Report OEMO 96/ OL
D. Pace
Delft/Zoetermeer
January 1996
:4#4,
T U Delft
Delft 'University of Technology'Faculty of Mechanical Engineering and Marine Technology Department of Marine Technology
van Buuren -van Swaay
_
Van Buuren - Van Swaay Zoetermeer
Measurements on
a refrigeration
system
Faulty Behaviour PART II
TU Delft
measurements on a refrigeration systemam=
INTRODUCTION 3
REFRIGERATION PROCESS 4
2.1. GENERAL WORKING OF A REFRIGERATION SYSTEM 4
2.2. A SHORT DESCRIPTION OF THE USED REFRIGERATION SYSTEM 5
PLACEMENT OF SENSORS AND SENSOR INFORMATION 8
3.1. SENSOR LOCATIONS 8
3.2. SENSOR PARAMETERS, SPECIFICATIONS AND DATATRANSFORMATION 8
MEASUREMENT PROGRAM 15
4.1. CHOICE OF CONDITIONS AND FAULTS 15
4.2. LOCATION OF THE DIFFERENT BYPASS PIPING AND VALVES 16
ACTUAL MEASUREMENTS 18
5.1. POST PROCESSING OF THE MEASURED DATA 18
5.1.1. Pressure measurements 18
5.1.2. Temperature measurements 18
5.1.3. Calculation of the freon flow 19
5.1.4. Measurement faults 5.2. MEASUREMENTS ON 07 - 09 - 1995 21 5.3. MEASUREMENTS ON 14 - 09 - 1995 5.4. MEASUREMENTS ON 18 - 09 - 1995 5.5. MEASUREMENTS ON 21 -09-1995 54 5.6. MEASUREMENTS ON 22 - 09 - 1995 65 5.7. MEASUREMENTS ON 25 - 09 - 1995 75
DATA ANALISYS ANDCONCLUSION
AppendixA: measurements log-book 98
Appendix B: derived graphs 114
paa. 1
20
32 42
TU Delft
Subscripts
discharge (in combination with compressor variables) env environmental variable
inlet, interior dimension mass
outlet
suction (in combination with compressor variables sub sub-cooling
sup superheat compressor
chw chilled water (cold water) cond condenser
crk crank
crkc crankcase icy/ cooling water
cyl cylinder cylw cylinder wall
fd filter/dryer element oil oil pi piping pist piston refrigerant tu tube ev evaporator exp expansion valve
Indices
(i) flow m3/h, kg/s p pressure N/m2 P power W T temperature (abs) K t temperature (rel) ocmeasurements on a refrigeration system van Buuren -van &nay
TU Delft
1.
Introduction
This measurement report is the second result of a measurement program, done under the
ICMOS-CRP research program'
of the faculty of Mechanical Engineering and Maritime Technology,
Technical University of Delft.The measurements were done on a refrigeration system located at Van Buuren - Van Swaay b.v. Zoetermeer. The goal of the measurement program is twofold. The first goal is to provide data for
tuning and validating the mathematical model of a refrigeration system developed by Grimmelius. The second goal is to provide training and testing data for a diagnosis system build by van Kuilenburg and
Grimmelius. To capture the whole working range of the refrigeration system, all the faults are
introduced at four different working points of the refrigeration system. These four points span theentire working range of the refrigeration system.
This report contains the second set of measurements, following those performed by van Kuilemburg and Grimmelius in June '95. The data is presented graphically and then analysed.
In the second chapter, a short description of the refrigeration process and real refrigeration system is
given. The third chapter describes the measurement equipment such as sensors and processing
equipment. Chapter four depicts the measurement program. Chapter five contains the recorded dataper measurement day for each introduced fault individually. The last chapter analyses and discusses the symptoms and system behaviour.
The different partners in this project are Van Buuren - Van Swaay and theTU-Delft2 The measurements were completed by D. Pace and H.T. Grimmelius.
I wish to thank the following people for their assistance and help during the measurements : H.T. Grimmelius TU-Delft
R. F. van Kuilemburg, TU-Delft
G. Been, Van Buuren - Van Swaay
M. van Will igen, Van I3uuren - Van Swaay R. Houtenbos, Van Buuren - Van Swaay
Dandolo Pace 08-01-1996
measurements on a refrigeration system van Buuren -van Swaay
ICMOS - CRP = Intelligent Control and Monitoring Systems - Compressor Refrigeration System
2 TU-Delft = Technical University of Delft
pag. 3
TU Delft
2.
Refrigeration process
In this chapter the theoretical basis is treated of the refrigeration process. Also the real refrigeration system layout is given together with the data of the different parts of the refrigeration system
2.1.
General working of a refrigeration system
A refrigeration plant has the following basic system scheme and basic components :
fw
Q2
figure 2-1, basic scheme of a refrigeration system
The whole purpose of a refrigeration system is to transport energy(Q2) from a relative low
temperature level to a relative high temperature level (Q1). The compressor (1) compresses the freon which comes from the evaporator (4). To compress the freon an amount of energy is needed (W), this energy causes an increase of the enthalpy of the freon. At this high pressure the (still) gaseous freon iscondensed in the condenser, releasing energy (Q1) to a cooling medium at a relatively high
temperature level. Now the pressure of the freon is adiabatically decreased in the choking device (3). At this low pressure the freon is evaporated in the evaporator (4) at a relatively low temperature level. The transportation of this energy costs energy due to mechanical losses in the various components and thermodynamic losses.measurements on a refrigeration system
1 1. Compressor
Condenser Choking device
Evaporator
van Buuren -van Swaay
pag. 4
TU Delft
It is custom to plot the process in a log(p) - h diagram of the refrigerant fluid measurements on a refrigeration system
enthalpy h 1.1/kg'
)
overheating
figure 2-2, refrigeration process plottedMaschematic log(p) - h diagram of freon-22
In this diagram the coexistent area of the cooling medium is drawn. After compression (1) the gas is
superheated. In the condenser (2) the gas is first cooled to a saturated gas and then condensed to
liquid. Often the temperature (energy) of the gas is lowered beyond the point where just all thegas
has become liquid. This is done to prevent the liquefied gas to evaporate before it reaches the
evaporator due to pressure losses in the pipes or height differences. This is called "under-cooling" ofthe gas. After the choking-valve the gas is evaporated (4). The temperature of the gas is more
increased then absolutely necessary, to ensure that only gas reaches the compressor. If liquid reachesthe compressor, the compressor can brake down (liquid is hard to compress). The extra temperature
increase of the gas is called "super-heating".
A log(p) - h diagram of R22 (freon) is given in appendix A
2.2.
A short description of the used refrigeration system3
The installation is a cold water maker, used for cooling the research rooms at Van Buuren - Van Swaay. For this investigation the system is coupled to a re-heater, in order to simulate the desired
workloads for the refrigeration system. The installation
is filled with freon R22, with a lowest
temperature of -1 °C. This implies that the pressure in the installation is at least 4.5 bar (abs). The
condenser is cooled with normal water, of which the flow can be controlled by a valve.
3 See for a detailed description of the refrigerationsystem' van der Heiden. OEMO 94/12
van Buuren -van Swaay
pai4. 5
Installation specifications
Electrical power : 14 kW
Cooling capacity : 80 kW Coldwater temp : 3.5 - 9 °C Cooling water temp 20 - 35 °C Amount of freon : 12.4 kg
:
TU Delft
measurements on a refrigeration system van Buuren -van Swaay coldwater filter (empty) water cooling Pi. compressor Control measurements Spy-glass filter/dryer L_J expansion valvefigure 2.3 real refrigeration system, used for generating the data
condensor
pag. 6
ievaporator
21-"U
Delft
measurements on a refrigeration system van Buuren -van SwaayTI! Delft
3.
