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电力系统之输电线路和电缆:Transmission Lines and Cables [2]

论文作者:留学生论文论文属性:案例分析 Case Study登出时间:2011-01-30编辑:anterran点击率:8013

论文字数:3615论文编号:org201101300958244804语种:英语 English地区:美国价格:免费论文

附件:20110130095824568.pdf

关键词:Transmission Lines and CablesFundamentalspower system

e representation
S2: Transmission Lines
13 EEE8044: Fundamentals
2.2 Relationships between Line Parameters and Physical Layout
2.2.1 Line inductance
Fig. 2.6 shows the relationship between physical layout of a three phase overhead line and
its’ series line inductance.
a
b
c
dab
dca
dbc
L
D
R
H m
where
permeability of space H m
R effective conductor radius
D geometric mean dis ce d d d ab bc ca
=
⎧⎨⎩
⎫⎬⎭
= = ×
=
= = × ×

− −
μ
π
μ π
0 1
0
7 1
3
2
4 10
.ln .
:
.
tan
Fig. 2.6 Line inductance
To simplify operation of the power system it is desirable to have low values of inductance,
i.e. small D and large R.
Decreasing D reduces the insulation between lines and is therefore limited by the working
voltage.
Increasing R causes an increase in conductor weight and therefore cost.
One method employed to increase the effective radius is the use of bundle conductors, as
shown in Fig. 2.7.
Cross-section of line for one-phase in the UK transmission system:
275kV
approx 30cms
400kV
approx 30cms
Fig. 2.7 Bundle conductors
S2: Transmission Lines
14 EEE8044: Fundamentals
In comparison to a single solid conductor, bundle conductors:
􀂃 increase effective radius and therefore reduce inductance
􀂃 reduce skin effect
􀂃 have a larger surface area and therefore better cooling
􀂃 are easier to handle during construction
2.2.2 Line resistance
The resistance of a line varies between 0.5Ω/km for an 11kV distribution line and
0.015Ω/km for a 400kV overhead line or a 33kV underground cable.
Resistance includes skin effect, which causes an increase in resistance of about 5% (in
comparison to dc) in a 2.5cm diameter copper conductor operating at 50 Hz.
2.2.3 Line capacitance
The capacitance per unit length of the line shown in Fig. 2.6 above is given by the
equation:
(D R)
C
ln /
2 0 πε
=
for a given working voltage and frequency, dv/dt is fixed, so to minimise charging current,
i (i = C dv/dt), the line capacitance should be as small as possible. A low value of C
implies large D and small R conflicting with the requirements for small L.
Typical values for capacitive reactance (1/ωC) are 200kΩ/km for a transmission line and
4kΩ/km for an underground cable. The capacitive charging current in an underground
cable is thus much higher than in an overhead transmission line.
2.2.4 Line conductance
Line shunt conductance G models losses due to corona (discharge through air) and leakage
currents across insulator surfaces. Typical losses on a 400KV line are 600 W/km in fine
weather and 90 kW/km in snow or fog.
S2: Transmission Lines
15 EEE8044: Fundamentals
2.3 Underground Cables vs. Overhead Lines
Cables are 15-20 times more expensive than overhead lines, because:
􀂃 insulation cost (overhead lines uses air insulation, which is free)
􀂃 the maximum operating temperature for a cable is typically 70 or 90°C, so more copper
must be used to reduce losses and give a reasonable operating temperature
􀂃 installation cost: trench, continuous path across the ground
Plus, the large capacitive charging current limits useful lengths of cables to 15-20 km. For
longer lengths of cable (e.g. under th论文英语论文网提供整理,提供论文代写英语论文代写代写论文代写英语论文代写留学生论文代写英文论文留学生论文代写相关核心关键词搜索。
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