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8/18/2019 Twin Lobe Compressor
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INSTRUCTION MANUAL
FOR
TWIN LOBE COMPRESSOR
TEST RIG
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INTRODUCTON:
Compressed air is a source of storing mechanical energy. It is a reversible
procedure where work can be returned with small loss of energy in the form of
heat. A compressor is machine which takes air from atmosphere, compressor it
with aid of some mechanical energy & delivers it to storage vessel. The pressure of
air is increased by reducing volume compressed air then can be taken by pipe
wherever it is required.
APPLICATION:
a. In blast furnace, boiler furnace.
b. neumatic tools spray painting, sand blasting.
c. neumatic conveying of cement & grains.
d. In construction of large pro!ects, highway & tunnels.
e. "upercharging in IC #ngines & gas turbines.
f. neumatic brakes & clutches.
g. In air conditioning drying & ventilators
CLASSIFICATION:
A. RECIPROCATING TYPE:
In this type, successive volumes of air or gas are confirmed within closed space
where pressure is increased by reducing the volume characteri$ed for volumetric
capacity & large delivery pressure. %or larger pressure ratio, the compression is
carried out in multistaging with intercooler so that the compression process can be
made near to isothermal so as to minimi$e the work to supplied.
B. ROTATING TYPE:
In this type, air is trapped in the space formed by two manually emerging
surface.ue to which the volume in between surfaces reduces & ressure
increases.The rotary type compressor are characteri$ed by large volumetric
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capacity & relative low pressure .They are high running compressor. '((T",
)*(+#'", "*II-, C#T'I%-A* & A/IA* %*(+ C(0'#""('" are
rotary compressor.
WORKING OF TWIN LOBE COMPRESSOR:
%igure 12a3 shows Twin lobe compressor. There are two rotors, each having two
lobes, one rotor sets the drive from the motor & the other rotor is driven by the first
by gears e4ternal to the casing. The lobes rotor in opposite direction pressuri$ing
the gas .The lobes have well designed cyclical profiles to give perfect meshing &
leak proof seating between the high pressure space & the low pressure space at all
regular positions. A slight clearance between the meeting lobes avoids wear at
sealing surface.
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THEORY:
A volume 5s of the gas at the suction pressure p1 is trapped between the left hand
rotor & the casing, of shown in figure. This trapped volume of the gas does not
change its stage until this space is opened to the high pressure side. Instantly, some
high pressure gas from the receiver rushes back & mi4es irreversibly with the gas
in the blower until the pressure is equali$ed. The gas is then displaced in to the
receiver.
%igure 12b3 shows p6v diagram for roots blower. The flow gas in to the receiver is
not continuous despite the rotors at uniform speed.
+ork required to drive7 ∫1
2
Vap KJ /Cycle
There are 8 cycles per revolution in a Twin lobe compressor
+ork required to drive,
+9 85s 2p:6p13 ; n min
94Vs( p2− p1)×n
60 min.
8vs is the volume of air delivered per revolution.
As the ideal compression process is isentropic, work required for isentropic
compression is,
+i 9γ
γ −1 ; p1×4 Vsn
60 ;( p2 p1 )¿
¿¿
61?
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'oots #fficiency 9 Isentropic work required
ActualWork required
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B. 'otary ositive displacement compressors are engineered & manufactured by
capable & e4perienced personnel in a modem plant with the latest imported &
.0.T 0achines & also with latest toolings. roduction is controlled by close
Inspection, tests & attention to the smallest detail. 'eliable field service is
maintained by factory trained personnel. Compressor range in capacity up to
D,DDD 0@>hr. Eou are invited to request information on si$es not covered in this
bulletin.
'otary ositive displacement has two figures eight impellers rotating in opposite
direction. As each lobe of an impeller passes the compressor inlet, it traps a quality
of air equal to e4actly one6fourth the displacement of the compressor. This
entrapment occurs four times per revolution, moving the entrained air around the
case to the compressor outlet -round helical timing gears accurately position the
impellers in relation to each other, maintaining the minute clearances so vital to the
high volumetric efficiency of the rotary positive compressor. )ecause the
compressor operates with very close internal tolerances, a slight amount of air
escapes past the opening clearances back to the suction side of the compressor.
This leakage, defined as FslipF is predictable constant volume for any given
compressor at any given pressure. %or ease in calculation, this leakage is e4pressed
in compressor rpm. A standard slip, based on handling air at standard condition,
has been established for each compressor si$e. %or gases having a specific gravity
other than
1.D the slip will vary & this must be taken into consideration when calculating total
operating speed unit. Compressor is built with the closest possible tolerances to
give highest volumetric efficiency.
7. SPECIAL FEATURES OF ROTARY POSITIVE DISPLACEMENT
COMPRESSOR.
a. 0anufactured on imported machines with latest technology.
b. All rotating parts dynamically balanced.
c. Computeri$ed profile of the Impeller for higher efficiency.
d. elical ground gears for silent operation & longer compressor life.
e. eavy6duty roller bearing ensure :8 hour continuous trouble free operation.
f. Tested as per )ritish "tandard 1G1 art6II
g. 5ery low maintenance cost.
h.1DDH oil free air.
