Effect of High Frequency Pulses on the Breakdown Voltage
Download
Report
Transcript Effect of High Frequency Pulses on the Breakdown Voltage
Electrical Power Engineering Department
Hijjawi Faculty of Engineering Technology
Yarmouk University
Irbid, Jordan
Effect of High Frequency Pulses on the
Breakdown Voltage and Lifetime of
MW Insulation of Flyback Transformer
Eyad A. Feilat, Ph.D.
US-Jordan Workshop
Modern Power Electronics Research and Education
December 16-17, 2002, PSUT, Amman, Jordan
Outline
Design Trends in Electrical and Electronics Equipment
Insulation System of Flyback Transformer
Consequences of Miniaturized Design
Statistical Analysis of Failures
Scope of the Research Paper
Accelerated Aging Test System
Experimental Results
Conclusion
Design Trends in
Electrical and Electronics Equipment
Reduce Size (Compact Design)
Light Weight
High Reliability (Low Failure Rates)
Reduce Manufacturing Time
Reduce Cost
Design Trends in
Electrical and Electronics Equipment
Bobbin-Wound Coils
Fine Gauge Magnet Wires
Thin Layers of Insulation
Encapsulation of HV Coils
Materials with High Thermal Class
High Frequency Switching Technology
DC-DC Converters (Flyback Transformers)
DC-AC Inverters (Adjustable Speed Drives)
DC-DC Converter
Flyback Transformer (FBT)
B+
+HV
HOT
Fine Gauge Magnet Wires (MW)
TV sets and computer monitors.
Pulse Frequencies of FBT
Application
of
Flyback Transformer
General (60 Hz)
General (50 Hz)
TV
HDTV (60 Hz)
HDTV (50 Hz)
Computers
Monitors
Displays
Number
of
Scanning Lines
525
625
1125
1250
various
various
Horizontal Deflection
(Flyback)
Frequencies (kHz)
15.75
15.625
33.8
31.3
24~50
60~90
Insulation System of Encapsulated Coil
Polyester Housing Layer (Polyethylene Terephthelate)
Impregnation Layer (Epoxy)
Heavy Build Enamel (Polyurethane)
Polyester Bobbin
(Polyethylene Terephthelate)
Randomly Wound on Bobbins
Bonded with Baked Coatings
Encapsulated with Epoxy
Magnet Wire (MW)
Insulation Material: polyurethane (PUR)
Over Coat: Polyamide (Nylon)
NEMA MW-80C, Class F
AWG 41 MW
Insulation Thickness = 6.35 m
Bare Wire Diameter = 71.1 m
Consequences of Miniaturized Design
Random Wound Coils
Beginning and End of the Coil may touch one another
High Level of Voltage Stress between Turns
High Frequency Switching
Very Short Pulse Period
Very Short Duty Cycle
High dV/dt
Uneven Voltage Distribution
Steady Degradation of the MW Enamel
High Temperature Rise, typically 100o-200o C
Causes of Insulation Failure
Electrical and Thermal Stresses
Partial Discharge Developed in Random Windings
Localized Dielectric Heating
Microvoids and Impurities in the Epoxy Fill Material
Insulation Degradation
Premature Failure
Statistical Analysis of Failures
Accelerated Life Tests (Accelerated Aging)
High Electrical Stresses
Elevated Temperatures
Combined Electrical and Thermal Stresses
Various Voltage Waveform and Frequencies
Statistical Analysis of Failures
Probability Distribution (Weibull)
x
f ( x ; , )
1
x
exp
Life Model (Single Stress, Multistress)
B1 B2V
L(V,T) exp A1 A2V
T
Scope of the Study
Effect of Rise Time on the Time-to-Failure
Effect of Duty Cycle on the Time-to-Failure
Evaluation of the Breakdown Voltage
Accelerated Life Tests
High Temperature (100o -180o C )
Pulsating Frequency (15-40 kHz)
Positive Polarity
Accelerated Aging System
DTS-1500 A
Computer
Air-Circulating
Oven
High Frequency
Pulse Generator
Typical Pulse Waveform
D
V
T
Experimental Results
Lifetime Studies
Effect of Duty Cycle
Effect of Rise Time
Effect of Duty Cycle
250
V = 950 V
f = 15 kHz
200
Time-to-Breakdown (s)
T = 100o C
= 200 ns
150
100
50
0
10
15
20
25
30
35
Duty Cycle %
40
45
50
55
Effect of Rise Time
250
V = 950 V
f = 15 kHz
Time-to-Breakdown (s)
200
T = 100o C
D = 16%
150
100
50
0
0
50
100
150
Rise Time (ns)
200
250
Experimental Results
Breakdown Voltage Studies
Effect
of Temperature
Effect
of Frequency
Effect of Temperature on the
Breakdown Voltage
2000
f = 15 kHz
1800
f = 25 kHz
f = 40 kHz
Voltage (V)
1600
1400
1200
1000
800
75
100
125
150
Temperature (oC)
175
200
D = 16%
=200 ns
Effect of Frequency on the
Breakdown Voltage
2000
1800
T=100 C
D = 16%
T=155 C
=200 ns
Voltage (V)
T=180 C
1600
1400
1200
1000
800
10
20
30
40
Pulsating Frequency (kHz)
50
Experimental Results
Lifetime Studies
Effect
of Pulsating Voltage
Effect of Temperature
Effect of Frequency
Lifetime Characteristics
V-t C/C
1.0E+8
155o C
f=15kHz
1.0E+7
180o C
100o C
T i m e (s )
1.0E+6
1.0E+5
1.0E+4
1000.0
100.0
10.0
700.0
760.0
820.0
Voltage (V)
880.0
940.0
1000.0
Lifetime Characteristics
V-t C/C
1.0E+8
25 kHz
T=155o C
15 kHz
1.0E+7
40 kHz
Time (s)
1.0E+6
1.0E+5
1.0E+4
1000.0
100.0
600.0
680.0
760.0
Voltage (V)
840.0
920.0
1000.0
Lifetime Characteristics
T-t C/C
1.0E+12
900 V
1.0E+11
800 V
700 V
f=15kHz
1.0E+10
1.0E+9
T i m e (s )
1.0E+8
1.0E+7
1.0E+6
1.0E+5
1.0E+4
1000.0
100.0
10.0
100.0
1000.0
Temperature (K)
Lifetime Characteristics
T-t C/C
1.0E+12
40 kHz
1.0E+11
V=800 V
25 kHz
15 kHz
1.0E+10
Time (s)
1.0E+9
1.0E+8
1.0E+7
1.0E+6
1.0E+5
1.0E+4
100.0
1000.0
Temperature (K)
Parameters of the
Electrical-Thermal Aging Model
f kHz
A1
A2
B1
B2
15
25
40
0.49
0.46
0.53
136.2
16.03
17.29
-0.167
-0.026
-0.028
-20846
14312
6412.5
32.51
-9.22
0.027
B1 B2V
L(V,T) exp A1 A2V
T
Conclusion
The
longer the duty, the shorter is the insulation
Lifetime
The
longer the rise time, the longer is the insulation
lifetime
The
Breakdown Voltage declines with the increase
of both the Frequency and Temperature
The Accelerated
Life Tests show that both the Voltage
and Temperature are the two main Factors of
Insulation Aging or Degradation
Conclusion
Effect of the pulse frequency on the lifetime is
indistinct
It changes with temperature and voltage stress
Reason:
Change of polarization
Space charge
Dielectric losses
Change of Breakdown Mechanisms