AIJRRLJSM VOLUME 1, ISSUE 6 (2016, JUNE) (ISSN-2455-6300) ONLINE ANVESHANA’S INTERNATIONAL JOURNAL OF RESEARCH IN ENGINEERING AND APPLIED SCIENCES
EXPERIMENTAL COMPARISON OF SINGLE AND MULTISTAGE AIR COMPRESSOR EFFICIENCIES UNDER THE SAME RECEIVER TANK PRESSURE 1
P.V.RAMANA & 2D.RAMBABU
1
Associate professor-Mechanical Engineering Department 2 Asst. professor-Mechanical Engineering Department CVR College of Engineering - Hyderabad (T.S)-India
ABSTRACT Compressors are widely used for many engineering applications in day to day life. Compressors are classified based on design as reciprocating and rotary compressors, Reciprocating compressors are single acting ,double acting ,air cooled ,water cooled and single stage ,multistage ,depends on application of usage. It is clear by theory as given by author’s multistage compressors having advantage over single stage compressors but practically not aware to what extent the variations in efficiencies are taking place and exact experimental figures in that area not focused with clarity. So here focus is given to conduct experiment on both single stage and multi stage compressors at the different receiver tank pressure. Obtained readings are calculated for the same receiver tank pressure and then comparing the results for both the compressors. To know the variations in efficiencies of both compressors results are tabulated and compared to find out the efficiencies for better understanding the subject. Keywords: single stage compressor, multistage compressor, LP cylinder, HP cylinder, volumetric efficiency, isothermal efficiency.
cylinder say L.P cylinder and allow this pressurized air to another cylinder say Intermediate cylinder (IP) and develop Higher pressure higher than the LP cylinder and allow this pressurized air in another cylinder say HP cylinder and develop more pressure then intermediate cylinder finally highly developed pressurized air is delivered to the end user applications. This is possible by going for multi stage cylinder compressor. This paper focused on conducting the experiment on compressors to find what differences made when using single and multistage compressor in efficiencies and comparing its experimental results for giving the conclusions for the usage. 2.0 EXPERIMENTAL SET UP SINGLE STAGE COMPRESSOR
OF
The details of the experimental setup of single stage reciprocating Air compressor is as follows
1.0 INTRODUCTION Reciprocating air compressors are widely used to get high discharge pressure. To get high discharge pressure single stage compressor has to work against high compression ratio in terms of pressure so to withstand high compression ratio body of compressor also be made robust in construction . It will add more weight to compressor and also leads many mechanical problems because it is working for the development of high pressure in single cylinder and also it is not suitable because of this reasons when to go for developing high delivery pressure for industrial applications. So alternative is increasing the delivery pressure in number of cylinders step by step and reducing the weight of the compressor. first developing pressure in one cylinder of
Fig1: single compressor
stage
reciprocating
Air
