Megger DELTA 4000 Reference Manual

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Reference Manual Applications Guide
DELTA 4000
12 kV Insulation Diagnostic System
ZM-AH02E
Advanced Test Equipment Rentals
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SWEDEN Megger Sweden AB
Eldarvägen 4 Box 2970 SE-187 29 TÄBY Sweden
T +46 8 510 195 00 F +46 8 510 195 95 seinfo@megger.com www.megger.comEDEN
UNITED STATES Megger
2621 Van Buren Avenue Norristown, PA 19403
USA
T +1 610 676 8500 F +1 610 676 8610 VFCustomerSupport@megger.com www.megger.com
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NOTICE OF COPYRIGHT & PROPRIETARY RIGHTS © 2010, Megger Sweden AB. All rights reserved. The contents of this manual are the property of Megger Sweden
AB. No part of this work may be reproduced or transmitted in any form or by any means, except as permitted in written license agreement with Megger Sweden AB. Megger Sweden AB has made every reasonable attempt to ensure the completeness and accuracy of this document. However, the information contained in this manual is subject to change without notice, and does not represent a commitment on the part of Megger Sweden AB. Any attached hardware schematics and technical descriptions, or software listings that disclose source code, are for informational purposes only. Reproduction in whole or in part to create working hardware or software for other than Megger Sweden AB products is strictly prohibited, except as permitted by written license agreement with Megger Sweden AB.
TRADEMARK NOTICES Megger® and Programma® are trademarks registered in the U.S.
and other countries. All other brand and product names mentioned in this document are trademarks or registered trademarks of their respective companies.
Megger Sweden AB is certified according to ISO 9001 and 14001.
Reference Manual Applications Guide
DELTA 4000
12 kV Insulation Diagnostic System
4 DELTA 4000 ZM-AH02E
Contents
1 Introduction ................................................. 6
General .................................................................6
Principle of operation .............................................6
Current, capacitance and dissipation factor
relationship ............................................................ 7
Connections for UST/GST Configurations ............... 8
2 Interpretation of measurements ............. 10
Significance of capacitance and
dissipation factor .................................................10
Dissipation factor (Power factor) of typical
apparatus insulation ............................................11
Permittivity and % DF of typical insulating
materials ..............................................................11
Significance of temperature ................................. 12
Significance of humidity .......................................13
Surface leakage ...................................................13
Electrostatic interference ...................................... 14
Negative dissipation factor ................................... 14
Connected bus work, cables etc ................................ 14
3 Testing power system components ......... 16
Transformers ........................................................ 16
Introduction .............................................................. 16
Definitions ................................................................ 16
Two-winding transformers......................................... 16
Three-winding transformers ...................................... 18
Autotransformers ...................................................... 19
Transformer excitation current tests ........................... 19
Shunt reactors ........................................................... 21
Potential transformers ............................................... 21
Current transformers ................................................. 21
Voltage regulators ..................................................... 21
Dry-type transformers ............................................... 22
Bushings .............................................................. 22
Introduction .............................................................. 22
Definitions ................................................................ 22
Bushing troubles ....................................................... 24
Bushing tests ............................................................. 24
Inverted tap to center conductor test C1 (UST) .......... 26
Power and dissipation factor & capacitance test C2 ... 26
Hot collar test ........................................................... 27
Spare bushing tests ................................................... 27
Circuit breakers .................................................... 28
Introduction .............................................................. 28
Oil circuit-breakers .................................................... 28
Air-blast circuit-breakers ............................................ 30
SF
6 Circuit-breakers ................................................... 31
Vacuum circuit breakers ............................................ 32
Air magnetic circuit-breakers ..................................... 33
Oil circuit reclosers .................................................... 33
Rotating machines ............................................... 33
Cables .................................................................35
Surge (lightning) arresters .................................... 35
Introduction .............................................................. 35
Test connections ........................................................ 36
Test procedure .......................................................... 36
Test results ................................................................ 36
Liquids ................................................................. 37
Test procedure .......................................................... 37
Miscellaneous assemblies and components .......... 37
High-Voltage turns-ratio measurements ...............38
Test procedure .......................................................... 38
Temperature considerations ....................................... 38
Index ............................................................. 40
References ........................................................... 42
Appendix A
Temperature correction tables .................... 44
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1 INTRODUCTION
1
Introduction
Principle of operation
Most physical test objects can be accurately represented as a two or three-terminal network. An example of a two­terminal capacitor is an apparatus bushing without any test tap. The center conductor is one terminal and the mount-
ing ange (ground) is the second terminal. An example of
a three-terminal capacitor is an apparatus bushing which has a power factor or capacitance tap. The center conduc­tor is one terminal, the tap is the second terminal, and the
mounting ange (ground) is the third terminal.