Placement of sensors and
sensor information
In this chapter the location and
specifications of the sensors is given. Information about dataprocessing equipment and the transformation of the data is given.
3.1.
Sensor locations
The sensors are placed according to figure 3.1. These locations are similar with the actual placement of the sensors on the system.
measurements on a refrigeration system
T1 1 k,a9) P6 rrio-s\ 72
->v<-figure 3-1, placement of the sensors on the refrigeration system
3.2.
Sensor parameters, specifications and data transformation
In the following tables, the specifications and parameters of the used sensors are given. The
transformation of the signal in the data-loggers (if used) can also be found in this tables. The signalsare collected in two different data-loggers (due to some practical problems,
two are used). The
NETDAQ 2645A and the HYDRA 2625A, both manufactured by Fluke. For more details about the
data-loggers see appendix B. In figure 3.2 the path is visualised, the signals follow before they are
saved on disk.
07(
van Buuren -van Swaay
P4
><1
TU Delft
synchronisation puts
measurements on a refrigeration system
netdaa
hydra
sensors
figure 3-2, signal path from sensor to disk
The two data-loggers are coupled by means of a synchronisation pulse generated in the Hydra. The sample interval is 9 sec. A external synchronisation pulse is used for creating a common signal on
both loggers. This synchronisation signal is used in two ways. It is used in combining the two separate data-files into one and it marks the beginning and end of a fault simulation.
The software of the NETDAQ is running under the standard Windows interface. For the control of the
Hydra a custom program is used developed at Van Buuren van Swaay. This program runs under
CONCURRENT DOS.
saving computer 1
dalatranstormation visualisation
van Buuren -van &pay
pag. 9
Sensor RI'
Parameter NI , Oil pressure
Description Compressor oil pressure, T-pipe and schrader
in + pipe oil pressure safety
Sensor type E&H Cerabar PMC 133 0/16 bar ; 24V DC
Signal 4-20 mA
Data-logger Netdaq 2645A (Fluke)
Channel number 101
Data transformation
-Remarks
-Sensor 13.2
Parameter PC,, Suction pressure
Description Suction pressure compressor, 1/2" flare schrader
on surface suction pipe closing valve
Sensor type B&H 10 bar
Signal 0-10 V
Data-logger Netdaq 2645A (Fluke)
Channel number 106 Data transformation Remarks -sensors datalransformation visualisation inggerPuis saving computer 2
TU Delft
measurements on a refrigeration system van Buuren -van Swaaypag. 10
Sensor P3
Parameter ped , discharge pressure compressor
Description Compressor discharge pressure, 1/4" flare schrader on surface outlet pipe closing valve
Sensor type E&H Cerabar PMC 133
0/20 bar ; 24V DC
Signal 4-20 mA
Data-logger Netdaq 2645A (Fluke)
Channel number 103
Data transformation
-Remarks
Sensor P4
Parameter peon& . pressure after condenser
Description Condenser liquid out T-piece and schrader on connection for the water control valve
Sensor type B&H 20 bar
Signal 0 - 10 V
Datalogger Netdaq 2645A (Fluke)
Channel number 107
Data transformation
Remarks
-Sensor PS
Parameter pew, , pressure before expansion valve
Description Liquid before expansion valve, additional 1/4" flare schrader on liquid pipe
Sensor type B&H 20 bar
Signal 0 - 1 0 V
Datalogger Netdaq 2645A (Fluke)
Channel number 105
Data transformation
Remarks
Sensor P6
Parameter
p; ,
pressure before evaporatorDescription Inlet pressure evaporator, additional 1/4" flare schrader on pipe
Sensor type B&H 10 bar
Signal 0 - 10 V
Data-logger Netdaq 2645A (Fluke)
Channel number 104 Data transformation Remarks -1
TU Delft
measurements on a refrigeration systemCI=
pag. II
Sensor P7
Parameter peric , carter pressure
Description Cater pressure, 1-pipe and schraderon connection of oil pressure safety
Sensor type E&H Cerabar PMC 133
0- 16 bar ; 24V DC
Signal 4 - 20 mA
Data-logger Netdaq 2645A (Fluke)
Channel number 102
Data transformation .Remarks
Sensor TO
Parameter t, room temperature
Description Room temperature
Sensor type Cu - Const insertion sensor (1.5 mm)
Signal TK
Data-logger Hydra 2625A (Fluke)
Channel number 5
Data transformation function = Type T thermocouple
Sensor TI
Parameter toil , oil temperature
Description Oil temperature Carter, tight coupling on relief valve
Sensor type Cu - Const insertion sensor (1.5 mm)
Signal TK
Data-logger Hydra 2625A (Fluke)
Channel number 6
1 Data transformation function = Type T thermocouple
Remarks
-Sensor T`")
Parameter tc suction temperature (freon) compressor Description Suction temperature freon gas, tight coupling
on plate burn out filter
Sensor type Cu - Const insertion sensor (1.5mm)
Signal TIC
Data-logger Hydra 2625A (Fluke)
Channel number 7
Data transformation function = Type T thermocouple
Remarks _ Remarks -1
TU Delft
measurements on a refrigeration system van Buuren-van Swaypag. 12
Sensor T3
Parameter t,d, outlet temperature (freon) compressor
Description Outlet temperature, surface sensor on pipe
Sensor type NiCr - Ni surface sensor
Signal TK
Data-logger Hydra 2625A (Fluke)
Channel number 8
Data transformation function = Type K thermocouple
Remarks.
-Sensor T4
Parameter teondo , temperature freon after condenser Description Liquid temperature after condenser, surface
sensor on pipe
Sensor type NiCr - Ni surface sensor
Signal TK
Data-logger Hydra 2625A (Fluke)
Channel number 9
Data transformation function Type K Thermocouple
Remarks
Sensor 15
Parameter tap, , temperature freon before expansion valve Description Liquid temperature before expansion valve,
surface sensor on pipe
Sensor type NiCr - Ni surface sensor
Signal TK
Data-logger Hydra 2625A (Fluke)
Channel number 10
Data transformation function = Type K thermocouple Remarks
Sensor T6
Parameter tts, , temperature freon before evaporator
Description Liquid - Gas temperature at the entrance of
evaporator
Sensor type NiCr - Ni surface sensor
Signal TK
Data-logger Hydra 2625A (Fluke)
Channel number 15
Data transformation function = Type K thermocouple
Remarks
-I
=
pag.
'Sensor _ 17
Parameter temperature inside Carter
Description Cartertemperature,tight coupling on blind nut
Carter
Sensortype Cu- Constinsertionsensor(1.5 mm
-Signal TK
Data-logger Hydra2625A (Fluke)
Channelnumber 16
Data transformation function=Type T thermocouple
Remarks
Sensor T8
Parameter , inlettemperaturecooling water
Description Inlet temperaturecooling water .Sensor type PT - 100 insertionsensor
Signal PT 100
Data-logger Hydra2625A (Fluke)
Channel number 1 ,
Data transformation function=4 terminalRTD , RID RO =100
Remarks
-Sensor 19
Parameter tcwo , outlettemperaturecooling water
Description Cooling water outlettemperature
Sensor type PT - 100 insertion sensor
Signal PT 100
Data-logger Hydra2625A (Fluke)
"Channel number 2
Data transformation function=4 terminal RID, RTD RO = 100
Remarks
-Sensor TIO ,
Parameter tch,,,i , inlettemperaturecold water
-Description Cold water inlettemperature
Sensor type PT - 100 insertionsensor+ F25
Signal RS232
Data-logger Hydra2625A (Fluke)
Channel number 3
Data transformation, function =4 terminal RTD, RID RD = i100
Remarks.
