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DENSITY OF LIQUID REFRIGERANTS 
By 
T SHYAMKUMAR 
14TH14F 
I sem, M Tech 
Thermal Engineering
CONTENTS 
 Introduction 
 Methods of measuring density 
 Literature Review 
 ISH correlation 
 Rackett equation 
 Rackett equation by Yamada and Gunn 
 Spencer and Danner modification of Rackett method(RSD) 
 Hankinson and Thomson (HT) method(COSTALD) 
 Reidel method 
 NM Correlation 
 Programming 
 Results 
 Conclusion
INTRODUCTION 
 Designing refrigeration cycles require thermodynamic 
properties of refrigerants, i.e., liquid density, vapour 
density, enthalpy of vaporization and vapour pressure 
Liquid density is needed for process simulation and 
equipment design. 
 Equations of state (EoS) are used in commercial simulation 
software for predicting phase behavior and thermodynamic 
properties.But, equations of state are not accurate enough 
for a wide range of applications. The popular EoSs such as 
SRK and PR predict liquid density with an average absolute 
error of about 8%, much higher than the correlations . 
 correlations have wider range of applicability and accuracy.
TWO SINKER DENSIMETER 
 Based on the 
Archimedes' 
buoyancy principle. 
 Both sinkers have 
the same mass, the 
same surface area, 
and the same surface 
material, but a 
considerable 
difference in 
volume.
Continue... 
 This sinker support is connected to a commercial analytical 
balance ( resolution 10 μg) by a thin wire via a magnetic 
suspension coupling . 
 “apparent mass difference” Δm* = (mD* − mS*) of the 
sinkers. 
 By means of the magnetic suspension coupling, the 
suspension force is contactlessly transmitted from the 
pressurized measuring cell to the balance at ambient 
conditions. 
 ρ = (Δm* − ΔmVac) / (VS − VD), 
where ΔmVac= ( mD − mS) corresponds to the very small 
mass difference of the two sinkers which is accurately 
determined by weighing in the evacuated measuring cell.
CORIOLIS FLOW METER 
 Based on coriolis principle. 
 An exciter causes tube to 
oscillate constantly 
 Sensors are located at inlet 
& outlet 
 Phase shift during flow is a 
measure of mass flow rate. 
 Oscillating frequency is a 
direct measure of density. 
.
LITERATURE REVIEW 
(a) ISH correlation (Iglesias et al [1]) 
= (2.1) 
= 0.03 – (2.1.a) 
= (1 - ) – 1 - 
(2.1.b) 
= 
n=0.5 and β is the scaling exponent having a value between 0.32 and 0.34
Rackett equation 
Rackett(1970),[2] proposed the following correlation 
......(Eq 2.2) 
= 
is critical compressibility factor.
Modified Rackett equation by 
Yamada and Gunn 
 Yamada and Gunn (1973), [2] proposed 
.....(Eq 2.3) 
Acentric factor 
= 
] - 1 
W represents accentricity or nonsphericity of a molecule.For 
monoatomic gases w =0. 
For higher hydrocarbon w increases.
Spencer and Danner modification of Rackett 
method 
By Kh.Nasrifar et al[3] 
Popularly known as RSD equation 
.....(Eq 2.4) 
= ( ) 
ZRA = 0.29056- 0.8775w
Hankinson and Thomson (HT) method 
By Hankinson et al[4] 
.......(Eq 2.5) 
( ) = [1- ] 
= 1+a +b +c +d 
a = -1.52816 ; b = 1.43907; 
c = -0.81446 ; d = 0.190454 ; 
e = -0.296123 ; f = 0.386914 ; 
g = -0.0427258 ; h = -0.0480645 ; 
is the characteristic volume 
=
Reidel method 
Reidel [3] suggested the following correlation 
......(Eq 2.6) 
= = 1 + 0.85 (1- + (0.53 + 0.2 ) 
= 1 + 0.85 (1- + (1.6916 + 0.984 ) 
is the slope of vapour pressure at critical temperature
NM Correlation 
KhashayarNasrifar and Mahmood Moshfeghian proposed the following 
correlation [5] 
= [1+ ] 
= 1+ 
+ 
+ + 
d1 = 1.1688 
d2 = 1.8177 
d3 = -2.6581 
d4 = 2.1613 
δ is the characteristic parameter for each compound. 
