+ All Categories
Home > Documents > Review of lecture 4

Review of lecture 4

Date post: 23-Jan-2016
Category:
Upload: beyla
View: 36 times
Download: 0 times
Share this document with a friend
Description:
Review of lecture 4. Contents:. The Basic Parameters The Integrated Quantities The Inception and Distinction Voltages Waveform Characteristics of Discharges. Basic Parameters. Review of lecture 4. Integrated Quantities. u i and u e. For oil-impregnated paper, u i >u e. - PowerPoint PPT Presentation
Popular Tags:
24
1 Review of lecture 4 1. The Basic Parameters 2. The Integrated Quantities 3. The Inception and Distinction Voltages 4. Waveform Characteristics of Discharges Contents: Basic Parameters c b c r u C C q ) ( c b a u C q r c b b a q C C C q c b b B m C C C c U u f fn N 4 4 a im q u W 2 1
Transcript
Page 1: Review of lecture 4

1

Review of lecture 4

1. The Basic Parameters

2. The Integrated Quantities

3. The Inception and Distinction Voltages

4. Waveform Characteristics of Discharges

Contents:

Basic Parameters

cbcr uCCq )(

cba uCq

rcb

ba q

CC

Cq

cb

b

B

m

CC

C

cU

uffnN

44

aimquW2

1

Page 2: Review of lecture 4

2

|]||||[|1

21 amaa qqqT

I

Integrated Quantities

][1 22

221 amaa qqq

TD

][1

2211 mamaa uququqT

P

ui and ue

Review of lecture 4

q

u

eu iuFor oil-impregnated paper, ui >ue

Page 3: Review of lecture 4

3

Estimation of ui for several typical internal discharges:

Review of lecture 4

a dielectric with a flat cavityU

+

c

b

b

aadU

+

c

b

b

aad

CBrb

rci Edu ])([

a dielectric with a spherical cavityd c b

]3

)2([

rb

rcrbCBi

dEu

r 1

r 2

r

the flat cavity in a cylindrical

)]1ln()1

1()1ln(1

[1

2

rr

rrEu

rbrbCBi

Page 4: Review of lecture 4

4

Review of lecture 4

Waveform Characteristics of Discharges

q

0

9 0

1 8 0

2 7 0

0

9 0

1 8 0

2 7 0

q

a b

c

+

_

q

0

9 0

1 8 0

2 7 0

Surface discharge

Corona discharge

0

9 0

1 8 0

2 7 0

0

9 0

1 8 0

2 7 0

Internal discharge

Page 5: Review of lecture 4

5

Lecture 5 Dielectric Deterioration and PD Evaluation

Page 6: Review of lecture 4

6

ContentsContents

1. Mechanisms of Dielectric Aging by PD

2. Process of Dielectric Aging by PD

3. The Influence Factors on Aging Rate

4. PD Evaluation Approaches

局部放电老化机理

局部放电老化过程

影响老化的因素

局部放电评估方法

Page 7: Review of lecture 4

7

1. Mechanisms of Dielectric Aging by PD

Electrical aging is a type of dielectric deterioration under the long-term

electrical field and due to the fact of partial discharges.电老化:在电场长期作用之下因局部放电而造成的绝缘性能劣化。(1) Bombardment of charged particle 带电质点轰击

(2) Thermal Effect 热效应

(3) Resultant of Reaction 反应生成物

(4)(4) Radiation Effect Radiation Effect 辐射效应辐射效应

(5)(5) Mechanical Effect Mechanical Effect 机械效应机械效应

Broke the chemical bond and damage molecular structure of insulation material .

High temperature of discharge point accelerates thermal damage to materials

resultants, such as ozone, moisture, nitric acid, oxalic acid , erode materials.

visible light, ultraviolet radiation, X-radial,γ-radial embrittle materials.

Successive blasting discharges result in high gas pressure and crack the materials

Page 8: Review of lecture 4

8

2.Process of Dielectric Aging by PD

2.1 Damage of internal discharge to polymer 内部放电对聚合物的破坏

(1) Surface Erosion

A uniform surface erosion, which may be caused by bombardment of particle, thermal degradation, radiation and trapped electrons below surface, etc. Deep pits are formed and carbonized. Discharges become concentrated, some deep pits are formed, the discharges further concentrate and sometimes carbonization of the pits occurs.