Sensor Till
Parameter thw, , outlettemperature coldwater
Description Cold water inlet temperature
Sensor type PT - 100insertion sensor+ F25
Signal RS 232
Data-logger Hydra2625A (Fluke)
Channel number 4
Data transformation function =4 terminalRID, RID RO = 100
Remarks
TU Delft
measurements Joni a refrigeration system vanBuuren -vanSway.13
-TU Delft
measurements on a refrigeration system van Buuren -van Swam(pag. 14
Sensor Fl
Parameter flow freon
Description Flow freon (R22), Venturi in elongated pipe. Valve after Venturi !
Sensor type Tekflo Venturi VN20 + AP transmitter
range 0-3 mwk
Signal 0 -20 mA
Data-logger Netdaq 2645A (Fluke)
Channel number 108
Data transformation
-,Remarks
-Sensor F2
Parameter w, flow cooling water
Description Flow cooling water, E&H Discomag in pipe
Sensor type E&H Discomag
range 0 - 6 ml/h
Signal 4-20 mA
Data-logger Hydra 2625A (Fluke)
Channel number 17
Data transformation function = VDC 300 mV Range Scale Factor = 0.0375
Offset Remarks
Sensor F3
Parameter lid,,,,, flow cold water
Description Flow cold water, F&P in workload simulator
Sensor type F&P
range 0 - 30 in3/h 4 -20 mA
Signal
Data-logger Hydra 2625A (Fluke)
Channel number 18
Data transformation function = VDC 300 mV Range Scale Factor = 0.0001875
Offset = -0.0075, data signal * 1000 in comp Remarks
Sensor El
Parameter compressor electrical power
Description Electrical power compressor engine Electrical wiring on power net
Sensor type power sensor
0 - 100 kW
Signal 0 - 100 mA
Data-logger Netdaq 2645A (Fluke)
Channel number 109 Data transformation Remarks , I I I'-I
TU Delft
measurements on a refrigeration system4.
Measurement program
In this chapter the measurement program is explained
4.1.
Choice of conditions and faults
The aim of the measurement program is to cover as much as possible the whole working ranged of the
refrigeration system while introducing the different faults. Therefore the choice has been made to introduce the faults at four different working points of the system. These working points are chosen
such that most of the working range of the compressor is covered. The following conditions have been chosen :
C=I=
In table 4.2 the different simulated faults are given. These faults could easily introduced, with only
simple modifications on the refrigeration system.
'for detailed measurements over the whole working range, see van der Heiden OEMO 94/12
A,B,C,D = working point of system, 1..40 is a unique measurement number
pag. 15
Code tend Pond Omcw Ochw Tcondicw Tevichw
A
3°C
40°C
15.32 bar 2.02 m3ih 11.1 ml/h 13.1°C I 1.8 °CB
9°C
40°C
15.32 bar 2.60 m3/h 11.2 mi/h 13.2°C20.5°C
C 9 °C 45 °C 17.30 bar 2.02 m3/h 11.2 m3fh 13.3 °C 19.2 °C
D
3°C
45°C
17.20bar 1.62 m3/h 11.2 m3/h 13.5°C 11.0°Cfault number Place Fault Action Codes
Compressor 1 suction side increased resistance suction line valve Al, BI8
C28, D12
/
discharge side increased resistance discharge line valveA2, BI9
C29, D13
1 power main one phase
disconnected
removal of one phase
B44
Condenser 4 water side too much cooling
water
water supply A3, B20 C33, D14
5 water side too little cooling
water
water supply A40, B21 C34, D15 Liquid line
Expansion valve
6 liquid line increased resistance liquid line valve A5, B22 C32, D37
7 valve no pressure
correction
close press. corr. line
A4 I, B26 C36. D10
8 valve stuck open bypass
valve
A8, B25 C35, D39
Evaporator refrigerant side leakage over
evaporator
by-pass A7, B24
C31, D11
10 water side increased resistance water control valve A6, B23 C30, D38 ' I I I -9
TU Delft
measurements on a refrigeration system 4.2.Location of the different bypass piping and valves
In figure 4.1 the location of the different valves which are used to simulate the different faults is
given. The dotted lines give the extra valves and piping which are installed to simulate several faults. These are not part of the original refrigeration system, but are specially installed for this measurement program. The code of each location corresponds with the numbers given in table 4.2. The automatic flow control of the cooling water has been shut off during the measurements.
F3
F 8
figure 4-1 locations where the different faults are introduced
;
F6
van Buuren -van Swaay
TO Delft
measurements on a refrigeration system van Buuren -van SwaayTU Delft
5.
Actual measurements
In this chapter (which is the main body of the report) the actual results of the measurements are given.
First general data is given such as initial values, correction factors and the formulas used in the
calculations. After this the measurements are given in a graphical way (looking at 10,000 numbers can be very boring).
5.1.
Post processing of the measured data
5.1.1. Pressure measurements
When a refrigeration system has been opened, the system must be tested afterwards for leaks. This
system has been tested at a pressure of 10 bar for about 24 hours. It is clear that all pressure sensors must give a reading of 10 bar when the system is tested. This procedure of testing gives a handy tool
for checking the pressure sensors. In table 5.1 the actual readings are given of the sensors and the
correction factors derived from it. These correction factors ensure that all the sensors give the same relative reading.
5.1.2. Temperature measurements
For this experiment these are not extra calibrated.
measurements on a refrigeration system van Buuren -van Swaay
pag. 18
Channel Parameter Value at testing Correction
factor
Value at testing 0 bar
101 Oil pressure compressor 9.96 bar +0.04 bar 0.04
102 Carter pressure 9.89 bar +0.11 bar -0.03
103 Outlet pressure compressor 9.99 bar +0.01 bar -0.03
104 Pressure before evaporator 9.95 bar +0.05 bar -3 10-3
105 Pressure before expansion valve 9.95 bar +0.05 bar 2 10-3
106 Suction pressure compressor 9.89 bar +0.11 bar 3 10-1 1
TU Delft
5.1.3. Calculation of the freon flow
The freon flow through the system is measured by a Venturi in the connection between the condenser
and the expansion valve. The Venturi transforms the velocity of the water to a pressure difference.
This pressure difference can be measured and transformed in a velocity of the freon. The Venturi has been calibrated with water and must be re-calculated for the use of freon.
According to Bernoulli6 the following relation is valid
Amin
41:1freon = .\I V2. pfreco (PI
10
Amm2
1 2
measurements on a refrigeration system
PI PI
figure 5-1, Venturi Finally the following formula emerges for calculating the freon flow :
42.75
(I)freo P P2 VPireon kgis
n 3600
For the calculation of the specific mass of freon the following formula is used
for more information see : Stroming en Warmteoverdracht I, Jr. FL Leidens, TU-Delfl
van Buuren -van Swaay
The pressure signal has a bias, this bias is calculated by looking at the signal while the installation is not running.
Warning : In many cases the flow measurement is very inaccurate because of the occurrence of
bubbles in the fluid. These bubbles ruin the flow measurement. The occurrence of bubbles is given in the measurements.
pag. 19
Channel Parameter Value at testing Correction factor
108 mass flow freon -0.73188 0.71388
log(1 / p)= pc, + 13 log(P) +132p +133P' 13.0 = 3.11554
131 = 4.1444 10_2
132= 3.1469 10
133 = 2.4704 10 -7=
6TU Delft
measurements on a refrigeration system For the calculation of the constant in the formula the following method is used.The enthalpy of the freon at the outlet of the condenser and the enthalpy at the outlet of the evaporator
are compared with each
other. This gives a increase of enthalpy of the freon per kg over the
evaporator. Also the decrease of the enthalpy of the cold water is calculated over the evaporator.
Since the flow of the cold water is known, the flow of the freon can be easily calculated from a energy balance over the evaporator.