= <1 
= >1 
c1, c2 and c3 are vapour pressure dependent parameters
Correlation Suitable refrigerants Comments 
ISH R22, R123, R134a, R152a, R290, R600, 
R600a, R717, R718, R12 
Rackett R22, R32, R123, R125, R134a, R152a, 
R290, R600, R600a, R717, R718, R1270 
R143a, R12 
For all 
compounds 
with Zc > 0.22 
Yamada& Gunn 
R22,R32,R123,R125,R134a,R152a, 
R290,R600,R600a,R717,R718,R1270 
R143a,R12 
Spencer& Danner R22,R290,R600,R600a,R717,R718,R1270 
Hankinson & Thomson R22, R290, R600, R600a, R717, R718, 
R1270 
Applicable 
when 
0.25 < Tr < 0.98 
Reidel 
R22,R32,R123,R125,R134a,R152a, 
R290,R600,R600a,R717,R718,R1270 
R143a,R12 
NM 
R22,R32,R123,R125,R134a,R152a, 
R290,R600,R600a,R717,R718,R1270 
R143a,R12
PROGRAMMING 
Coding language:MATLAB 
The program reads input data from excel sheet, 
calculates saturated liquid densities and percentage 
deviation from ASHRAE values for temperature ranges 
specified in ASHRAE data hand book and writes it 
back to another excel sheet.Average absolute 
percentage deviation is also calculated. 
Two plots for each refrigerant: 
Density vs temperature 
%error vs temperature
ERROR ESTIMATION 
Percentage deviation from ASHRAE values, 
δ =(ρs –ρexp)*100 .... (Eq 7) 
Average absolute percentage deviation = 1/N*Σ|δ|..(Eq8) 
Where N is the number of data points .
RESULTS 
calculated densities
Average absolute percentage deviations 
Refrigerant ISH Rackett Yamada 
& Gunn 
RSD HT Reidel NM Best 
correlation 
R22 0.281556 1.442423 1.2503372 1.52110 0.33468 0.29246 0.25362 NM 
R32 2.289975 3.49270887 2.91578 0.7023 NM 
R123 1.049479 1.049479 0.3235613 0.68225 0.37057 Yamada 
& Gunn 
R125 2.3816 0.80894612 0.43202 0.56296 Reidel 
R134a 1.225932 1.225932 1.21537009 1.09272 0.40607 NM 
R152a 0.65903 0.65903 3.44362871 2.90145 0.52618 NM 
R290 0.371952 0.618689 0.363586 0.3766 0.1066 0.49043 0.29022 HT 
R600 0.374877 0.691794 0.45620980 0.3777 0.3487 0.58189 0.25245 NM 
R600a 0.484182 3.240646 2.36065152 0.5651 0.0735 2.16849 0.75051 HT 
R717 0.55532 1.184232 4.15963261 1.2214 0.9787 3.39811 0.8985 ISH 
R718 6.659881 4.832748 4.70070317 3.1206 23.835 4.57693 RSD 
R1270 1.552219 1.13710968 0.6716 0.3774 3.26391 0.6126 HT 
R143a 2.530843 1.580401291 1.36151 1.78446 Reidel 
R12 2.3492844 2.3492844 1.20655272 1.476334 0.89878 NM
CONCLUSIONS 
 NM correlation has been found the best the for 
prediction of saturated liquid densities for R22, R32, 
R134a, R152a, R600 and R12 with a maximum AAPD of 
0.89878 % for R12 
 Equation predicted by Hankinson and Thomson.et al 
is best suited for R290, R600a and R1270 
 Reidel’s correlation can be applied to R143a and R125 
 Modified Rackett equation by Yamada and Gunn and 
Spencer and Danner gives fairly accurate results for 
R123 and R718 respectively. 