在放电的各种效应作用下,逐步腐蚀气隙表面

In nitrogen gasIn air

放电集中的地方,形成一些深坑;放电进一步集中,并造成一些深坑碳化

表面腐蚀

Page 9: Review of lecture 4

9

2.Process of Dielectric Aging by PD

(2) Propagation of electrical tree 树枝放电的发展The dielectric breaks down over a distance of some microns. The stress at the top of the pit approaches the breakdown strength over a distance of some microns owing to the field concentration around this sharp tip.

complete breakdown. The field concentration moves to the new tip and narrow carbonization channels propagate quickly through the dielectric, initiating complete breakdown.

深坑端部一定距离内场强集中,达到了击穿场强,这些区域发生击穿。

击穿造成了新的深坑端部电场集中,碳化的狭窄通道很快在介质中发展,最后介质完全击穿。

Page 10: Review of lecture 4

10

2.Process of Dielectric Aging by PD

Simulation of electrical tree in XLPE cable

Two configurations of electrical tree

branched type brush type tree 刷状 丛林状

Page 11: Review of lecture 4

11

Development of treeing discharges

2.Process of Dielectric Aging by PD

( a ) inception ( b ) branch growing ( c ) reaching to the opposite electrode

( d ) complete breakdown

Page 12: Review of lecture 4

12

2.Process of Dielectric Aging by PD

2.2 Damage of internal discharge to oil-paper

(1)Discharges in void adjacent to the conductor attack the insulation. After some time, discharge penetrate the first layer.

(3)The tracks follow the weakest points in the insulation.

在靠近导体的气隙处发生放电,轰击绝缘表面。一段时间之后,放电穿透第一层纸

在绝缘纸存在薄弱点时,碳化轨迹容易穿透绝缘纸 .

(2) Surface discharges occur along the layers after penetrating the first few paper layers, and trees or carbonized tracks are formed.沿着层间纸的表面发生沿面放电,形成树枝或碳化通道

碳化通道达到一定的长度,击穿发生。(4)The tracks finally attain enormous lengths, ultimate breakdown occurs.

Page 13: Review of lecture 4

13

3. The Influence Factors on Aging Rate

3.1 Electrical field stress 电场强度nKEL

log(E)

log(L)

a

b

c

d EnKL logloglog

The principle of accelerating aging tests:

(Lb, Lc, Ld) at higher stresses (Eb, Ec, Ed) to , extrapolate La at lower stress Ea

3.2 Voltage frequency 电压频率

cb

b

B

m

CC

C

cU

uffnN

44

Page 14: Review of lecture 4

14

3. The Influence Factors on Aging Rate

3.3 Situation of cavity and gas contents inside 气隙状态及成分

d c b a

HV

e

(a) Single flat cavity parallel with electric field.

(b) Single flat cavity , perpendicular with electric field.

(c) Double cavities, in series in the direction of electric field.

(d) Double cavities, in parallel in the direction of electric field.

单个扁平气隙,平行电场方向单个扁平气隙,垂直于电场方向

两个串联气隙两个并联气隙

(e) Cavities, adjacent to electrodes. 紧邻金属电极的气隙

( a ) is more harmful than (b)( c ) is more harmful than (d)( e ) is more harmful than the cavities bounded by dielectric.

Page 15: Review of lecture 4

15

3. The Influence Factors on Aging Rate

3.4 Temperature and humidity 温度和湿度

the upper limited operating temperature of insulation. 绝缘的最高允许工作温度。

heat resistant grades of insulation 绝缘耐热等级

G ra d e Y A E B F H C

Pe rmiss ib le

te mp e ra tu re (oC )9 0 1 0 5 1 2 0 1 3 0 1 5 5 1 8 0 >1 8 0

3.5 Mechanical force 机械应力

)exp(RT

EAk aa Ea - activation energy (kJ/mol-1)

k - aging rate

Aa - pre-exponential factor

T – temperature (K)

宅急修
绝缘材料在此温度下工作,能在预定使用期内保持其性能不超出允许的范围。
Page 16: Review of lecture 4

16

4. PD Evaluation Approaches

4.1 Estimation by the basic parameters

(1) Apparent charge, qa

The maximum qa at 1~1.5 rated voltage of HV equipment should be smaller than the permissible discharge magnitude.