This is done for four differentpoints.
corr factor = ,(1) f"" 3600
Ap
5.1.4. Measurement faults
A wrong measured signal will be given the value of -1
pag. 20 Measurement number day 23-06-1995 A tow,
.c
4)chw m3711 Pwater kg/m3Specific heat water kJ/kg Cooling power UR 100 3.6 11.1 998 4.18 46.3052 200 4 11.2 998 4.18 51.9137 700 4.8 11.2 998 4.18 62.2964 850 3.2 11.2 998 4.18 41.5309 Measurement number Pcondo bar tcondo °C Pei bar tcl °C licondo kJ/kg HQ kJ/kg Flow freon kg/s corr factor 100 15.50 38.90 5.46 11.20 248.58 411.57 0.284 42.539 200 15.83 39.50 5.75 14.50 250.12 414.72 0.315 44.944 700 17.28 43.30 6.71 19.20 254.69 416.63 0.384 46.176 850 17.41 42.40 5.66 11.90 254.48 413.05 0.261 38.779 I I I I
TU Delft
5.2.
Measurements on 07 - 09 - 1995
measurements on a refrigeration system
CS=
For detailed information about the measurements on day 07-09-1995 see appendix A row numbers are the row number in the excel sheet, not the row numbers of the Ascii files !
nag. 21
Filenames ic07tin.xls Excel 5.0 worksheet
ic07fin.txt ASCII (spaces as delimiters)
Begin time 11:42:32
End time 16:33:05
Number of measurements
1596
Measured condition A (12:05 until 12:19) 135- 225 healthy condition A B (13:37 until 14:56) 750 - 935 healthy condition B C (15:47: until 16:03:) 1270- 1382 healthy condition C D (16:16 until 16:36) 1460- 1600 healthy condition D I
cr) 15 a) '5 a)
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time Hydratemperature cooling water in
temperature Cooling water out
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1000 1200 1400 1600 1800 400 600measurement number daa
07-09-95 1 1600 1 1 1 1000 1200 1400 1600 1800 1800 CI CL. 1000 1200 1400 3 40 a) 30 a) a) I
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°
105
E 10 0 200 400 600 800 1000 1200 1400 1600 1800measurement number ciao 07-09-95
200 400 600 800 1000 1200 1400 1600 1800 0 ;40 a) .-I I
-1 in '20 15 10 16 10 0 200 _ _ 400
synchronisation signal Hydra
_-J 1
600
800 time netdaq pressure crankCase 1000 1200 200 400 600 800 1000 1200measurement number daa 07-09-95
_ 1400 1600 1800 f` I ta.) CL
.
-.
-1 ei
_ J .. I -e7
_L
____Ii j6
L. f i -1TM
L
4 Zre-_ 1400 1600 1800 200 400 600 800 1000 1200 1400 1600 8 -5 180020
15
10
8
pressure discharge compressor
pressure evaporator in pressure oil W.)
11
1 1 1 1 I i 1 1 1 I 1 1 1 1 rviVr...,-,...r-I 1 1 1 I i . r L 1 i i i .-t!
---I_
11 I -I' I I I I I. 1 I i r I I 1 Ir
I -1 I I,
r r I 4 I I I 1 I 1 I I I r 1 I I ri I I I F I 4 1 i-i,
I I I I I I i I I i I I i i 1 1 L I J I I I 1 i I I 1 I i 1 1 1 i TI i 1r
I 0 200 400 600 800 1000 1200 1400 1600 1800measurement number daa 07-09-95
200 400 600 800 1000 1200 1400 1600 1800 200 400 600 800 1000 1200 1400 1600 1800 12 10 8 6 00 0-I I I I
0 tt .r. 22 co 0 w 44-7
a
D
20 15 10 Bi 20 15 200 200 400 400 600 600 800 800Epressure expansion valve in
pressure compressor in
pressure contlensor out
1000 1200 1000 1200 200 400 600 800 1000 1200'
measurement number daa 07-09-95
1400 1400 1400 1600 1600 1600 1800 1800 1800 -, I-_ _ ... i
\_,Lr.7,.,
1r
I 1 I' i _ .1 -I i J II_ I I m _.---,_ -I er w - t,r. -I i, ,
=r, , , r -.. I I_ _. 17
_ _ i I l i I I 1 L -Jt
I 4 I I I. -I 1 I I I I I I I0 rn 0 0 £
iS
10 20 15 10 -200 400 600pressure difference flow freon
power
synchronisation signal netdaq
800 1000 0 200 400 600 800 1000 1200 1400
measurement number dao 07-09-95
1200 1400 1 L 1600 _
-1600 1800 1800 1 . I -/ -i entti/4401444 I I 40"r4i. F = I / i I iincc,....--,,-,---; --: i?, I IT.
. _-t
ii. _ . _ r.,=_ 4 rii
' L _ 4,
, , 1 0.5 ?;', 1 -11 Cr: D. =0.5 200 400 600 800 1000 1200 1400 1600 18000
5 .4pressure difference correcteu
800
specific mass freoni
800 flow freon 1000 1000 1200 1200 1400 1400 1600 1600 1800' 1800
MASNY \ 0644
, I -1--IMe
II
r thitt1060A. 1 -,., ---1 I I--_ -e. z t____ t - --, 1 . . 1 Ii
T _ -r -__ I-1
i I I I I 1 i IAipottriwittilin
1 , ;1IT
J i IL 1 7:-1r
--. r 1 1 4 I 200 400 600 800 1000 1200 1400 1600 1800measurement number daa 07-09-95
1100 1050 cn 1000o 0 r C.-I I I I-I I I I
4/ .f
TU Delft
Measurements on 14 - 09 - 1995
measurements on a refrigeration system van Buuren -van S),vaay
For detailed information about the measurements on day 14-09-1995 see appendix A
row numbers are the row number in the excel sheet, not the row numbers of the ASCII files !
pag. 32
Filenames ic14fin. x Is Excel 5.0 worksheet
ic I 4 tin.tort ASCII (spaces as delimiters)
Begin time 13:03:05
End time 16:17:20
Number of measurements 1301
Measured faults C 11(13:50 until 14:35) Too little refrigerant (condenser):
319-619 extraction of 3.05 kg freon
C 10(14:49 until 15:45) Too much refrigerant (condenser): 718 - 973 injection of 2.00 kg freon
A 10(15:45 until 16:17) Too much refrigerant (condenser): 1086-1301 extraction of 2.00 kg freon
715 16 14 7 17
165
(-5 16 (/) 15 5 Z:-y) a) 15 0 40 a) 30 1 500 500 alea". I or._i.temperature cooling water in
temperature cooling water out
:
1000
1000
500
1000
measurement number daa 14-09-95
1500 1500 1500
t--- t--- r li it
I Thl A ____ _ _ 0 .J
r
ao>" 4-,C(1) 20 a) 8 6 0 25 24
i23
0 If) a) 22 ci) 21 73 0temperature chilled water in
temperature chilled water out
temperature environment r4-1 t.or) Ca_ I , , , , , i , , , : 1
-i , : - :-. ,,
1 i,
L 1 1 r i I, l'-. I i I I, 1 I I I I I, . -,._1,..nes° 1 i i I 0 (3)4" If) 7 C12 0 500 1000 1500measurement number daa I-1-09-95
500 1000 1500 16 14 12 10 500 1000 1500 10 a)
50 u) 49 75 48 0 En Cl) 47 a) 20 90 crr 500
temperature oil
MW-inkyvyts_r?"temperature compressor in
temperature compressor out
1000
500
1000
measurement number daa 14
-09-95 1500 1500 I
-I I I I I -I I I I 1 a ii-i 1 1 i 1 I L I I 1 I i 1 I i I i 0 500 1000 1500 Cl)45
45
10
temperature condensor out
temperature expansion valve in
temperature evaporator in
500
1000
measurement number daa 14 -09-95
1500 It 1 " 1 i \.... I e IL i il-! . -I
7
, . , , , : --, , 1 _,---^..._____F"
, , L , , , , i , , , , , , I 500 1000 1500 500 1000 1500 3500
U) a) I20
15 10 5 0 16 14 0 (13 ID 4 5 0Syllent Of lisation Signal nyth
time netdaq
pressure crankcase
500
1000
measurement number daa 1-1 -09-95
1500 :- II-1 1 : i I 1 1 I 1 i_ r I--, L 500 1000 1500 0 500 1000 1500 6.5 6 (7) 5 5 RI 5 a) E 10 0 1
-19 18 17 7 6.5 6 11 10 9 na3 5 5 Lc6
.05
0 500 pressure oilpressure evaporator in
1000 500 1000measurement number daa 14 -09-95
1500 1 500 -1 ,
7-, , _ _ ---L_ , ,_ -_--
---, , ----I 1 I , : , I 1 110 I L L ' j i I 1 1 ! ' I , ir
, 1 1 1 i _ : : 500 1000 1500 018 17 8 7 18 17
515
pressure expansion valve in
pressure compressor in
pressure condensor out
(.2 14
0
500
1000
measurement number daa
14 -09-95 1500
Id,
..:r
-_
_ _ t"CMISS4C.P.V.A.N.