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Specifications of the compressor: Make Type Stage Cylinder Bore Stroke length Motor rating Motor speed Compressor speed Electric supply HZ Type of starter Belt size Type of lubrication Type of cooling Type of fan
: ELGI : Reciprocating Type : single stage : single cylinder : 60 mm : 60 mm : 2 HP : 1420 RPM : 930 RPM : 415V/380V, 3ph, 50
Rec eiv er Tan k Pre ssur e (bar s)
Suc tio n Pre ssu re P1( bar s)
Disc harg e pres sure P2(b
Suctio n Temp eratur e T1 0 C
ars)
3.1 Sample calculations for Reading -1 at 2 bar pressure Sample calculations for Reading -1 Volume of air sucked in to the cylinder Va =Cd x Ao x
: DOl : B40 : splash : Air cooled : forced draught
Where H =
Disc harge Tem perat ure T2 0 C
S pe ed R P M
Man omet er Read ing(h )mm
x 3600 x
= 16.825 meters
Ti me per 10 Re vol uti on ssec
2
3
2
4
6
1
1
1
3.8
6.4
8.4
24
24
24
109
125
136
8 7 6. 0 8 7 2. 2 8 6 9. 3
20
6.7 8
x
Theoretical volume of air Vth = d2xLxNx60
M3/hr
Vth = x0.062 x0.06 x876x60= 8.9165 M3/hr Volumetric efficiency
ηvol
=
ηvol
=
x 100 x 100 = 80.3%
Compression ratio Rp = 1
M3/hr
Va =0.62 x 1.767 x10-4 x 3600 = 7.1656 M3/hr
3.0 SINGLE STAGE COMPRESSOR Table1: table of Readings of single stage compressor as follows S . N O
Ta = Ambient Temperature of air P1 = suction pressure of air P2 = discharge (cylinder outlet) pressure
=
= 3.8
Piso = max RaxT1 x ln(Rp) Where ma = Va x
15
6.5
=density of air ma = 7.1656 x 1.1887 =8.5117 M3/hr
14
6.0
Piso = max RaxT1 x ln(Rp) Piso =
x 0.287xT1 (273+24)x ln(3.8)
=0.269 KW T1 = suction Temperature of air entering in to the cylinder T2 = discharge Temperature of air leaving the compressor
As per the relation (temperature, pressure and volume) for polytrophic process
=
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ln(
) = =
Theoretical volume of air
x ln(3.8)
Vth = d2xLxNx60
= 0.1885
M3/hr
Vth = 8.877 M3/hr I.P = I.P
x
max RaxT1
=
1]
x
x
Volumetric efficiency ηvol = x 100
0.287x297
ηvol
1] =0.302 KW
= 70.46%
Power input to Motor (Pm )
Compression ratio Rp =
Pm =
Piso = max RaxT1 x ln(Rp)
Where 3200 = Energy meter constant Pm =
Where ma = Va x
= 1.659 KW
=density of air
Power input to compressor Pc = Pm x 0.8 Pc = 1.659 x 0.8 = 1.327 Kw
Mechanical efficiency
= =
x 100 x 100 =
ma = 7.4365
M3/hr
Piso = max RaxT1 x ln(Rp) Piso =0.326 KW As per the relation (temperature, pressure and
22.75 %
Overall efficiency
= 6.4
=
x 100 =
x 100 =
volume) for polytrophic process ln(
) =
=
x ln(6.4)
20.27 % = 0.15768 Isothermal efficiency
= =
x 100 x 100 = 89
%
I.P =
x
max RaxT1
1]
I.P =0.3796 KW
3.2 Similarly Sample calculations for Reading -2 at 4 bar pressure Volume of air sucked in to the cylinder Va =Cd x Ao x
x 3600
M3/hr
Power input to Motor (Pm ) Pm = Where 3200 = Energy meter constant
Where H = 12.618 meters
Pm = 1.7307 KW
Va = 6.256 M3/hr
Power input to compressor Pc = Pm x 0.8
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Pc = 1.7307 x 0.8 = 1.384 Kw
Piso =0.359 KW As per the relation (temperature, pressure and
Mechanical efficiency Overall efficiency
=
= x 100 = 27.41 % x 100 = 23.5 %
=
Isothermal efficiency
volume) for polytrophic process ln(
) =
x ln(8.4)
= 0.1503
x 100
I.P =
= 85.8%
=
x
max RaxT1
1]
I.P =0.423 KW
3.3 Similarly Sample calculations for Reading -3 at 6 bar pressure
Power input to Motor (Pm )