It is possible to have a complex insulation system that has four or more terminals. A direct measurement of any capacitance component in a complex system can be made with this test set since it has the capability for measuring both ungrounded and grounded specimens.
Figure 1 shows a simplied measuring circuit diagram of
the DELTA 4000 test set measuring a two-winding trans­former
in UST test mode. The test voltage is connected to the HV terminal and the current is measured at the LV terminal. Voltage and current are accurately measured in amplitude and phase and CHL capacitance, dissipation factor, power loss etc are calculated and displayed.
Figure 1: UST-R test setup for a 2-w transformer
Dissipation factor measurements can generally be per-
formed with two different congurations, UST (Unground­ed Specimen Test) where the ground act as natural guard or GST (Grounded Specimen Test) with or without guard.
Figure 2 shows a guarded UST measurement. The current
owing through CHL is measured but the current paths
through CH and CL is guarded/grounded and not mea­sured. Figure 3 shows a guarded GST measurement where the CH current to ground is measured but the current through CHL is guarded and measured.
General
The intention of this reference-application manual is to guide the operator in the appropriate method of making capacitance and dissipation factor/power factor measure­ments on power apparatus and to assist in the interpretation of test results obtained. It is not a complete step-by-step procedure for performing tests.
Before performing any test with this apparatus, read the user manual and observe all safety precautions indicated.
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1 INTRODUCTION
Figure 2: UST connection for measuring CHL in a two-wind­ing transformer
Figure 3: GST connection for measuring CH in a two-wind­ing transformer
Current, capacitance and dissipation factor relationship
In an ideal insulation system connected to an alternating voltage source, the capacitance current Ic and the voltage are in perfect quadrature with the current leading. In ad­dition to the capacitance current, there appears in practice a loss current Ir in phase with the voltage as shown in Figure 5.
The current taken by an ideal insulation (no losses, I
r
= 0)
is a pure capacitive current leading the voltage by 90° (q = 90°). In practice, no insulation is perfect but has a certain amount of loss and the total current I leads the voltage by a phase angle q (q< 90°). It is more convenient to use the dielectric-loss angle d, where d = (90° - q). For low power factor insulation Ic and I are substantially of the same mag­nitude since the loss component Ir is very small.
The power factor is dened as:
Power factor= cos Θ = sin δ =
Ir
I
and the dissipation factor is dened as:
Dissipation factor = cot Θ = tan δ =
Ir Ic
PF =
DF
1+DF
2
DF =
PF
1 – PF
2
The DELTA 4000 is able to display either dissipation factor or power factor based on user’s choice.
Figure 5: Vector diagram insulation system
In cases where angle d is very small, sin d practically equals tan d. For example, at power factor values less than 10 percent the difference will be less than 0.5 percent of read­ing while for power factor values less than 20 percent the difference will be less than 2 percent of reading.
The value of I
c
will be within 99.5 percent of the value I
for power factor (sin d) values up to 10 percent and within
98 percent for power factor values up to 20 percent.
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1 INTRODUCTION
Connections for UST/GST Configurations
DELTA 4000 supports two basic groups of operation, GST and UST mode. GST stands for grounded specimen test while UST stands for ungrounded specimen test. Within the two groups the test set can be operated in seven test modes as summarized in Table 1.1. Measurements are always made between the high-voltage lead and the lead/ connection in the measure column.