_ t-_ 1 = w ---.7---S. -_ ---_rat
1 I . A I- -= 7. I -4-LRAMMANUAIV, -- 1_ i -_ -,_ -..-- t 1_,.tT "" if' _vY \freiL mv L- yi -7, rvyr ,,_ .-- ,, - -. , - , . , . , 500 1000 1500 500 1000 15000.5
0
15
10
5
pressure difference flow freon
power
synchronisation signal netaaq
SY 1
a a ,,
m- .- .. -k-. -- , --, ,7 = -..- -IN-, . _ r I _-r
-1 1 I 11
7 03 ro E =0.5 -1 0 500 1000 1500measurement number daa 14 -09-95
-500 1 000 1500' 500 1000 1500 20 15 10
a-vs
02 1.5 1 0 5 1040 1030 1020 1010
-21000
0.5 500ebbui e UITTel et lee UM leGlCU
specific mass freon
flow freon 14-09-95 1000 1500 ca r 500 1000 1500 500 1000 1500 0 1 -I
TU Delft
Measurements on 18 -
09 - 1995measurements on a refrigeration system van Suuren -van Swaay
For detailed information about the measurements on day 18-09-1995 see appendix A row numbers are the row number in the excel sheet, not the rownumbers of theASCII files!
pag. 42
Filenames icl8fin.xls Excel 5.0 worksheet
icl8fin.txt ASCII (spaces as delimiters)
Begin time 11:51:59:
End time 12:53:47
Number of measurements 418
Measured faults C 12(11:51 until 12:09)
019- 127
condenser water side fouling
A 12 (12:30 until 12:53)
280 - 418
40 r, 50 100 T ; -1 ;_ : . I; , , , , ,
;,
, , , , , 1 -:. IL-.4 I,-_.: I I I I t I I 1 i 1 I Ir rI I 7 I TI 1 I I i I I I I I I time Hydra 111
t al si 10o 17 16.5 (7) 16 CT) win 15 5 a) a) 15 D 50 100 0 50 100 i , , , jr -, I 7 : 1: I I I I I 1 I I I I I 250 300 350 400 450 500 150 200temperature cooling water out
-I I II I 7 7 1 I : 7 i I
II
I II 1 I I I t I I I I I 1 L. I li 1 1 1 i i I I 1 II1
i I 1 : I t t T 1 r 1 T I i i 1 I 1 150 200 250 300 350 400 450 500measurement number daa
1 -9-95 150 200 250 300 350 400
450
500temperature cooling water in
12
11, 5
I
,2 151
cn Et2 10 a) a) 1:3 0 16 140 12
co a) 6-1:2 0 24 50 100, 100 150temperature chilled water in
temperature chilled water out
4 , = 200 250
temperature environment
I _ I 180 200 250 300 350 23 (11J
a)0 22
a) 22 (3) a) 21 50 100 150 200 250 300 350measurement number dag 18-09-95
400 450 500 - 11-1 -- -- t w L, I
If
1 400 450 500 300 350 400 450 500 20 10 50 I I I I I L 050
20
90 I I Iw85
1 D I 6 I I a) 1 1 c.) I I . i'80
a) I 1.1 i.1:12 I I 0) I I a) -c) 0 50 10011--- 11-
---50 100 I 14--I : 4: \i \r N Ill I I I 1, I I I I-I I I 11 . 1 I I I I I I 1 s I I 11_I
I 1. 1 11 1 1 i 1 ,... i *--- 1 __.--,-,i_
1 1 1 $ --"---,14.,-^-, 1 ______ -: ______ it- _________ I. III
1 I I 150 200 250 300 350 400 450 500 -A temperature oiltemperature compressor in
0 50 100 150 200 250 300 350 400 450 500temperature compressor out
4
measurement number daa
-09-95 150 200 250 300 350 400 450 500 48 I 1 1== -I
If) a) 45 (D 35 7' 0
45r
1-- 1 10 , 50 100 50 100 50 100temperature condensor out
, , , ,
,,
I , , ,I,
, . _,I , 1,
.._ : :-150 200 250 300 350 400 450 500temperature expansion valve in
1 . , . . , , , . , . , . , , , , . . . , , . . ; , ,_ , :-.4 , , , , , , , , , , , , , , , , , . 1 I I 1 I 150 200 250 300 350 400 450 500
temperature evaporator in
i 1 . I , 1 , I , I ! : : 41 1-4. I i i I I I I I I I I I I I I I I I I I I I I I I I I I I I I I -r 4 TI I I I : I Ir -I, II1
i I I III
I I I 1_L
L I I 1 I i 150 200 250 300 350 400measurement number ciao ix -09-95
450 500 -35 0
-
---0 52 (i) 51 50 cu 49 a) 48 773 0 re 1.50 12
115
's 11 E 10 5o 1, 50 100 I 1 T---I I, 1 7 -;Ir-; IT-, I I. 1 L. 1 1 i I I 1 I.,-I: I-i I I i i Ilel I pei cilUI e
I 01 Imt...ciJc
flow cold water
-44\-kemi\pAv-I , ! I ! , , , , :,_ :-1,ATAilLaik_AAL:_
, . , I I I I i ! I, ! , 4 I : , , . . , . l ;-r i I I 350 400450
500 Li 50 100 150 200 250 300 350 400 450 500measurement number daa
I -09-95 50 100 ,t , : r , ,
'1-35
325
_c 2 150 200 250 300 350 400 450 500flow cooling water
J a 150 200 250 300 I
I
20
15 10 5 oo 12 0 50 1 200 250 300 350 400 450 500 100 50 100synchronisation signal Hydra
I I I I T i I I I t . -I I - I, 1 -I 1 I I I I I I I
II
1 -: It -- I I-. I I I I III
I I I. ii II 11 r. : I I 1 I I I I I , I I 1 I 1 1 I I 150 200 250 300 350 400 450 500 time netdaq 1 i I I I I I I 1 ITIir
II : - II : TI I I I I I I i I I I I I I, Ai I-. -J 4. l . I I I I 1 i I I i i I I I I I I i Ir I I irr
1 --1 7 1 I I I I I I I 1 I 1 1 1 Ipressure crankcase
I 7 1 I j I r 7 I I I I I I III
L 4 -L 7 I I I 150 200 250 300 350measurement number daa 18-09-95
400 450 500 E 10 0 : 1 50 100 150 8 7 -15 -J
;TA-5 (13 I (Y3sj 4
I-0
20 18 n 1 4 0 Cot n4-00 50 100 150 200 250 300 350 400450
500 50 100 II 1 i I 1, : 4 i I, TI I I II i I 1-I I i I I I I I I-I I-I r 1 I 1 1 1 I i 150 200 250 300 350 400 450 500pressure discharge compressor
I I I I I 1... 1 I I I I i I I I I I I I I 1 I -J L Li I I I I I I I 1 1 i i I pressure evaporator in pressure oil 1 1 1 ____1_ 200 250 300 350
measurement number dab 18-09-95
400 450 500 1: I 8 I IT I 7 1 I -II. I +I 6 4 -I (13 5 4 150
a
20 18 9 18 17 14 0 50 100 -11 -50 1. 100pressure expansion valve in
I I T , ; , I i I
II
_I, IL L t I 1 I 1 I I I I i 1 1ff
\
7 \ - \ NI .v-'-'"---T A--.; t 1 I 1 i 1 : T t t f 1 1 1 1 I 1_--____-1 I I I 1 1 150 200250
300 350 400450
pressure compressor in
I
r i i T -1 . , e I I i I I I I I I, -I I ir : I 1 T 1 I 4 I I 1 I I I I I i I 1 1 I e 1 -I" .1, 1 1-i I -i I 1 1 , 1 i I -Ti 1 i I 1 1 I 1 I I 1_. 150 200 250 300 350 400pressure condensor out
, -;, , ; -,, ; , , , , , ;
i
1 , ; . , _ "-., , ; ; 4 I 1 I I I i50
100
150
200
250
300
measurement number daal -09-95
350 400 450 500
500
-450
500
7 0 14 160 5 151 1 t.--I 1-i al 1. -1 1 i I I I I I I I i I I I 1 t. -t I--i i I I I
II
i I I I i i t t I r-ItT.
