- Open Access
- Total Downloads : 16
- Authors : Deepak, Munisha Bage, Pushpanjali Singh Bisht, Parasnath, Arrik Khanna
- Paper ID : IJERTCONV4IS02026
- Volume & Issue : CMRAES – 2016 (Volume 4 – Issue 02)
- Published (First Online): 24-04-2018
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Transformer Fault Diagnosis Based on DGA using Classical Methods
Deepak 1,
1Student EEE Department,
RVS College of Engineering and Technology, Jamshedpur, India
Munisha Bage2
2 Student EEE Department,
RVS College of Engineering and Technology, Jamshedpur, India
Pushpanjali Singh Bisht 3
3Assistant Professor EEE Department, RVS College of Engineering and Technology,
Jamshedpur, India
Parasnath4
4Assistant Professor& HOD EEE Department, RVS College of Engineering and Technology, Jamshedpur, India
Arrik Khanna5
5 3Assistant Professor EEE Department, Chitkara University Punjab
Abstract- During the last few years there has been trend of continuous increase in transformer failures. It is therefore necessary to diagnose the incipient fault for safety and reliability of electrical network. Various faults could occur in transformer such as overheating, partial discharge and arching which can generate various fault gases so in order to diagnose the fault DGA (Dissolved gas Analysis) is done. In this paper the proposed methods are used which is based on standards and guidelines of International Electro technical Commission (IEC), Central Electric Generating board (CEGB), and the American Society for testing and Material (ASTM). Fault diagnoses methods by the DGA technique are implemented to improve the interpretation accuracy of transformer.
Keywords: Dissolved gas Analysis (DGA), Central Electric Generating board (CEGB), The American Society for testing and Material (ASTM), Institute of Electrical and Electronics Engineering (IEEE), International Electro technical Commission (IEC), British Standard (B.S.), Decomposition (Decomp).
-
INTRODUCTION
Transformers are the essential part of the electrical power system because it has the ability to alter voltage and current levels, which enables the power transformer to transmit and distribute electric power and utilize the power at economical and suitable levels. In electrical power system, voltage of electricity generated at the power plant will be increased to a higher level with step-up transformers. A higher voltage will reduce the energy lost during the transmission process of the electricity. After electricity has been transmitted to various end points of the power grid, voltage of the electricity will be reduced to a usable level with step-down transformer for industrial customers and residential customers. Since power transformer is vital equipment in any electrical power system, so any fault in the power transformer may lead to the interruption of the power supply and accordingly the
financial losses will also increase. So it is of paramount importance to detect the incipient fault of transformer as early as possible. The following characteristics of oil were laid down in B.S.148:1959 the values stated being obtained by the testing method specified in the, appendices of the standard:-
Table I: Physical Properties of Transformer Oil
Characteristic
Limit
Sludge Value(max)
1.20%
Acidity after oxidation(max)
2.5 mg KOH/gm
Flash Point (closed) (min)
295° F (146.1°C)
Viscosity at 70°F(21.1°C)(max)
37 cS
Pour Point (max)
(-25.06°F) (-31.7°C)
Electric Strength, 1 minute (min)
40 kV (r.m.s)
Acidity(neutralization value) Total (max) Inorganic
0.05mg. KOH/gm Nil
Saponification Value (max)
1.00 mg. KOH/gm
Copper discoloration
Negative
Crackle
Shall pass test
Specific gravity
No Limit
Faults can be differentiated for their energy, localization and occurrence period. Along with a fault, there are increased oil temperatures and generation of certain oxidation products such as acids and soluble gases. These gases, hydrogen ( H2), methane ( CH4 ), ethane ( C2H6 ), ethylene ( C2H4 ), acetylene ( C2H2 ), propane ( C3H8 ), propane ( C3H6 ), together with carbon monoxide ( CO ) and carbon dioxide ( CO2 ) are considered as fault indicators and
can be generated in certain. The operating principle of transformer is based on the slight albeit harmless deterioration of the insulation that accompanies incipient faults, in the form of arcs or sparks resulting from dielectric breakdown of weak or overstressed parts of the insulation, or hot spots due to abnormally high current densities or due to high temperature in conductors. Whatever the cause, these stresses will result in the chemical breakdown of oil or cellulose molecules constituting the dielectric insulation
-
DISSOLVED GAS ANALYSIS
Thermal and electrical distributions in the operating transformer are two most important causes of dissolved gases in oil. The gases produced from thermal decomposition of oil and solid insulation are because of losses in conductors due to loading. Also decomposition occurs in oil and solid insulation is due to occurrence of arc. In case of electrical disturbances the gases are formed principally by ionic bombardment. The gases are generated mainly because of cellulose and oil insulation deterioration. In the normal operation of the transformer, gases such as Hydrogen (H2), Methane (CH4), Ethylene (C2H4), Acetylene (C2H2), and Ethane (C2H6) and so on are released. In the existing methods, parts per million (PPM) values are determined for each gas in the oil along with a total value of combustible gasses. When there is an abnormal situation such as a fault occurrence, some specific gases are produced in greater quantity than in the normal operation. Thus, the amount of these gases in the transformer oil increases. The increase in the amount of gases results in saturation of the transformer oil and no further gas can be dissolved in oil. Therefore, when the oil is saturated, the gas is released from the oil. The amount of the dissolved gas is related to the temperature of the oil and the type of gas. The produced gas can be classified into three groups: polarization, corona, and arcing. These groups coming from the severity of the released energy during the fault are different. The largest and lowest amounts of the released energy are associated with the arcing and corona.