Table 1.1 DELTA 4000 test modes and internal measure­ment connections
UST: Ungrounded specimen testing
Tes t mo de Measure Ground Guard
UST- R Red Blue – UST- B Blue Red – UST- RB Red and Blue
GST: Grounded specimen testing
Tes t mo de Measure Ground Guard
GST- GND Ground Red and Blue – GSTg-R Ground Blue Red GSTg-B Ground Red Blue GSTg-RB Ground Red and Blue
In UST test mode, Ground and Guard are internally connected. Internally the Red and Blue leads are either
connected to be measured or connected to Ground (and Guard).
In GST test modes the current returning from Ground is measured. Internally the Red and Blue leads are either con­nected to Ground or Guard to be included in or excluded from the measurement.
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1 INTRODUCTION
10 DELTA 4000 ZM-AH02E
2 INTERPRETATION OF MEASUREMENTS
in operation with consequent deterioration. Some increase
of capacitance (increase in charging current) may also be
observed above the extinction voltage because of the short circuiting of numerous voids by the ionization process.
An increase of dissipation factor accompanied by in severe cases possible increase of capacitance usually indicates excessive moisture in the insulation. Increase of dissipation factor alone may be caused by thermal deterioration or by contamination other than water.
Unless bushing and pothead surfaces, terminal boards, etc., are clean and dry, measured quantities may not necessar­ily apply to the volume of the insulation under test. Any leakage over terminal surfaces may add to the losses of the insulation itself and may, if excessive, give a false indication of its condition.
2
Interpretation of
measurements
Significance of capacitance and dissipation factor
A large percentage of electrical apparatus failures are due to a deteriorated condition of the insulation. Many of these failures can be anticipated by regular application of simple tests and with timely maintenance indicated by the tests. An insulation system or apparatus should not be con­demned until it has been completely isolated, cleaned, or serviced and measurements compensated for temperature. The correct interpretation of capacitance and dissipation factor tests generally requires knowledge of the apparatus construction and the characteristics of the particular types of insulation used.
Changes in the normal capacitance of an insulation material indicate such abnormal conditions as the presence of a moisture layer, short circuits, or open circuits in the capaci­tance network. Dissipation factor measurements indicate the following conditions in the insulation of a wide range
of electrical apparatus:
Chemical deterioration due to time and temperature, including certain cases of acute deterioration caused by localized overheating.
Contamination by water, carbon deposits, bad oil, dirt and other chemicals.
Severe leakage through cracks and over surfaces.
Ionization.
The interpretation of measurements is usually based on experience, recommendations of the manufacturer of the
equipment being tested, and by observing these differences:
Between measurements on the same unit after successive intervals of time.
Between measurements on duplicate units or a similar part of one unit, tested under the same conditions around the same time, e.g., several identical transformers or one winding of a three-phase transformer tested separately.
Between measurements made at different test voltages on one part of a unit; an increase in slope (tip-up) of a dissipation factor versus voltage curve at a given voltage is an indication of ionization commencing at that voltage.
An increase of dissipation factor above a typical value may indicate conditions such as those given in the previous para­graph, any of which may be general or localized in charac-
ter. If the dissipation factor varies signicantly with voltage
down to some voltage below which it is substantially con­stant, then ionization is indicated. If this extinction voltage is below the operating level, then ionization may progress
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Dissipation factor (Power factor) of typical apparatus insulation
Values of insulation dissipation factor for various appara­tus are shown in Table 2.1. These values may be useful in roughly indicating the range to be found in practice. Please note that the higher values are not to be regarded as “OK” but instead examples of “to be investigated/at risk” data.
Table 2.1 DF (PF) of typical apparatus insulation
Type apparatus % DF (PF) at 20°C
Oil-filled transformer: New, high­voltage (115 kV and up)
0.25 to 1.0
15 years old, high-voltage 0.25--
Low-voltage, distribution type 0.30-­Oil circuit breakers 0.5 to 2.0 Oil-paper cables, “solid” (up to 27.6
kV) new condition
0.5 to 1.5
Oil-paper cables, high-voltage oil-filled or pressurized
0.2 to 0.5
Rotating machine stator windings, 2.3 to 13.8 kV
2.0 to 8.0
Capacitors (discharge resistor out of circuit)
0.2 to 0.5
Bushings: Solid or dry 3.0 to 10.0
Compound-filled, up to 15 kV 5.0 to 10.0
Compound-filled, 15 to 46 kV 2.0 to 5.0
Oil-filled, below 110 kV 1.5 to 4.0
Oil-filled, above 110 kV and con-
denser type
0.25--
In IEEE 62-1995, typical values for dissipation/power fac­tor are given as in Table 2.2.
