mollier Diagram 26
52 10 6 AEDC.TDR c "''':' ::F' l 1'1' ;... "' "".... i:= : F 1= 11'.. 1==::: f'.. r ;: ::: 1=== ft!: :::.r: i""... roo... :;E t'" f:: ;<:.J ::: fo fo fo SR Fig. 24 Air Mollier Diagram
53 AEDC.TDR SR Fig. 25 Air Mollier Diagram
54 tt :. ++i :le rl' +. :1 '±±: ++ + H + AEDC.TDR '.:. o... o 'f) 10 5 u SR Fig. 26 Air Mollier Diagram 29
55 AEDC.TDR =r H/R ok () 105wwwwww S/R Fig. 27 Air Mollier Diagram 30
56 106 AEDC. TDR ". 105WWWWLULLUWLULULLLULLUULU SR Fig. 28 Air Mollier Diagram
57 AEDCTDR63_ SR Fig. 29 Air Mollier Diagram 32
58 10 6 AEDCTDR63190 " = SR Fig. 30 A ir Moll ier 0 iagram 33
59 AEDC.TDR SR Fig.31 Air Mollier Diagram 34
60 106 : A EDC. TDR SR Fig. 32 Air Moll ier 0 iagram 35
61 AEDC.TDR SR Fig.33 Air Mollier Diagram 36
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