-
Polarization: In the transformer oil, the released gases at low temperature are CH4 and C2H6, and at high temperature are C2H6, CH4, C2H4, and H2. In cellulose, the generated gases at low and high temperatures are CO and CO2.
-
Corona: In corona, the produced gas in oil is H2 and the released gases in cellulose are H2, CO, and CO2.
Sl. No.
Code
Kind of fault
Grouping of fault
X
Y
Z
1
0
0
0
No fault
F1
2
0
1
0
Partial discharge with low intensity discharge
F2
3
1
1
0
Partial discharge with high intensity discharge
F3
4
1 or
2
0
1 or
2
Partial discharge with low intensity discharge
F2
5
1
0
2
Partial discharge with high intensity discharge
F3
6
0
0
1
Thermal fault with temperature less than 150°C
F4
7
0
2
0
Thermal fault with temperature between 150° C to 300° C
F5
8
0
2
1
Thermal fault with temperature between 300 °C to 700° C
F6
9
0
2
2
Thermal fault with temperature greater than 700°C
F7
Sl. No.
Code
Kind of fault
Grouping of fault
X
Y
Z
1
0
0
0
No fault
F1
2
0
1
0
Partial discharge with low intensity discharge
F2
3
1
1
0
Partial discharge with high intensity discharge
F3
4
1 or
2
0
1 or
2
Partial discharge with low intensity discharge
F2
5
1
0
2
Partial discharge with high intensity discharge
F3
6
0
0
1
Thermal fault with temperature less than 150°C
F4
7
0
2
0
Thermal fault with temperature between 150° C to 300° C
F5
8
0
2
1
Thermal fault with temperature between 300 °C to 700° C
F6
9
0
2
2
Thermal fault with temperature greater than 700°C
F7
-
Arcing: In this case, the released gases are C H , CH ,
Table II: IEC code determination Criteria
Gas ratio
Value
Code
X= C2H2/C2H4
X<0.1
0
0.1<X<3
1
X>3
2
Y= CH4/H2
Y<0.1
1
0.1<Y<1
0
Y>1
2
Z=C2H4/C2H6
Z<1
0
1<Z<3
1
Z>3
2
Gas ratio
Value
Code
X= C2H2/C2H4
X<0.1
0
0.1<X<3
1
X>3
2
Y= CH4/H2
Y<0.1
1
0.1<Y<1
0
Y>1
2
Z=C2H4/C2H6
Z<1
0
1<Z<3
1
Z>3
2
Table III: Fault Diagnosis IEC codes
C2H4, and H2.
2 6 4
In this method at first a sample of transformer oil is taken then the dissolved gases is extracted, separated and measured by means of chromatography. In order to interpret result of experiment data is produced is produced in suitable form to diagnose the fault. The different standard are used which are explained in following sections.
-
Rogers ratio method I (IEC Standard)
According to the IEC standards, the extended Rogers method is used to produce a three digit code. The code is determined based on the three gas ratios of C2H2/C2H4, CH4/H2, and C2H4/C2H6 as given in Table II.
-
Rogers ratio method II. (CEGB Standard)
In this standard, a four digit code is created using the Rogers method and four gas ratios of CH4/H2, C2H6/CH4, C2H4/C2H6, and C2H2/C2H4. From the obtained codes the faults are diagnosed.