 ISH correlation is best suited for R717 with AAPD of 
0.555%.
REFERENCES 
[1] Gustavo A Iglesias-Silva,Kennath.R.Hall,”A saturated liquid density 
equation for refrigerants”,Fluid Phase Equilib 131(1997) 97-105 
[2]The properties of Gases and Liquids, Fifth Edition, Bruce E poling, John M 
Prausnitz John P O’Conell , McGraw Hill, ’Rackett equation’(145-146) 
[3]Khashayar Nasrifar, Mahmood Moshfeghian, ”Evaluation of saturated 
liquid density prediction methods for pure methods”, Fluid phase Equilib 
158-160(1999),437-445 
[4]Risdon W Hankinson, George H Thomson, AIChE Journal (vol25, no4) 
(1979), 653-663 
[5]Khashayar Nasrifar, Mahmood Moshfeghian, “A saturated liquid density 
equation in conjunction with the Predictive-Soave–Redlich – Kwong 
equation of state for pure refrigerants and LNG multi component systems”, 
Fluid phase Equilib 153(1998),231-242
[6]Kh.Nasrifar,Sh.Ayatollahi,M.Moshfeghian,”An extended saturated liquid 
density equation”,Fluid phase Equilib166 (1999),163-181 
[7]Kh.Nasrifar,Sh.Ayatollahi,M.Moshfeghian,”Generalised saturated liquid 
density prediction method for pure compounds and multi-component 
mixtures”,Fluid phase Equilib168(2000),71-90 
[8]”Refrigerants-Physical properties”, http://www.EngineeringToolBox.com 
[9] “Liquid density by volume translated method- 
Part1”,http://www.jmcampbell.com/tip-of-the-month/2011/03/liquid-density- 
by-volume-translated-method-%e2%80%93-part-1-pure-compound/ 
[10]“Liquid density by volume translated method- 
Part2”,http://www.jmcampbell.com/tip-of-the-month/2011/07/liquid-density- 
by-volume-translated-method-%e2%80%93-part-2-recent-development/
Density of liquid refrigerants
Density of liquid refrigerants

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Density of liquid refrigerants

  • 1. DENSITY OF LIQUID REFRIGERANTS By T SHYAMKUMAR 14TH14F I sem, M Tech Thermal Engineering
  • 2. CONTENTS  Introduction  Methods of measuring density  Literature Review  ISH correlation  Rackett equation  Rackett equation by Yamada and Gunn  Spencer and Danner modification of Rackett method(RSD)  Hankinson and Thomson (HT) method(COSTALD)  Reidel method  NM Correlation  Programming  Results  Conclusion
  • 3. INTRODUCTION  Designing refrigeration cycles require thermodynamic properties of refrigerants, i.e., liquid density, vapour density, enthalpy of vaporization and vapour pressure Liquid density is needed for process simulation and equipment design.  Equations of state (EoS) are used in commercial simulation software for predicting phase behavior and thermodynamic properties.But, equations of state are not accurate enough for a wide range of applications. The popular EoSs such as SRK and PR predict liquid density with an average absolute error of about 8%, much higher than the correlations .  correlations have wider range of applicability and accuracy.
  • 4. TWO SINKER DENSIMETER  Based on the Archimedes' buoyancy principle.  Both sinkers have the same mass, the same surface area, and the same surface material, but a considerable difference in volume.