Table 2.2 IEEE 62-1995 power factor values
Typical power factor values @ 20°C
“New” “Old” Warning/alert limit
Power trans­formers, oil insulated
0.2-0.4% 0.3-0.5% > 0.5%
Bushings
0.2-0.3% 0.3-0.5% > 0.5%
IEEE 62-1995 states; “The power factors recorded for routine overall tests on older apparatus provide information regarding the general condition of the ground and inter­winding insulation of transformers and reactors. While the power factors for older transformers will also be <0.5%
(20°C), power factors between 0.5% and 1.0% (20°C) may be acceptable; however, power factors >1.0% (20°C) should
be investigated.”
Permittivity and % DF of typical insulating materials
Typical values of permittivity (dielectric constant) k and
50/60 Hz dissipation factor of a few kinds of insulating
materials (also water and ice) are given in Table 2.3.
Table 2.3 Permittivity and dissipation factor of typical insulating materials
Material k % DF (PF) at 20°C
Acetal resin (Delrin*) 3.7 0.5 Air 1.0 0.0 Askarels 4.2 0.4 Kraft paper, dry 2.2 0.6 Oil, transformer 2.2 0.02 Polyamide (Nomex*) 2.5 1.0 Polyester film (Mylar*) 3.0 0.3 Polyethylene 2.3 0.02-0.05 Polyamide film (Kapton*) 3.5 0.3 Polypropylene 2.2 0.05 Porcelain 7.0 2.0 Rubber 3.6 4.0 Silicone liquid 2.7 0.01 Varnished cambric, dry 4.4 1.0 Water** 80 100 Ice** 88 1.0 (0°C) * Dupont registered trademark. ** Tests for moisture should not be made at freezing tempera-
tures because of the 100 to 1 ratio difference of % dissipation factor between water and ice.
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2 INTERPRETATION OF MEASUREMENTS
Any sudden changes in ambient temperature will increase the measurement error since the temperature of the appara­tus will lag the ambient temperature.
Dissipation factor-temperature characteristics, as well as dissipation factor measurements at a given temperature, may change with deterioration or damage of insulation. This suggests that any such change in temperature char­acteristics may be helpful in assessing deteriorated condi-
tions. As an example, bushings have typically a rather at
temperature correction with only slightly elevated values at high temperatures. Generally a bushing showing highly increased dissipation factor at elevated temperature should be considered “at risk”.
Be careful making measurements below the freezing point of water. A crack in an insulator, for example, is easily
detected if it contains a conducting lm of water. When
the water freezes, it becomes non-conducting, and the defect may not be revealed by the measurement, because ice has a volumetric resistivity approximately 100 times higher than that of water. Moisture in oil, or in oil-impregnated solids, has been found to be detectable in dissipation factor measurements at temperatures far below freezing, with no discontinuity in the measurements at the freezing point.
Insulating surfaces exposed to ambient weather conditions may also be affected by temperature. The surface tempera­ture of the insulation specimen should be above and never below the ambient temperature to avoid the effects of condensation on the exposed insulating surfaces.
Significance of temperature
Most insulation measurements have to be interpreted based on the temperature of the specimen. The dielectric losses of most insulation increase with temperature; however, e.g. dry oil-impregnated paper and polyethylene of good quality exhibit decrease of dielectric losses when temperature is
raised moderately, e.g. from 20°C to 30°C. It is also known
that the effect of temperature depends on the aging status of the insulation. In many cases, insulations have failed due to the cumulative effect of temperature, i.e., a rise in tem­perature causes a rise in dielectric loss which in turn causes
a further rise in temperature, etc (thermal runaway).