Table IV: CEGB code determination Criteria
Gas ratio
Value
Code
W=CH4/H2
W<=0.1
5
0.1<W<1
0
1<=W<3
1
W>=3
2
X=C2H6/CH4
X<1
0
X>=1
1
Y=C2H4/C2H6
Y<1
0
1<=Y<3
1
Y>=3
2
Z=C2H2/C2H4
Z<0.5
0
0.5<=Z<3
1
Z>=3
2
Table V: Fault Diagnosis using CEGB codes
-
Rogers ratio method III (ASTM Standard)
-
In this standard a four digit code is generated based on the codes given in table using the Rogers method and the four gas ratios of C2H4/C2H6, C2H6/CH4, C2H2/C2H4, and CH4/H2 is considered.
Table VI: ASTM code determination criteria
Gas ratio
Value
Code
0<W<0.1
1
J=CH4/H2
0.1<W<1
1<=W<3
2
3
W>3
4
K=C2H6/CH4
X<1 X>1
0
1
Y<1
0
L=C2H4/C2H6
3<Y<1
1
Y>3
2
Z<0.5
0
M=C2H2/C2H4
3<Z<0.5
1
Z>=3
2
S.NO
Codes
W X Y Z
Kind of fault
Grouping of fault
1
0
0
0
0
No fault
F1
2
5
0
0
0
Partial discharge
F2
3
1 or
2
0
0
0
Increase in temperature less than equal to 150° C
F3
4
1 or
2
1
0
0
Increase in temperature 150 °C to
200 °C
F4
5
0
1
0
0
Increase in temperature 200°C-
300°C
F5
6
0
0
1
0
Increase in overall temperature in conductive parts
F6
7
1
0
1
0
Circulating currents in winding
F7
8
1
0
2
0
Circulating current between core and tank
F8
9
0
0
0
1
Spark with low energy discharge
F9
10
0
0
1 or
2
1 or 2
Spark with high energy discharge
F10
11
0
0
2
2
Continuous spark
F11
12
5
0
0
1 or 2
Partial discharge with tracking
F12
S.NO
Codes
W X Y Z
Kind of fault
Grouping of fault
1
0
0
0
0
No fault
F1
2
5
0
0
0
Partial discharge
F2
3
1 or
2
0
0
0
Increase in temperature less than equal to 150° C
F3
4
1 or
2
1
0
0
Increase in temperature 150 °C to
200 °C
F4
5
0
1
0
0
Increase in temperature 200°C-
300°C
F5
6
0
0
1
0
Increase in overall temperature in conductive parts
F6
7
1
0
1
0
Circulating currents in winding
F7
8
1
0
2
0
Circulating current between core and tank
F8
9
0
0
0
1
Spark with low energy discharge
F9
10
0
0
1 or
2
1 or 2
Spark with high energy discharge
F10
11
0
0
2
2
Continuous spark
F11
12
5
0
0
1 or 2
Partial discharge with tracking
F12
Table VII: Fault Diagnosis using ASTM codes
Sl.
No.
Codes
Kind of Fault
Grouping of fault
W
X
Y
Z
1
2
0
0
0
Normal
F1
2
1
0
0
0
Partial discharge
F2
3
3
0
0
0
Increase in temperature less than equal than 150 C
F3
4
4
0
0
0
Increase in temperature less than equal than 150 C
F3
5
3
1
0
0
Increase in temperature 150C-200C
F4
6
4
1
0
0
Increase in temperature 150C-200C
F4
7
4
0
1
0
Increase in temperature 200 C to 300 C
F5
8
2
0
1
0
Increase in temperature of conductor
F6
9
3
0
1
0
Circulating current in winding
F7
10
3
0
2
0
Circulating current between core and tank
F8
11
2
0
0
1
Spark with very low energy density
F9
12
2
0
1
1
Spark with high energy density
F10
13
2
0
1
2
Spark with high energy density
F10
14
2
0
2
1
Spark with high energy density
F10
15
2
0
2
2
Continuous spark
F11
16
1
0
0
1
Partial discharge with tracking
F12
-
-
DUVAL TRIANGLE METHOD
This method is more graphical method than ratio method. Duval triangle method uses concentration of the three key gases for the diagnosis of fault. These gases are CH4 (Methane), C2H4 (Ethylene), C2H2 (Acetylene).
The ratio of the gases is calculated using the expressions as below:
CH4% = (100 X) / (X+Y+Z) C2H4% = (100 Y) / (X+Y+Z) C2H2% = (100Z) / (X+Y+Z)
Where X = CH4 in p.p.m Y = C2H4 in p.p.m Z = C2H2 in p.p.m
These values are then plotted on the triangle. The point of interception falls into a zone in the triangle which depicts the fault in the transformer.
Fig I:
Where,
PD depicts Partial Discharge.
T1 depict thermal fault below 300°C.
T2 depict thermal fault between 300°C to 700°C T3 depict thermal fault with overhauling.