Volume of air sucked in to the cylinder
Pm =
Va =Cd x Ao x
x 3600
M3/hr
Where 3200 = Energy meter constant
Where H = 11.77 meters
Pm = 1.875 KW
Va = 5.995 M3/hr
Power input to compressor Pc = Pm x 0.8
Theoretical volume of air Vth = d2xLxNx60
Pc = 1.875 x 0.8 = 1.5 Kw
M3/hr
Mechanical efficiency
Vth = 8.877 M3/hr
=
= 28.2 %
Volumetric efficiency
ηvol
=
ηvol
= 67.52 %
Overall efficiency
x 100
Compression ratio Rp =
x 100
=
x 100 = 23.9 %
= 8.4
Isothermal efficiency
=
x 100
= 84.8%
Piso = max RaxT1 x ln(Rp) Where ma = Va x =density of air
Ma = 7.126 M3/hr Piso = max RaxT1 x ln(Rp) ANVESHANA’S INTERNATIONAL JOURNAL OF RESEARCH IN ENGINEERING AND APPLIED SCIENCES
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3.4 Comparisons table of values for single stage compressor Table2: table of results B ηv a ol r 2 80 .3 4
6
70 .4 6 67 .5 2
Pis
IP
Pc
o
ηm
ηo
ηi
ech
vera
so
T 2
8 9. 0 8 5. 8 8 4. 8
1 0 9 1 2 5 1 3 6
ll
0. 26 9 0. 32 6 0. 35 9
0.3 02 0.3 79 6 0.4 23
1. 32 7 1. 38 4 1. 5
22 .7 5 27 .4 1 28 .2
20 .2 7 23 .5 23 .9
R P M 87 6 87 2. 2 86 9. 3
Comparison shows as pressure is increasing volumetric efficiency and isothermal efficiency is decreasing but isothermal power increases and also other efficiencies like mechanical, overall efficiencies are increases with increase of the pressure 4.0 EXPERIMENTAL SET UP MULTISTAGE COMPRESSOR
Stroke length Motor rating Motor speed Compressor speed Electric supply HZ Type of starter Belt size Type of lubrication Type of cooling Type of fan
Table3: Table of Readings of multistage compressor as follows Ta P P P nk 1 2 3 Pr ess ur e 2
4
6
Specifications of the compressor: Make Model Type Stage Cylinder LP cylinder bore HP cylinder bore
: ELGI : TS 03120 : Reciprocating Type : two stages : two cylinders : 70 mm : 50 mm
: DOl : A68 : splash : Air cooled : forced draught
5.0 MULTISTAGE COMPRESSOR
OF
Fig2: multistage compressor test rig.
: 85mm : 3 HP : 1420 RPM : 930 RPM : 415V/380V, 3ph, 50
1 0 . 9 5 1 1 . 0 5 1 1 . 1
1 . 9 4 . 4 5 6 . 4
M a n o m et er 2 0 0
Time RPM per 5 revol ution s
T T 1 2
T T 3 4
42.75 928
2 1 8 0 0
8 8 6 8
1 9 3
36.97 923
2 1 9 1 4
9 1 6 3 1
1 8 9
34.59 917
2 1 9 1 4
9 1 8 5 7
T1 =Temperature of air entering L.P cylinder T2 =Temperature of air leaving L.P cylinder T3 =Temperature of air after intercooler and entering H.P cylinder T4 = temperature air leaving HP cylinder Ta = ambient temperature/ P1 = atmosphere pressure 1 bar P2 = L.P cylinder outlet pressure P3 = H.P cylinder outlet pressure
5.1 Sample calculations for Reading -1 at 2 bar pressure Sample calculations for Reading -1 Volume of air sucked in to the cylinder Va =Cd x Ao x x 3600 M3/hr
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Where H =
x
I.P =
= 170.517 meters
Va =0.62 x 1.767 x10-4 x 3600 = 22.812 M3/hr
x
I.P
x
max RaxT1
=
1]
x
x
0.287x301
1] =0.430 KW Theoretical volume of air Vth = LxNc (A1 + A2) x60 M3/hr
Power input to Motor (Pm )
Area of first cylinder-A1=
Pm =
Area of first cylinder-A1= Where 3200 = Energy meter constant -3
-3
Vth = 0.085x928 (1.9634 x 10 + 3.848 x 10 ) x60 M3/hr Vth = 27.506 M3/hr
= 2.105 KW
Power input to compressor Pc = Pm x 0.8 Pc = 2.105 x 0.8 = 1.684 Kw
Volumetric efficiency ηvol = x 100
ηvol
Pm =
Mechanical efficiency =
=
x 100
x 100 = 82.9%
= Compression ratio Rp =