  • 5. Continue...  This sinker support is connected to a commercial analytical balance ( resolution 10 μg) by a thin wire via a magnetic suspension coupling .  “apparent mass difference” Δm* = (mD* − mS*) of the sinkers.  By means of the magnetic suspension coupling, the suspension force is contactlessly transmitted from the pressurized measuring cell to the balance at ambient conditions.  ρ = (Δm* − ΔmVac) / (VS − VD), where ΔmVac= ( mD − mS) corresponds to the very small mass difference of the two sinkers which is accurately determined by weighing in the evacuated measuring cell.
  • 6. CORIOLIS FLOW METER  Based on coriolis principle.  An exciter causes tube to oscillate constantly  Sensors are located at inlet & outlet  Phase shift during flow is a measure of mass flow rate.  Oscillating frequency is a direct measure of density. .
  • 7. LITERATURE REVIEW (a) ISH correlation (Iglesias et al [1]) = (2.1) = 0.03 – (2.1.a) = (1 - ) – 1 - (2.1.b) = n=0.5 and β is the scaling exponent having a value between 0.32 and 0.34
  • 8. Rackett equation Rackett(1970),[2] proposed the following correlation ......(Eq 2.2) = is critical compressibility factor.
  • 9. Modified Rackett equation by Yamada and Gunn  Yamada and Gunn (1973), [2] proposed .....(Eq 2.3) Acentric factor = ] - 1 W represents accentricity or nonsphericity of a molecule.For monoatomic gases w =0. For higher hydrocarbon w increases.
  • 10. Spencer and Danner modification of Rackett method By Kh.Nasrifar et al[3] Popularly known as RSD equation .....(Eq 2.4) = ( ) ZRA = 0.29056- 0.8775w
  • 11. Hankinson and Thomson (HT) method By Hankinson et al[4] .......(Eq 2.5) ( ) = [1- ] = 1+a +b +c +d a = -1.52816 ; b = 1.43907; c = -0.81446 ; d = 0.190454 ; e = -0.296123 ; f = 0.386914 ; g = -0.0427258 ; h = -0.0480645 ; is the characteristic volume =
  • 12. Reidel method Reidel [3] suggested the following correlation ......(Eq 2.6) = = 1 + 0.85 (1- + (0.53 + 0.2 ) = 1 + 0.85 (1- + (1.6916 + 0.984 ) is the slope of vapour pressure at critical temperature
  • 13. NM Correlation KhashayarNasrifar and Mahmood Moshfeghian proposed the following correlation [5] = [1+ ] = 1+ + + + d1 = 1.1688 d2 = 1.8177 d3 = -2.6581 d4 = 2.1613 δ is the characteristic parameter for each compound. = <1 = >1 c1, c2 and c3 are vapour pressure dependent parameters
  • 14. Correlation Suitable refrigerants Comments ISH R22, R123, R134a, R152a, R290, R600, R600a, R717, R718, R12 Rackett R22, R32, R123, R125, R134a, R152a, R290, R600, R600a, R717, R718, R1270 R143a, R12 For all compounds with Zc > 0.22 Yamada& Gunn R22,R32,R123,R125,R134a,R152a, R290,R600,R600a,R717,R718,R1270 R143a,R12 Spencer& Danner R22,R290,R600,R600a,R717,R718,R1270 Hankinson & Thomson R22, R290, R600, R600a, R717, R718, R1270 Applicable when 0.25 < Tr < 0.98 Reidel R22,R32,R123,R125,R134a,R152a, R290,R600,R600a,R717,R718,R1270 R143a,R12 NM R22,R32,R123,R125,R134a,R152a, R290,R600,R600a,R717,R718,R1270 R143a,R12
  • 15. PROGRAMMING Coding language:MATLAB The program reads input data from excel sheet, calculates saturated liquid densities and percentage deviation from ASHRAE values for temperature ranges specified in ASHRAE data hand book and writes it back to another excel sheet.Average absolute percentage deviation is also calculated. Two plots for each refrigerant: Density vs temperature %error vs temperature
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  • 17. ERROR ESTIMATION Percentage deviation from ASHRAE values, δ =(ρs –ρexp)*100 .... (Eq 7) Average absolute percentage deviation = 1/N*Σ|δ|..(Eq8) Where N is the number of data points .