通常在 1~1.5 倍额定电压下测量设备视在放电量,需小于规定的允许放电水平Disadvantages:(1) The qr is quite different with qr 视在放电量和真实放电量有差别 r

cb

ba q

CC

Cq

(2) qa is often transient and fluctuant. qa 是瞬变的和无规则波动的

(3) qa only indicates the maximum of discharge magnitude corresponding to the defects in the largest size. 仅代表最大缺陷中的最大放电量

(2) Discharge energy and power, W and P

Page 17: Review of lecture 4

17

4. PD Evaluation Approaches

(3) The phase angle of pulses When partial discharges act more excitedlythe pulses occur at the wider range of phase angle. 放电相位变宽Inception pulses will shift to zero or a negative phase angle. 起始脉冲 朝着过零点或者负半周移动Average phase angle of pulses in a power-frequency half cycle also becomes smaller. 平均放电相位也变小

(4) Ui and Ue Under the same test voltage, higher discharge magnitude or more pulses exist in the tested equipment with smaller inception and extinction voltages.

在同样的实验电压下, ui 越低,放电量 qa 越大,放电次数 n 也就越多

Page 18: Review of lecture 4

18

4. PD Evaluation Approaches

4.2 Estimation by distribution (statistical) graphs采用分布 (统计 )图谱评定

t

q a( t )

q i

t i

u i

))(,( iii tutq )),(,,( iiiii nunq

ff

nt iii 360

Every PD activity is a sequence of PD pulses qi(ti)

0 0.002 0.004 0.006 0.008 0.010 0.012 0.014 0.016 0.018 0.020

-0.5

0

0.5

Page 19: Review of lecture 4

19

4. PD Evaluation Approaches

(1) q-φ graph , H(q, φ)

q

0 0.002 0.004 0.006 0.008 0.010 0.012 0.014 0.016 0.018 0.020

-0.5

0

0.5

t

0 50 100 150 200 250 300 3500

0.2

0.4

0.6

0.8

φ

The average, (maximum, sum) pulse height distribution: the average (maximum, sum) amplitude in each phase window as a function of the phase angle,

The phase range is divided into 2n parts firstly, each part is a phase window.

0 50 100 150 200 250 300 3500

0.2

0.4

0.6

0.8

q ave

统计每个相位窗中的放电量平均(最大,之和)值

放电量 -相位分布图

Page 20: Review of lecture 4

20

(2) n-φ graph , H(n, φ)

4. PD Evaluation Approaches

The pulse count distribution: the number of observed discharges in each phase window as a function of the phase angle.

放电次数 -相位分布图

0 50 100 150 200 250 300 3500

0.2

0.4

0.6

0.8

φ

统计每个相位窗中的放电次数

0 50 100 150 200 250 300 3500

2

4

6

8

10

12

N (

tim

es)

Page 21: Review of lecture 4

21

4. PD Evaluation Approaches

(3) n-q graph , H(n, q)The q range is divided into 2n parts firstly, each part is a q window.

the number of observed discharges in each q window as a function of the discharge magnitude.

将放电量等分为 2n 份,每一份为一个放电量窗

统计每个一个放电量窗中脉冲的个数

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.80

10

20

30

40

q(mV)

N(t

imes

)

(4) w-n graph , H(w, n)

iiquW2

1

the number of observed discharges in each w window as a function of the discharge energy.

Page 22: Review of lecture 4

22

4. PD Evaluation Approaches

4.3 parameters extracting from graphs (statistic operators)

图谱的特征参数提取 ( 统计算子 )(1) Skewness, sk 偏斜度

f(x)

x

f(x)

x

f(x)

x

( a ) sk>0 ( b ) sk=0 ( c ) sk<0

3

3)(

ii px

Sk

ii

iii

iiii

px

px

xxp

22 )(

/

(2) kurtosis, ku 陡峭度

4

4)(

ii pxku

(3)others 其他

Page 23: Review of lecture 4

23

4. PD Evaluation Approaches

4.3q-u hysteresis curve Q-u 迟滞曲线

q

u

eu iu

The area surrounded by curve. Larger area means poorer performance to absorb gas

Δu=ui-ue. Difference of ui and ue.曲线包围面积,越大材料吸气性能越差

Page 24: Review of lecture 4

24

The end


Recommended