=
= 1.9
x 100 =
25.53%
Piso = max RaxT1 x ln(Rp) Overall efficiency Where ma = Va x =density of air
=density
of air
=
x 100 =
=
=1.1729
x 100
= 24.47 % Isothermal efficiency
ma = 22.812 x 1.729 =26.756 M3/hr
= =
x 100 x 100 =
Piso = max RaxT1 x ln(Rp)
95.9 %
Piso =
5.2 Sample calculations for Reading -2 at 4 bar pressure
x 0.287x (273+28)x ln(1.9)
=0.4121 KW Sample calculations for Reading -2 As per the relation (temperature, pressure and volume) for polytrophic process ln(
) = =
=
x ln(1.9) = 0.28317 and n=1.396
Volume of air sucked in to the cylinder Va =Cd x Ao x x 3600 M3/hr Where H =164.549 meters Va =0.62 x 1.767 x10-4 x 3600 = 22.812 M3/hr
x
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Theoretical volume of air Vth = LxNc (A1 + A2) x60 M3/hr
Pm = Where 3200 = Energy meter constant
Area of first cylinder-A1= Area of first cylinder-A1=
Pm = 2.434 KW
Vth = 0.085x923 (1.9634 x 10-3 + 3.848 x 10-3) x60 M3/hr
Power input to compressor Pc = Pm x 0.8 Pc = 2.434 x 0.8 = 1.947 Kw
Vth = 27.354 M3/hr
Mechanical efficiency
Volumetric efficiency ηvol = x 100
ηvol
=
=4.45
Overall efficiency
=
x 100 =
x 100
= 48.3 %
Where ma = Va x =density of air of air
x 100
= 52.09%
Piso = ma x RaxT1 x ln(Rp)
=density
x 100
=
x 100 = 81.9%
Compression ratio Rp =
=
Isothermal efficiency
=
x 100
= =
=1.1729
x 100 =
92.8 % 3
ma = 22.409 x 1.729 =26.283 M /hr Piso = max RaxT1 x ln(Rp)
5.3 Sample calculations for Reading -3 at 6 bar pressure
Piso =
Sample calculations for Reading -1
x 0.287x (273+28)x ln(4.45)
=0.9415 KW As per the relation (temperature, pressure and
Volume of air sucked in to the cylinder Va =Cd x Ao x x 3600 M3/hr
volume) for polytrophic process
Where H = 161.139 meters
ln(
) = =
I.P =
=
Va = 22.175 M3/hr
x ln(4.45)
Theoretical volume of air Vth = LxNc (A1 + A2) x60 M3/hr
= 0.1971 and n=1.2454
x
max RaxT1
I.P = 1.0143 KW Power input to Motor (Pm)
Area of first cylinder-A1= 1]
Area of first cylinder-A1= Vth = 0.085x917 (1.9634 x 10-3 + 3.848 x 10-3) x60 M3/hr Vth = 27.178 M3/hr
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Mechanical efficiency
Volumetric efficiency ηvol = x 100
ηvol
Overall efficiency
Isothermal efficiency
of air
Table 4: table of results for multistage compressor
Piso = max RaxT1 x ln(Rp) x 0.287x (273+28)x ln(6.4)
pre ssu re 2
ηv
Pis
ol
o
8 2. 9
0. 41 21
0. 45 19
1. 68 4
2 6. 8
4
8 1. 9 2 8 1. 5 9
0. 94 15
1. 09 4
1. 94 7
5 6. 1
1. 15 85
1. 33 7
2. 08 15
6 4. 2 3
=1.1585 KW As per the relation (temperature, pressure and
) =
=
x ln(6.4) 6
= 0.1921 and n=1.2377
I.P =
x
x 100
5.4 Comparisons of values for multi stage compressor
=
ma = 22.175 x 1.729 =26.009 M3/hr
volume) for polytrophic process
= = 93.5%
=1.1729
ln(
x 100 = 55.6 %
Where ma = Va x =density of air
Piso =
=
=
Piso = max RaxT1 x ln(Rp)
=density
x 100
= 59.6%
=81.59%
Compression ratio Rp =
=
max RaxT1
1]
I.P =1.2377 KW Power input to Motor (Pm) Pm = Where 3200 = Energy meter constant Pm = 2.6019 KW
IP
Pc
η
ηo
ηi
me
vr
so
2 4. 4 7 4 8. 3
9 1. 1
ch
5 5. 6
8 6. 0 6 8 6. 6
T R 4 P M 8 9 9 2 8 1 3 1
9 2 3
1 5 7
9 1 7
Comparison shows as pressure is increasing volumetric efficiency and isothermal efficiency is decreasing but isothermal power and indicated power increases and also other efficiencies like mechanical, overall efficiencies increases with increase of the pressure. It was observed this is same in both cases of single and multi stage compressor