D1 depicts low energy discharge (Spark)
D2 depicts high energy discharge (Electric Arc)
DT depicts a mix between thermal and electric faults.
-
DOERNENBURG RATIO METHOD
This method utilizes the gas concentration from ratio of CH4/H2, C2H2/CH4, C2H4/C2H6, C2H2/C2H4.
Table VIII:Fault diagnosis using Doernenburg Ratio
M
N
O
P
CH4/H2
C2H2/C2H4
C2H6/C2H2
C2H2/CH4
Suggested Fault Diagnosis
>0.1
<0.75
>0.4
<0.3
Thermal Decomposition
<0.1
<0.001
>0.75
<0.4
>0.3
Corona (Low Intensity PD)
<0.1
<0.75
>0.4
<0.3
Arcing(High Intensity PD)
PROBLEM 1
DGA result of TATA STEEL, Jamshedpur (Tata Nagar). Equipment: 15/18.75 MVA
Make BHEL
Rated Voltage: 420/220/33 KV
Rated current: 434/526.6/837.03 Ampere
Table VIII: DGA result of Transformer
FAULTY GASES
Sl.
No.
H2
CH4
C2H6
C2H4
C2H2
CO
CO2
1
178
506
176
583
11.7
151
1844
2
315
865
510
2062
1
233
4851
3
383
1040
534
2315
2
233
4851
4
380
363
308
1700
61.5
48
1683
5
279
192
255
746
0
136
2831
6
695
1340
629
2720
2.5
335
5655
7
253
174
233
718
0
98
2477
8
5239
40972
6101
7784
233.9
588
5222
9
173
161
79
417
9.5
21
1000
ROGER'S RATIO
Fault Gases(IEC STANDARD)
RATIO
CODES
S.
No.
X
Y
Z
X
Y
Z
Kinds of Faults
1
0.02
2.84
3.312
0
2
2
Thermal fault with temp
>700ºC
2
0.0004
2.74
4.04
0
2
2
Thermal fault with temp
>700°C
3
0.0008
2.71
4.33
0
2
2
Thermal fault with temp
>700°C
4
0.0361
0.95
5.51
0
2
2
Thermal fault with temp
>700°C
5
0
0.688
2.92
0
2
1
Thermal fault having temp b/w 300 &
700°C
6
0.0009
1.928
4.32
0
2
2
Thermal fault with temp
>700°C
7
0
0.679
3.081
0
2
2
Thermal fault with temp
>700°C
8
0.030
7.82
1.275
0
2
1
Thermal fault having temp b/w 300 &700°C
9
0.022
0.93
5.27
0
2
2
Thermal fault with temp
>700°C
ROGER'S RATIO
Fault Gases(ASTM STANDARD)
Ratio
Codes
Fault
S.
No.
W
X
Y
Z
W
X
Y
Z
Kinds of Faults
1
2.84
0.347
3.312
0.020
3
0
2
0
Circulating current bet. core & tank
2
2.74
0.589
4.0431
0.00048
3
0
2
0
Circulating current bet. core & tank
3
2.715
0.513
4.335
0.00086
3
0
2
0
Circulating current bet. core & tank
4
0.955
0.848
5.5194
0.03617
2
0
2
0
No Result
5
0.688
1.328
2.925
0
2
1
1
0
No Result
6
1.928
0.4694
4.324
0.00091
3
0
2
0
Circulating current bet. core & tank
7
0.687
1.339
3.0815
0
2
1
2
0
No Result
8
7.82
0.1489
1.2758
0.030
4
0
1
0
No Result
9
0.93
0.4906
5.278
0.0227
2
0
2
0
No Result
ROGER'S RATIO
Fault Gases(ASTM STANDARD)
Ratio
Codes
Fault
S.
No.
W
X
Y
Z
W
X
Y
Z
Kinds of Faults
1
2.84
0.347
3.312
0.020
3
0
2
0
Circulating current bet. core & tank
2
2.74
0.589
4.0431
0.00048
3
0
2
0
Circulating current bet. core & tank
3
2.715
0.513
4.335
0.00086
3
0
2
0
Circulating current bet. core & tank
4
0.955
0.848
5.5194
0.03617
2
0
2
0
No Result
5
0.688
1.328
2.925
0
2
1
1
0
No Result
6
1.928
0.4694
4.324
0.00091
3
0
2
0
Circulating current bet. core & tank
7
0.687
1.339
3.0815
0
2
1
2
0
No Result
8
7.82
0.1489
1.2758
0.030
4
0
1
0
No Result
9
0.93
0.4906
5.278
0.0227
2
0
2
0
No Result
Table X: Diagnose of fault by ASTM method
Table IX: Diagnose of fault by IEC method
ROGERS RATIO
Fault Gases(CEGB STANDARD)
Ratio
Codes
Fault
S.