It is important to determine the dissipation factor-tempera­ture characteristics of the insulation under test. Otherwise, all tests of the same specimen should be made, as nearly as practicable, at the same temperature.
To compare the dissipation factor value of tests made on the same or similar type apparatus at different temperatures, it is necessary to convert the value to a reference tempera­ture base, usually 20°C (68°F). Examples of standard tables of multipliers for use in converting dissipation factors at test temperatures to dissipation factors at 20°C are found in the Appendix A of this document.
In reality, temperature correction for a specic compo­nent is always individual and pending age/condition. DELTA 4000 has a unique and patented feature for estimat­ing the individual temperature correction (ITC). By measur­ing dissipation factor over frequency and using mathemati­cal formulas and models of insulation characteristics, the correct temperature correction can be determined from
5 to 50°C measurement temperature to 20°C reference
temperature. The input data for the calculation is dissipa­tion factor measured from 1 to 500 Hz and the method is principally based on Arrhenius’ law, describing how the insulation properties are changing over temperature.
κ = κ
0
·exp(-Wa/kT)
With activation energy W
a
and Boltzmann constant k
The test temperature for apparatus such as spare bushings,
insulators, air or gas lled circuit breakers, and lightning
arresters is normally assumed to be the same as the ambient temperature. For oil-lled circuit breakers and transform­ers the test temperature is assumed to be the same as the top oil temperature or winding temperature. For installed bushings where the lower end is immersed in oil the test temperature lies somewhere between the oil and air tem­perature.
In practice, the test temperature is assumed to be the same as the ambient temperature for bushings installed in oil-
lled circuit breakers and also for oil-lled transformers
that have been out of service for approximately 12 hours. In transformers removed from service just prior to test, the temperature of the oil normally exceeds the ambient temperature. The bushing test temperature for this case can be assumed to be the midpoint between the oil and ambient temperatures.
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Significance of humidity
The exposed surface of bushings may, under adverse rela­tive humidity conditions, acquire a deposit of surface mois-
ture which can have a signicant effect on surface losses
and consequently on the results of a dissipation factor test. This is particularly true if the porcelain surface of a bush-
ing is at a temperature below ambient temperature (below dew point), because moisture will probably condense on the
porcelain surface. Serious measurement errors may result even at a relative humidity below 50 percent when moisture condenses on a porcelain surface already contaminated with industrial chemical deposits.
It is important to note that an invisible thin surface lm of
moisture forms and dissipates rapidly on materials such as glazed porcelain which have negligible volume absorption. Equilibrium after a sudden wide change in relative humid­ity is usually attained within a matter of minutes. This,
however, excludes thicker lms which result from rain, fog,
or dew point condensation.
Surface leakage errors can be minimized if dissipation factor measurements are made under conditions where the weather is clear and sunny and where the relative humid­ity does not exceed 80 percent. In general, best results are obtained if measurements are made during late morning through mid afternoon. Consideration should be given to the probability of moisture being deposited by rain or fog on equipment just prior to making any measurements.
Surface leakage
Any leakage over the insulation surfaces of the specimen will be added to the losses in the volume insulation and may give a false impression as to the condition of the specimen. Even a bushing with a voltage rating much greater than the test voltage may be contaminated enough to cause a signi­cant error. Surfaces of potheads, bushings, and insulators should be clean and dry when making a measurement.
It should be noted that a straight line plot of surface resis­tivity against relative humidity for an uncontaminated por­celain bushing surface results in a decrease of one decade in resistivity for a nominal 15 percent increase in relative humidity and vice versa.
On bushings provided with a power factor or capacitance tap, the effect of leakage current over the surface of a porcelain bushing may be eliminated from the measurement by testing the bushing by the ungrounded specimen test
(UST).
When testing bushings without a test tap under high humidity conditions, numerous companies have reported that the effects of surface leakage can be substantially minimized by cleaning and drying the porcelain surface and applying a very thin coat of Dow Corning #4 insulating grease (or equal) to the entire porcelain surface. When mak­ing a hot collar test, the grease is generally only applied to the porcelain surface on which the hot collar band is to be located and to that of one petticoat above and one below the hot collar band.