5.5 Comparisons tables for single stage and multi stage compressors
Power input to compressor Pc = Pm x 0.8 Pc = 2.6019 x 0.8 = 2.0815 Kw
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Table: 5 -Comparisons table for single and
Table: 6 -Comparisons table for single and
multi stage compressor
multistage compressor
Tank Press ure
Volumetric Efficiency
Piso
2
Sin gle stag e 80.3
Sin gle stag e 0.20 9 0.32 6 0.35 9
4 6
IP
70.4 6 67.5 2
Mul ti stag e 82.9 81.9 2 81.5 9
Mult i stage
Singl e stage
Multi stage
0.41 21 0.94 15 1.15 85
0.30 2 0.37 96 0.42 3
0.451
Tank Pressure
ηmech
Pc
ηover
Single Multi stage stage
Single Multi Single Multi stage stage stage stage
2
1.327
1.684
22.75
26.8
20.27
24.47
4
1.384
1.947
27.41
56.1
23.5
48.3
6
1.5
2.0815 28.2
64.23 23.9
55.6
1.094 1.337
power to compressor 3
volumetric efficiency
2
100 Single stage
50
Multi stage
0 2
4 Tank pressure
1
Single stage
0
Multi stage 2
6
4
6
Tank pressure
Isothermal power
mechanical efficiency
1.5 1 0.5 0
100 50
Single stage 2
4
6
Single stage
0
Multi stage
2
4
Multi stage
6
Tank pressure
Tank pressure
Indicated power
overal efficiency 60
1.5 1 0.5 0
40 Single stage 2
4
6
Multi stage
20
Single stage
0
Multi stage 2
tankpressure
4
6
Tank pressure
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Table: 7 -Comparisons table for single and
multi stage compressor Tank Pressu re
Delivery temperatur e
ηiso Singl e stage
Mul ti stae
Singl e stage
2
89.0
91.1
109
4
85.8
125
6
84.8
86.0 6 86.6
136
RPM
Mu lti sta ge 88
Single stage
876
Mul ti stag e 928
13 1 15 7
872.2
923
869.3
917
multistage compressor having higher efficiency then the single stage compressor. REFERENCES [1] Internal combustion engines and Air pollution by professor (Dr.) R.Yadav Third revised edition –central publishing house 18C, Sarojini Naidu Marge-Allahabad-211001 [2]A Text book of internal combustion Engines (Including Air compressor, Gas turbines and Jet propulsions) Unit second Edition By R.K.Rajput published by Laxmi Publications Pvt Ltd 113, Golden house,Daryaganj,New Delhi-110002 [3] A Text book of Thermal Engineering by J.K Gupta and R.S.Khurmi
iso thermal efficiency 92 90 88 86 84 82 80
Single stage Multi stae 2
4
6
Tankpressure
6.0 CONCLUSIONS It was observed with increase of tank pressure isothermal power, indicated power mechanical efficiencies are increasing for both single and multistage compressors and also observed with increase of delivery pressure volumetric efficiency is reducing in both cases. As temperature of incoming air increasing, the density of air decreasing and volume of air sucked in to cylinder increases, it may be the reason because of less dense of air which may be entering in to the engine cylinder. On comparison of volumetric efficiency, isothermal power indicated power, mechanical efficiency; isothermal efficiencies are higher for multistage compressor then the single stage compressor with marginal rise of power input to the compressor. We may conclude for almost same equal power consumption ANVESHANA’S INTERNATIONAL JOURNAL OF RESEARCH IN ENGINEERING AND APPLIED SCIENCES
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