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  • 34. Average absolute percentage deviations Refrigerant ISH Rackett Yamada & Gunn RSD HT Reidel NM Best correlation R22 0.281556 1.442423 1.2503372 1.52110 0.33468 0.29246 0.25362 NM R32 2.289975 3.49270887 2.91578 0.7023 NM R123 1.049479 1.049479 0.3235613 0.68225 0.37057 Yamada & Gunn R125 2.3816 0.80894612 0.43202 0.56296 Reidel R134a 1.225932 1.225932 1.21537009 1.09272 0.40607 NM R152a 0.65903 0.65903 3.44362871 2.90145 0.52618 NM R290 0.371952 0.618689 0.363586 0.3766 0.1066 0.49043 0.29022 HT R600 0.374877 0.691794 0.45620980 0.3777 0.3487 0.58189 0.25245 NM R600a 0.484182 3.240646 2.36065152 0.5651 0.0735 2.16849 0.75051 HT R717 0.55532 1.184232 4.15963261 1.2214 0.9787 3.39811 0.8985 ISH R718 6.659881 4.832748 4.70070317 3.1206 23.835 4.57693 RSD R1270 1.552219 1.13710968 0.6716 0.3774 3.26391 0.6126 HT R143a 2.530843 1.580401291 1.36151 1.78446 Reidel R12 2.3492844 2.3492844 1.20655272 1.476334 0.89878 NM
  • 35. CONCLUSIONS  NM correlation has been found the best the for prediction of saturated liquid densities for R22, R32, R134a, R152a, R600 and R12 with a maximum AAPD of 0.89878 % for R12  Equation predicted by Hankinson and Thomson.et al is best suited for R290, R600a and R1270  Reidel’s correlation can be applied to R143a and R125  Modified Rackett equation by Yamada and Gunn and Spencer and Danner gives fairly accurate results for R123 and R718 respectively.  ISH correlation is best suited for R717 with AAPD of 0.555%.
  • 36. REFERENCES [1] Gustavo A Iglesias-Silva,Kennath.R.Hall,”A saturated liquid density equation for refrigerants”,Fluid Phase Equilib 131(1997) 97-105 [2]The properties of Gases and Liquids, Fifth Edition, Bruce E poling, John M Prausnitz John P O’Conell , McGraw Hill, ’Rackett equation’(145-146) [3]Khashayar Nasrifar, Mahmood Moshfeghian, ”Evaluation of saturated liquid density prediction methods for pure methods”, Fluid phase Equilib 158-160(1999),437-445 [4]Risdon W Hankinson, George H Thomson, AIChE Journal (vol25, no4) (1979), 653-663 [5]Khashayar Nasrifar, Mahmood Moshfeghian, “A saturated liquid density equation in conjunction with the Predictive-Soave–Redlich – Kwong equation of state for pure refrigerants and LNG multi component systems”, Fluid phase Equilib 153(1998),231-242
  • 37. [6]Kh.Nasrifar,Sh.Ayatollahi,M.Moshfeghian,”An extended saturated liquid density equation”,Fluid phase Equilib166 (1999),163-181 [7]Kh.Nasrifar,Sh.Ayatollahi,M.Moshfeghian,”Generalised saturated liquid density prediction method for pure compounds and multi-component mixtures”,Fluid phase Equilib168(2000),71-90 [8]”Refrigerants-Physical properties”, http://www.EngineeringToolBox.com [9] “Liquid density by volume translated method- Part1”,http://www.jmcampbell.com/tip-of-the-month/2011/03/liquid-density- by-volume-translated-method-%e2%80%93-part-1-pure-compound/ [10]“Liquid density by volume translated method- Part2”,http://www.jmcampbell.com/tip-of-the-month/2011/07/liquid-density- by-volume-translated-method-%e2%80%93-part-2-recent-development/