When testing potheads, bushings (without test tap), and
insulators under unfavorable weather conditions, the dis­sipation factor reading may, at times, appear to be unstable and may vary slightly over a very short period of time. The variation is caused by such factors as the amount of surface exposure to sun or shade, variations in wind velocity, and gradual changes in ambient temperature and relative humid­ity. Similar bushings may have appreciably different dissipa­tion factor values for the case where one bushing is located in the sun while the other is in the shade. A test made on the same bushing may have a different dissipation factor value between a morning and an afternoon reading. Due consideration must be given to variations in readings when tests are made under unfavorable weather conditions.
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Negative dissipation factor
Creep currents inside an insulation system or more com­monly on surfaces; create change of potential distribution that may give increased or decreased dissipation factor, and in some cases also negative dissipation factor. This condi­tion is most likely to arise when making UST and GST measurements on specimens who have a capacitance value of a few hundred picofarad or less. Equipment such as bushings, circuit breakers, and low loss surge arresters fall into this category.
The error is usually accentuated if tests are made under unfavorable weather conditions, especially a high relative humidity which increases surface leakage.
There appears to be no clear-cut way of knowing whether
an error is signicant or what remedies should be taken to
overcome an error. A frequency sweep may give additional information. The best advice is to avoid making measure­ments on equipment in locations where negative dissipation factors are known to present a problem when unfavorable weather conditions exist, especially high relative humidity. Make sure the surface of porcelain bushings are clean and dry to minimize the effects of surface leakage. Make sure all items such as wooden ladders or nylon ropes are removed from the equipment to be tested and are brought out of
any electrostatic interference elds that could inuence a
measurement.
Connected bus work, cables etc
A complete disconnected component is preferred when performing dissipation factor measurements. All connected bus work, cables, disconnect switches etc may add signi­cant capacitance and losses in GST measurements where they are in parallel with the desired insulation measure­ment. For this reason, many test engineers will ask that the equipment under test be totally isolated from connected apparatus.
UST data is principally possible to measure without fully disconnecting the test object. The capacitance from the connected parts results only in a current to ground that is not measured in UST test mode.
Electrostatic interference
When tests are conducted in energized substations, the
readings may be inuenced by electrostatic interference
currents resulting from the capacitive coupling between energized lines and bus work to the test specimen. Other
sources for interference may be corona discharges (espe­cially at high humidity) and is some cases DC uctuations in the grounding system. Trouble from magnetic elds
encountered in high-voltage substations is very unlikely.
To counter the effects of severe electrostatic interference on the measurement, it may be necessary to disconnect the specimen from disconnect switches and bus work. Experi­ence in making measurements will establish the particular equipment locations where it is necessary to break the connections. The related disconnect switches, leads and bus work, if not energized, should be solidly grounded to minimize electrostatic coupling to the test set.
The measurement difculty which is encountered when
testing in the presence of interference depends not only
upon the severity of the interference eld but also on the
capacitance and dissipation factor of the specimen. Unfa­vorable weather conditions such as high relative humidity, fog, overcast sky, and high wind velocity will increase the
severity and variability of the interference eld. The lower
the specimen capacitance and its dissipation factor, the
greater the difculty is to perform accurate measurements.
It is also possible that a negative dissipation factor reading may be obtained so it is necessary to observe the polarity
sign for each reading. Specically, it has been found that some difculty may be expected when measuring capaci-
tance by the GST test method in high interference switch­yards when the capacitance value is less than 100 pF. This
difculty may be minimized considerably by:
Using the maximum voltage of the test set if possible.
Disconnecting and grounding as much bus work as possible from the specimen terminals.
Making measurements on a day when the weather is sunny and clear, the relative humidity is less than 80 percent, the wind velocity is low, and the surface temperature of exposed insulation is above the ambient temperature.
Tests made by the UST method are less susceptible to in­terference pickup than are tests made by the GST method. In the UST test method, the capacitive coupled pickup
current in the high-voltage circuit ows directly to ground
after having passed through the high-voltage winding of the power supply transformer. In the GST test method the same pickup current, after passing through the high-voltage transformer winding, must pass through one of the bridge transformer-ratio measuring arms before reaching ground.
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