: t, , , i_i
1 50 100 150 200 250 300measurement number daa 18-09-95
pressure difference now lieu
1, 1 1 1 1_ 1 _l_. 250 300 350 400 power I 1
-400synchronisation signal netdaq
450 500 1 450 500 350 400 450 500 I t ,,--,.-.---.. i I i I i i i b i 10 5 oo 350
50
100 150 200 250 300 20 15 10 5 > 0o -150 -= -I -I 200 I1 0.5 1080 1060 1040 :13E 1020
IJICJOUI C UIII CI CI Rae Lull ecaCt..1
1. flow freon
specific mass freon
15p 200 250 300 350 400 450 500 L.--_i
-klmyitiviviiii
i -s. 1 . . -...,I
I -v..= 1 i t 1 --wooo 0.5 0.4 0.3 cn O.2 50 100Niervitfi
1 50 100 50 100 150 200 250300
350 400 450 500 150 200 250 300 350Measurement number dad 18-09-95
400 450 500 0 -4 tr
1
I I I 1 -I I L-TU Delft
measurements on a 'refrigeration system van Butien -van Swaay1!TU Delft
Measurements on 21 - 09 - 1995
measurements on a refrigeration system
For detailed information about the measurements on day 21-09-1995 see appendix A
row numbers are the row number in the excel sheet, not the row numbers of the ASCII tiles!
van Suuren -van Swaay
54
Filenames ic211m.xls Excel 5.0 worksheet
ic211m.txt ASCII (spaces as delimiters)
Begin time 08:29:58
End time 16:39:16
Number of measurements 3268
Measured faults A 12(09:50 until 10:01)
546 - 616
condenser water side fouling
C 12(10:01 until 11:02)
617- 780
condenser water side fouling
A I 1 (13:07 until 13:35) 1860 - 2139
Too little refrigerant (condenser): extraction of 3.00 kg freon C 11(15:02 until 16:39)
2622 -2975
Too little refrigerant (condenser): extraction of 3.55 kg freon
pug.
16 14 12 7
2 o
( ) 30 0 25o
a) 7 20 a) Fa) L_ 0) sp 15 77 0 40 in 357
15 300
to a) 25 C7) CD 20 13 0 500 500 1000 1000time rwara
temperature cooling water in
1500
1500
2000
temperature cooling water out
2000 21-09-95 2500 2500 3000 3000 3500 3500
4000
4000 LF
T _ Li L I"II
-I_ IL L. 4 L. _ L I i i s-t_\
i 17
\
i 1 i I i 1 --:-il
1 -_ 1 _ , -s I -, = a-:-,-- a-:,--I 500 1000 1500 2000 2500 3000 35004000
a) I20 20 15 25
7 20
'5 a) a)-10 0 500 500 1000 1000 1500emperatu e cniiieu water iii
temperature chilled water out
temperature environment
1500 2000 200021-09-95
2500 2500 3000 3000 35003500
4000
4000
45 In Of) o:t0-
F-r ..----1...,,,,,,w_te...
IV 1- e_-_-I s- 71-t I _ si s 1 , 1 ______ 1 I I I I 1 I-1
1 I 1ii
I.. _._- _-_ . I I I "'".IL_
,...,_. - I -_,. 13 0 500 1000 1500 2000 250Q 30003500
4000
0
-I I I I I I I-I50 K) 45 a) co -(1) 40 173 0 20 a.) (I) 10 90 85 VI
o 80
a) a) 75 1:3 0 500 1000 1500 2000 2500 3000 35004000
500 1000 temper atui etemperature compressor in
11500temperature compressor out
2000
21-09-95
2500 30003500
4000
-. .. . r
r
1 ...\
\
\ '"fr E-
--! 1 I I171601
a 1iti
/45.1 I s I :LI< I i 1 - - .a-.., I-I I-I k i -) -500 1000 1500 2000 2500 30003500
4000
0
I I/
I L L L457
40 ai 30 -0 0 45 40 a)0 35
0.) 30 20orirr"
L. 500 1000 1500temperature condensor out
temperature evaporator in
L.
2500
temperature expansion valve in
3000
3500
4000 00 t.1.1r
, i L L L t_ I L _ I I I / I 1 I /...C,".-.-Ar--r"
. t I, t I t , , e rr
i . t t , , r -...----1... I 1 ./.#-^ Lh . _ _ 1 -, i 500 1000 1500 2000 2500 3000 3500 4000 21-09-95 13 0 500 1000 1500 2000 2500 3000 3500 4000 (i)3
35 0 200055 50
0 45
a) Lci. a) 40no
500 1000 1500 2000 2500 3000 35004000
_C -CO 325
E2
0 12115
0 cg 10 5 --0 500 1000 500 1000 temperature crankcase 1500 1500flow cooling water
2000
flow cold water
2000 21-09-95 2500 2500 3000 3000 i 11 3500
4000
3500 4000 I-I I -I I I-I III
ill
I I I I I 1 i Irq
I I I I I I I I $161"Vtel4it4t0N4111VII i . I I I I I I I I 1 1 I I 1 1 Oi______ , , I , , , 4 4 ' , 1' 1111 .1 irk INI I I 1 1 ' 111- 1111 -: . ,20 15 10 5 -5 oo
-16f,-
--I 14 9 8 7 6 _a 5 0 500 1000 1500 2000 2500 3000 3500 4000 1 -rsynchronisation signal Hydra
time netdaq
pressure crankcase
1 500 1000 1500 2000 2500 3000 3500 4000 21-09-95 1,~% I \ 1 1 I I L-I I ; I t _ T I LA...,
L.