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8. CASING: ewly designed one piece style, including e4tra deep rib section for greater
rigidity under vaccum or pressure since. #very casing is hydraulically tested. In many
of internal inspection & clearance checks
IMPELLERS:
Are accurately machined for close tolerance operation, dynamically balanced for
smooth running & lower bearing loads. I.". -rade : is used in standard model however,
in higher speeds of compressors, forged>"o -. Iron material is used with integral shaft
arrangement.
TIMING GEARS:
Alloy steel, eat Treated, elical -round cut for greater strength & quieter
operation. elical -ears %itted with ad!ustable hub 2called locking device3 are mounted on
shaft for easy timing setting & easy in dismantling. o hydraulic !ack or any ammering
required ensuring longer life for )earings.
STEELSHAFT;
Are carefully machined & ground from Chrome Alloy "teel. The ground shafts are
fitted in impellers through interference fit which eliminates torsional deflections & permits
increased ratings & -reater efficiency.
BEARINGS:
Are eavy duty 'oller "pherical, double row, for ma4imum loading )earings are
held in machined bearing cartridges -ear & )earings are fi4ed a4ially against shaft
shoulder to control thrust loads & maintain end clearances.
LUBRICATION:
The basic units in the seriesF features trouble free splash lubrication of a Timing
-ears, -enerous si$e sumps are located in the -ear Case. The oil is poured in the gear
case & high temperature grease is poured in driver & driven cover. To prevent undedutcted
losses of lubricant, the series has been designed with visual indicator at oil end cover.
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SPECIFICATIONS:
The technical specifications of the test rig are as follows7
Comp!""o U#$%:
0odel T 6 8:
%abrication umber ::D1BJ
0anufacturing Eear7 :DDD
Tested on 18>D>:DDD.
%ree Air elivery :8.JJ m3/hr
+orking ressure D6@DDD mm of +C
'0 188D
MOTOR:
ower
'0 188D
5olts 88D5, @ , D $,
Type T#%C
COMPRESSOR TEST RIG:
The TestF 'ig Consists of Air Compressor with air suction tank, is fitted with an
orifice to determine the volume flow rate at the inlet side & pitot tube at outlet side
to measure pressure of compressed air. The e4it side of the compressor is
connected to reservoir. #nergy meter is used to record the power input to motor &
in turn the work required for compression. The control panel houses starter for
motor, main switch, Temperature Indicator.
PRECAUTIONS:
1. The reservoir cum air tank should be emptied before stating the compressor.
:. (rifice should not be blocked otherwise rubber sheet of Air tank will cut
drastically.
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A$m: To etermine 'oots #fficiency
APPARATUS:
"top +atch, Tachometer.
SPECIFICATIONS
0a4 elivery ressure @DDD mm of +C
ia. of (rifice 8D mm.
Coefficient discharge 2cd3 of surface D.B:
PROCEDURE:
1. ote down barometric pressure in mm of g & room temperature in Kc.
:. "tart the compressor.
@. After reaching stable pressure note down manometer reading in mm of water to
obtain intake air pressure.
8. ote down the pressure gauge manometer reading in mm of g to determine
outlet air pressure
. ote the time in sec required for 1D revolutions of energy meter.
G. 'epeat the same procedure @ 6 G for other desired pressure
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OBSERVATION TABLE:
S.
No
D!&$'!(
p!"")!
M*#om!%!
R!*+$#,
-mm
Comp!""o
"p!!+ /001
I#&!% A$
T!mp
-23
I#&!% A$
P!"")!
-B*
T$m! % -"!3
4o /1 R!' o4
E#!,( m!%!
H!*+ H* $#
m!%". o4
*$1.
:.
@.
8.
.
B.
G.
L.
J.
1D.
WORK RE5UIRED FOR ISENTROPIC COMPRESSION.
+i 9γ
γ −1 ; p1×4 Vsn
60 ;( p2 p1 )¿
¿¿
61?
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g9 J.L1 m>sec:
a9 #quivalent manometer head of air in meters.
a is calculated as7
Mw w9Ma a
Mw9 ensity of water
w90anometer head of water in mtrs.
Ma 9 ensity of air
Ma is calculated by using relation7
a5a 9 m'Ta
Ma 9 Pa
Ra
ressure from height of mercury is calculated as
9 mMmg
Mm 9 ensity of mercury
m 9 )arometer height of mercury in m
' 9 Characteristic air constant
Ta 9 Temperature of intake air Kk
The atmospheric pressure is calculated as
a90.760×13600×9.81
103
91D1.8
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ensity of air is now given as
9 Ra
Pa 9101.4×103
287×297 9 1.1LJB m@
The eight of Air is given as
a 9 !wHw
!a
910×123×10−3
1.1896
C*&3)&*%$o#:
* A3%)*& 6o o4 3omp!""$o#
+a95 2:613
+here,
595olume of air handled in cubic m>sec.
19 Atmospheric pressure in bar.
: 9 ischarge pressure in bar.
I"!#%op$3 6o o4 3omp!""$o#
+i 9
γ
γ −1 ;
p1×V
;
( p2 p1 )¿¿¿
61? "
3 Roo%" E44$3$!#3( 9 Isentropic work required
ActualWork required
+a9
4Vs×n
60 ; 2:613
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94×0.0672×1404
60 ; 21.@613
9 1.LL