density of liquid refrigerants
TRANSCRIPT
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])
n=0.5 and β is the scaling exponent having a value between 0.32 and 0.34
= (2.1)
= 0.03 – (2.1.a)
= (1 - ) – 1 -(2.1.b)
=
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
W represents accentricity or nonsphericity of a molecule.Formonoatomic gases w =0.
For higher hydrocarbon w increases.
=
] - 1
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)
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
( ) = [1- ]
= 1+a +b +c +d
=
Reidel method
Reidel [3] suggested the following correlation
......(Eq 2.6)
is the slope of vapour pressure at critical temperature
= = 1 + 0.85 (1- + (0.53 + 0.2 )
= 1 + 0.85 (1- + (1.6916 + 0.984 )
NM CorrelationKhashayarNasrifar and Mahmood Moshfeghian proposed the following
correlation [5]
d1 = 1.1688d2 = 1.8177d3 = -2.6581d4 = 2.1613δ is the characteristic parameter for each compound.
c1, c2 and c3 are vapour pressure dependent parameters
= [1+ ]
= 1+ + + +
= <1
= >1
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 & GunnR22,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 .
RESULTScalculated densities
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
Average absolute percentage deviations
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 MPrausnitz 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 Equilib158-160(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 – Kwongequation 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/