2500 3000 3500 4000 500 2000 1000 1500 rcr) 8 7 12 10 500 1000
pressure discharge compressor
pressure evaporator in
pressure oil2000
2500 2500 3000 3500 3000 3500 40004000
1 vI-4"-, , , , , i ,,---,
I I 1 I I r i I I i i 1 i 1 __-I i I I I 1 Yk.,---,,,---1,----I r I I I i I 1 I I i i 1 1 i I I I 1 1 i 1 I I I I _ i ' ii"
r WOK/in**-*INOMPOS
r I I 1 1 i : I :i :1 . i 1 1 1 i 1 , I i 1 : ' I , I t I 1 I , -2000 21-09-95 500 4000 3500 2500 3000 1500 1000 20 15 500 1000 1500-r
I I 150018 16 14
12
(' 9 8-o12
0pressure expansion valve in
pressure compressor in
pressure condensor out
I_ .,e...41..4.40 L I i I 1 I I I f-I L I I 1 I 1 I I I I i I I r. I i I I I _ 1 1 L_ L L I _ 1 1 1 1 Vw.or--\\...., i I I _. I , r 1 1 1 1 '-i 1 i I 1 1 , 1
1
I , , 1 1 i 1 1 1 I I : Ir
1 1 I I I I I I-I _ : 1 I 1 1 I I I I 500 1000 1500 2000 2500 3000 3500 4000) 21-09-95 500 1000 1500 2000 2500 3000 3500 400C 0 500 1000 1500 2000 2500 3000 3500 400C4 18 16 0-r I-r
1 0.5 0 20 15 10 0 500 1000
bsuie umeierice now
Iuu
1500 power 2000 21-09-95 2500synchronisation signal netdaq
2500 3000 3000 3500 4000 3500 4000 at) al C._ C i i
,
I
...WI L.J.,/
r"..."4" \..ie 1._ L 1 I l I I , L L. 1--I rr
r I 1 I . --0 500 1000 1500 2000 500 1000 1500 2000 2500 3000 3500 4000 151 10 5 oo pi I -a I I I I >It
2 1.5 0.5 0.6 0.4 0pressure difference corrected
specific
mass
freOnflow freon
21-09-95 1 -_ 1 , 1 _ r. --u ; i ---,_____ . !I, I t 1 t r. e.:1":"..,r I-, -1 1 Ire#°4"ri'l-. 1 1 . I 1--I INsLY,2222 12,2II
I 2, i I r r _ rIHITI
lil
_ 1.110441 m 1... -0 500 1000 1500 20002500
30003500
4000
500 1000 1500 20002500
3000 3500 4000 35004000
500 1000 15002000
2500 3000 1100 1050woo
r I 002
1LB
TU Delft
5.6.
Measurements on 22 - 09 - 1995
measurements on a refrigeration system
van Buuren -van Swaay,For detailed information about the measurements on day 22-09-1995 see appendix A row numbers are the row number in the excel sheet, not the row numbers of the ASCII files
Pag
II
Filenames ic221in.xls Excel 5.0 worksheet
ic22fin.txt ASCII (spaces as delimiters)
!Sin time
10:06:54 -.. --_ End time 16:30:00 Number of measurements 2560 'Measured faults , 'C 19 (10:09 until 10:50) 239 - 505bulb temperature 'forced' down (from 18.7 to 17.0
i. C 19(10:50 until 12:32)
545 - 1182
bulb temperature 'forced' up
(from 18.7 to 24.0 °C)
m
A 19(14:09 until 14:56) 1420 - 2100
bulb temperature 'forced' down
(from 11.6 to 7.0 °C)
A19 (14:57 until 15:39) 2150 - 2420
bulb temperature 'forced' up
(from 11.6 to 13.0 °C)
65
16 14 12 8 17 16.5 6 16 a) (.) Low 15.5
5
3) 15-o 0 45 40 TD 35 a) a) a) 30 time Hydratemperature cooling water in
temperature cooling water out
I 1 1 1 r 1 1 1 ' 1 1 1. 1 1 _ r _ I I 1 , L _ 1 1 41 I I --I i r 1 1 r 1 1 1 1 1 I I I 7 1 1 T I 1 ir 1 1 L , :-. I , n rwrurr-i__kirr-a___: I II 1 1 , t I i
flIrTT1--I I I I 1 1 4 1 1 1-I -11111111 1 . i ir 1 1 1 1 i I 1 I I LI_ , , , -ri I 1 I I I i I I I , I I I L 4 e_ . i I I 1 1 1 1 1 I 1 _le _e _.. 1 i e 1 1 i 1 1 0 500 1000 1500 2000 2500 3000 35002/-09-95
500 1000 1500 20002500
30003500
500 1000 1500 2000 2500 3000 3500 0 I 10 a)20
15
25
500
1000
temperature chilled water in
temperature chilled water out
temperature environment
1500 2000 22-09-95 2500 3000 3500 rzfi -...-.--..-.1.--...-,,-....,i
\
I i I I i I I I i 1 i iHHWT
--- __ Ill ii I.- 1.---I I I I I I 1 ....,...,-,--. I I I-I I . i I I 1 1 1 1 1 I ---\t"--"----..--,,_1i
r 1 1 1 1 i 1 1 i 1 : 1 i : 1 t s o :i t 1 ____L 500 1000 1500 2000 2500 3000 3500 500 1000 1500 2000 2500 3000 3500 1-0
50 20 u) 15 Cr) 10 rja)0
90 temperature oil temperature compressor intemperature compressor out
I I I I I-I I I I I I - 4 1 I I-I .---'----''''----"-.--s'"'""'-*---'---Th-4f I 1 1 1 I -I L _/ L 1 1 1 1 i 1 i 1 1 1 1 1 1 1 1 1-1 I 1 __ t t 1 r\ r---:"---t r 1 1 t ._, t i i I I --N---"--r----I 1 I t 1 -1 1 1 I t I [ I t 1 ri i pl. 1 t 1 ] 4, o 1 I I I 1 I I I I ,. -4 I I l--I I I I I I I I I I 1 I i I I I I -1 L --4 , I I I I I I I I I I I I I I I I I I II 1 L J L 1 i 1 i / 0 500 1000 1500 2000 2500 3000 3500 Ta-) 0 500 1000 1500 2000 2500 3000 3500
22-09-95
00
500 1000 1500 2000 2500 3000 3500-45 45 40 E5 a) 10
temperature condensor out
temperature expansion valve in
temperature evaporator in
1 i i 1 i i i I i 1 : t 1 I I I I i 1 1 1 1 I ir I 1 , 1 -0----,,,A,...----, . 1 1 , 1 1 I _ I i, I IL I L, i : 1 , , iiN...--,
-1, I i I I I Ir I .1 I I L I I I I I I I I I I I I I I I I I I, r r I I I i i I I I I 500 1000 1500 2000 2500 3000 3500 fl 500 1000 1500 2000 2500 3000 350022-09-95
500 1000 1500 2000 2500 3000 3500-0
_c 50 in 45 if) 40 a) 35 (1) 30DO
3 2.5 2 0 12 11 52
10 500 1000 500 1000temperature crankcase
1500flow cooling water
1500
flow cold water
2000 2000 2500 2500 3000 3500 1 i i 1 -1 L-- I i i
L
al _ -, I ! I I 1 i I ilifrAifitit
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7
6
synchronisation signal Hydra
time netdaq
pressure crankcase
-- ,---t i I I 1 I -I 1 1 o I _ t I I I I I ' I I I I i i i i I t 1 I I I t i i I : I I L 1 I I r I I I I 1 I II I I I I 1 1 I t I IL 1 ..I, IL i i i I I I 1 1 I I I I I i I I i I i I I i I I i 1 1 1 i 1 I r : i i 1 I r I - I T 1 I i 1 1 i 1 1 . i 1 I . . . . . . . . . 1 i i 0 500 1000 1500 2000 2500 3000 3500 20 15 10 4, 50
500 1500 2000 22-09-95 1000 2500 3000 3500 500 1000 1500 2000 2500 3000 3500 --1 1 1 0 019 18 17 nco 16
n15
0 12 10 500pressure aiscnarge compressor
1500 pressure oil. 2000
pressure evaporator in
2500 3000 3500 -1 11 1I
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3000 3500 1000 2500 7 6 500 1000 1500 2000 2500 3000 3500 en 0 ena
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o14
8 7 18 17 s(f)3 14pressure expansion valve in
pressure compressor in
pressure condensor out
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-
-I-0 5 0.5 0 15 10 20 15 10 5
pressure difference flow freon
power
synchronisation signal netdaq
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--I I I / I I I I I I I I I I 4 I.-I 1 L --I I I I I I t I I I I 1 r: : Ir I I I I I I II I I I I I I I I IIi_
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10
105
E 0 1100 1050 0.1 0 500 1000pressure difference corrected
1500
specific mass freon
flow freon 2000 250 3000
3500
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I I I IT U Delft
Measurements on 25 - 09 - 1995
measurements on a refrigeration system
For detailed information about the measurements on day 25-09-1995 see appendix A row numbers are the row number in the excel sheet, not the row numbers of the ASCII files !