No
W
X
Y
Z
W
X
Y
Z
Kinds of Faults
1
2.84
0.347
3.312
0.020
1
0
2
0
Circulating current bet. core & tank
2
2.74
0.589
4.0431
0.00048
1
0
2
0
Circulating current bet. core & tank
3
2.715
0.513
4.335
0.00086
1
0
2
0
Circulating current bet. core & tank
4
0.955
0.848
5.5194
0.03617
0
0
2
0
No Result
5
0.688
1.328
2.925
0
0
1
1
0
No Result
6
1.928
0.4694
4.324
0.00091
1
0
2
0
Circulating current bet. core & tank
7
0.687
1.339
3.0815
0
0
1
2
0
No Result
8
7.82
0.1489
1.2758
0.030
2
0
1
0
No Result
9
0.93
0.4906
5.278
0.0227
0
0
2
0
No Result
ROGERS RATIO
Fault Gases(CEGB STANDARD)
Ratio
Codes
Fault
S.
No
W
X
Y
Z
W
X
Y
Z
Kinds of Faults
1
2.84
0.347
3.312
0.020
1
0
2
0
Circulating current bet. core & tank
2
2.74
0.589
4.0431
0.00048
1
0
2
0
Circulating current bet. core & tank
3
2.715
0.513
4.335
0.00086
1
0
2
0
Circulating current bet. core & tank
4
0.955
0.848
5.5194
0.03617
0
0
2
0
No Result
5
0.688
1.328
2.925
0
0
1
1
0
No Result
6
1.928
0.4694
4.324
0.00091
1
0
2
0
Circulating current bet. core & tank
7
0.687
1.339
3.0815
0
0
1
2
0
No Result
8
7.82
0.1489
1.2758
0.030
2
0
1
0
No Result
9
0.93
0.4906
5.278
0.0227
0
0
2
0
No Result
Table X1: Diagnose of fault by CEGB method Table XII: Diagnosis of fault using DUVAL Triangle method
DUVAL TRAINGLE METHORD
PERCENTAGE
FAULTS
Sl. No
%CH4
%C2H2
%C2H4
TRANSFORMER FAULT DIAGNOSIS
1
45.84
52.82
1.06
Thermal fault with temp >700° C
2
29.54
70.42
0.03
Thermal fault with temp >700° C
3
30.98
68.96
0.059
Thermal fault with temp >700° C
4
17.08
80.01
2.89
Thermal fault with temp >700° C
5
20.46
79.53
0
Thermal fault with temp >700° C
6
32.98
66.95
0.061
Thermal fault with temp >700° C
7
19.50
80.49
0
Thermal fault with temp >700° C
8
83.63
15.88
0.477
Thermal fault below 700° C
9
27.40
70.97
1.617
Thermal fault with temp >700° C
Table XIII: Fault Diagnose of fault by Doernenburg ratio method.
DOERNENBURG RATIO
RATIO
FAULT
Sl. No
M
N
O
P
TRANSFORMER FAULT DIAGNOSIS
1
2.84
0.020
15.04
0.023
Thermal Decomp
2
2.74
0.00048
510
0.0011
Thermal Decomp
3
2.715
0.00086
267
0.00192
Thermal Decomp
4
0.955
0.03617
5
0.169
Thermal Decomp
5
0.688
0
N.R.
p>0 Thermal Decomp
6
1.928
0.00091
251.6
0.00186
Thermal Decomp
7
0.687
0
N.R.
0
Thermal Decomp
8
7.82
0.030
26.08
0.005708
Thermal Decomp
9
0.93
0.0227
8.31
0.0590
Thermal Decompo
-
CONCLUSION
In this thesis the analysis of dissolved gas of transformer is used to diagnose the fault in the transformer using Rogerss ratio through IEC, CEGB, ASTM standards parallel with DUVAL triangle and Doernenburg method. These techniques are implemented for better decision on the power transformer state and classification of power transformer fault using dissolved gas analysis as input data. It is presented here that how one technique is superior over the other for diagnosing the fault of the transformer in the most convenient manner. This shows great promise in that a number of faults likely to cause future trouble in service have been detected, although in each case the transformer had satisfactorily passed the routine tests. The technology presently exists and is being used to detect and determine fault gases below the part per million levels. However there is still much room for improvement in the technique, especially in developing the methods of interpreting the results and correlating them with incipient faults.
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