van Buuren -van Swaay
pal. 75
Filenames ic25fin.xls Excel 5.0 worksheet
ic25fin.txt ASCII (spaces as delimiters)
Begin time 10:06:54
End time 16:30:00
Number of measurements 2560
Measured faults A 21(10:40 until 12:12) oil injection (evaporator)
230 - 840 +2.50 kg
A 9 (10:01 until 11:02) air injection (nitrogen in condenser)
16 14 1 0 0 18 50 40 CD time Hydra
temperature cooling water in
temperature cooling water out
! ; -1 . . . 1 . -_
,
i 1____
t___ I -, i -_ i t -;i
I..,---:--1_-..
L. r _ ._-- ._-- rr
-. _ IIi
! L , ii : -1 2000 2500 3000 500 . 1500 25-09-95 1000 2000 2500 3000 500 1000 1500 500 1000 1500 2000 2500 3000 17 a) 3 30 20 0 12 016 0 12 16 14 cy) a) 6
P
0 24 0 22 ci) 20 a) ,(1) 18 a) 500 1000temperature chilled water in
temperature chilled water out
temperature environment
2000 2500 3000 <7.1 C.. r rr
1 _.---.-'-'-H--I I I I I i I .77+_...._,...._..,_ :1 I I r I. I I 1 r 11 i . 1 1 1 _,
1 , 500 1000 1500 2000 2500 3000 25-09-95 500 1000 1500 2000 2500 3000 10 0 12 _ ) 0 1500t
'o45
Ills
Tu cn ai a) 40 1:3Ho
-50 90 80.4
-(1) tno0 70
0
o ..D
um 60 A (i) cna) 50 C)00
500 1000 temperature oil 1500 temperature compressor in 2000 2500temperature compressor out
25-09-95 3000 _ 00 p.
Ills
A
.__
:,
---; = -1 -1 1` eiArtiMhErSer-W166* i I 4'1 _r______ a L _ _ _ _ 1 1 , -I HTrl'ir
1, !.. i. I 500 1000 1500 2000 2500 3000 500 1000 1500 2000 2500 3000 12 10-4
? 2 0 It45
40 5 a). 35 Cu a) 30g 30
D 0temperature condensor out
temperature evaporator in
25-09,95J -s t -,e,..°'1---vt
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0 35
Ct a) -590 1909 1500 2000 2500 3000temperature expansion valve in
20 15
0
10 0 5 cm 500 1000 1500 2000 2500 3000 500 1000 1500 2000 2500 3000 I I I52
a)
0
4 3 12 11.52
CO) 10 temperature crankcaseflow cooling water
flow cold water
25-09-95
e
III
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1 -r _ _ , . .--. - -I 500 1000 1500 2000 2500 3000 i0D
0 500 1000 1.500 2000 2500 3000 500 1000 1500 2000 2500 3000 50 48 46 0-1
11 00 -I I I I I I I I I I I I I I I I I I16
8
6
...naive notateva I °ay. 1 CA 1
I iyUl 0 time netdaci pressure crankcase 1500
25-09-95
2000 2500 3000 .--= g a_
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-,-- 2 a- ..r ,, .-n
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c 5 0 1500 2000 2500 3000 1000 1500 2000 25000
14 0 a) 10 1 500 1000 I I I I I I I --- I-I J 3000 15 >20
18
8
7
pressure aiscnarge compressor
pressure evaporator in pressure oil = 1500 2000 25-09-95 2500i 3000 I _ _ _._ _ _ _ -i
,
IC
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2_'
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18 17 16 "E) co 15 0 co-o14
500 1000 15002000
2500 3000 -L. 1000pressure expansion valve in
pressure compressor in
pressure condensor out
1 500 1000 1500 2000 2500 3000 f'") 00 01) I Li , , ,L
,
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t : i 1 ! 1r
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pressure difference flow freon
power
1500
synchronisation signal netdaq
25-09-95 2000 2500 3000
1111
II
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ill
ii. es_r
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I ___ _ I 500 1000 1500 2000 2500 3000I.
-a5 20 15 10 5 500 10001 1500 2000 2500 3000 0 I I I I I I I I I I I I I I I I I I I I I I I I I I I I I Ii
500$3 0 1 Q,5
woo
0.4'03
0.2 0.1pressure difference corrected
flow freon
specific mass freon
25-09-95
=
--, ) ; Lnit'st L. I _L -1--_ . ___ _ _ 1 -t -I_
-, L s-_ 1150 ft; 1100 al .r. 1050 500 1000 1500 2000 2500 3000 500 1000 1500 2000 2500 3000 500 . 1000 1500 2000 2500 3000 I-0 0TU Delft asurements on a refrigeration system
6. Data analysis and conclusion
6.1
Measurements on 14 - 09 - 1995
In the next sections, we will analyze the effects of varying the refrigerant quantity in the cooling
system. The freon is added to (fault it 10) or removed (fault # 11) from the system just after the
condenser, simulating respectively a leakage and a too large refill. The test starts with the system in
an healthy condition (C). The leakage steadily reaches a maximum 3.05 kg of freon after
approximately 45 min. After restoring the healthy condition C, a surplus of refrigerant is simulated:
2.0 kg of freon is added to the system in about 30 min. The system is then brought to condition A,
from which the refrigerant surplus will be removed.
6.1.1
Too little refrigerant (C 11)
observations
The chilled water and the cooling water flow remain constant throughout the experiment. There is a decrease in the in-going evaporator temperature: Te, goes from 9 °C to 4.5 °C andTcd shows a slight tendency to increase first, then to decrease (±0.5 °C). At the end, it will have the same temperature of the start: 86-0 °C. Tn,,falls from 36 down to 33°C, as opposed to the raise inTaw° 15.3 to 16.2 °C. The sub-cooling decreases (4 °C to 2 °C), while the superheating increases from 10 °C to 15 °C. The condensing temperature also decreases (45 to 39 °C).
The compressor power decreases by 10%. We also observe a decline in condenser power 69 to 56
kW, along a loss of evaporator power: 45 kW at the end
of
the test against 55 kW during 'healthy'operation.
Gaseous freon bubbles appear just after the first 300 g of refrigerant are drawn from the system.
Interpretation
As the freon level decreases, some bubbles appear in the spy-glass: this means that momentarily less liquid freon circulates through the expansion valve ( temporary with constant opening ). However, for
a short period, the compressor maintains its power constant, causing a pressure decrease in the
evaporator. The lower pressure in the evaporator induces the expansion valve to open further. The compressor reduces marginally its production; consequently, the condenser will condense less gas. The condensation pressure also decreases. We have now reached the new equilibrium point: lower condenser and evaporator pressures, lower mass-flow and compressor power. The system alsopresents a lower sub-cooling and superheating.
van Buuren -van Swaay