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POWER SYSTEMS NEVER MISS A FORMULA

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NEVER MISS A FORMULA SERIES
FORMULA BOOK
POWER
SYSTEMS
MADURA COACHING
#62, Rakame Complex,
T.P.K Road, Madurai-625011
______________________________________________________________________________
Unit - I Generating Power
Stations
1)
Water power p =
0.736
75
iv.
Qπœ‚H kW
Q → Discharge : π‘š3 /sec
H → Water head : m
πœ‚ = Overall efficiency
v.
𝑁√𝑃𝑑
𝑁𝑠 → Specific speed in metric units
N → Speed of turbine in rpm
𝑃𝑑 = Output in metric h.p
H → effective head in metres
3)
Base
load
High
Peak
load
4)
Low
Fuel
cost
Low
Typical
annual
load
factor
Type of
Plant
65-75
Nuclear,
thermal
5-10
Gas,
hydro,
pump
storage
High
For thermal power station:
i. πœ‚π‘‘β„Žπ‘’π‘Ÿπ‘šπ‘Žπ‘™
=
iii. Overall efficiency
πœ‚π‘œπ‘£π‘’π‘Ÿπ‘Žπ‘™π‘™ =
π»π‘’π‘Žπ‘‘ π‘’π‘žπ‘’π‘–π‘£π‘Žπ‘™π‘’π‘›π‘‘
π‘œπ‘“ π‘’π‘™π‘’π‘π‘‘π‘Ÿπ‘–π‘π‘Žπ‘™
π‘œ/𝑝
π»π‘’π‘Žπ‘‘ π‘œπ‘“
π‘π‘œπ‘šπ‘π‘’π‘ π‘‘π‘–π‘œπ‘› π‘œπ‘“
π‘π‘œπ‘Žπ‘™
iv. Overall efficiency
= Thermal efficiency × electrical
efficiency
v. Energy output = Coal consumption
× calorific value
= coal consumption × 6500 K.cal
π‘€π‘Žπ‘₯π‘–π‘šπ‘’π‘š π‘‘π‘’π‘šπ‘Žπ‘›π‘‘
πΆπ‘œπ‘›π‘›π‘’π‘π‘‘π‘’π‘‘ π‘™π‘œπ‘Žπ‘‘
Hydro power station:
i. Metric output =
π΄π‘£π‘’π‘Ÿπ‘Žπ‘”π‘’ π‘™π‘œπ‘Žπ‘‘
π‘ƒπ‘’π‘Žπ‘˜ π‘™π‘œπ‘Žπ‘‘
π‘Šπ‘„π» × πœ‚
75
(H.P)
1 H.P = 75 kg - m/sec
π‘†π‘’π‘š π‘œπ‘“ π‘–π‘›π‘‘π‘–π‘£π‘–π‘‘π‘’π‘Žπ‘™
π‘šπ‘Žπ‘₯π‘–π‘šπ‘’π‘š π‘‘π‘’π‘šπ‘Žπ‘›π‘‘
π‘€π‘Žπ‘₯π‘–π‘šπ‘’π‘š π‘‘π‘’π‘šπ‘Žπ‘›π‘‘
π‘œπ‘“ π‘”π‘Ÿπ‘œπ‘’π‘
ii. Metric output in watt =
π‘Šπ‘„π» × πœ‚
75
× 735.5
iii. Volume of water = Catchment
(Diversity factor > 1)
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π»π‘’π‘Žπ‘‘ π‘’π‘žπ‘’π‘–π‘£π‘Žπ‘™π‘’π‘›π‘‘ π‘œπ‘“ π‘šπ‘’π‘β„Ž−π‘’π‘›π‘’π‘Ÿπ‘”π‘¦
π‘‘π‘Ÿπ‘Žπ‘›π‘ π‘šπ‘–π‘‘π‘‘π‘’π‘‘ π‘‘π‘œ π‘‘π‘’π‘Ÿπ‘π‘–π‘›π‘’
π»π‘’π‘Žπ‘‘ π‘œπ‘“ π‘π‘œπ‘Žπ‘™ π‘π‘œπ‘šπ‘π‘’π‘ π‘‘π‘–π‘œπ‘›
ii. πœ‚π‘‘β„Žπ‘’π‘Ÿπ‘šπ‘Žπ‘™ = πœ‚π‘π‘œπ‘–π‘™π‘’π‘Ÿ × πœ‚π‘‘π‘’π‘Ÿπ‘π‘–π‘›π‘’
(Demand factor < 1)
iii. Diversity factor=
π‘€π‘Žπ‘₯π‘–π‘šπ‘’π‘š π‘™π‘œπ‘Žπ‘‘
5)
6)
ii. Load factor =
× π‘™π‘œπ‘Žπ‘‘ factor
Utilization factor = π‘…π‘Žπ‘‘π‘’π‘‘ π‘π‘™π‘Žπ‘›π‘‘ π‘π‘Žπ‘π‘Žπ‘π‘–π‘‘π‘¦
Operational factors:
i. Demand factors =
π‘€π‘Žπ‘₯π‘–π‘šπ‘’π‘š
π‘™π‘œπ‘Žπ‘‘
π‘ƒπ‘™π‘Žπ‘›π‘‘
π‘π‘Žπ‘π‘Žπ‘π‘–π‘‘π‘¦
vi.
Q → Quantity of water flow π‘š3 /sec
g → Acceleration due to gravity =
9.81m/𝑠𝑒𝑐 2
H → Water head, metre
𝜌 → density of water
Capital
cost
π΄π‘£π‘’π‘Ÿπ‘Žπ‘”π‘’ π‘Žπ‘›π‘›π‘’π‘™π‘Žπ‘™
π‘™π‘œπ‘Žπ‘‘
π‘…π‘Žπ‘‘π‘’π‘‘ π‘π‘™π‘Žπ‘›π‘‘
π‘π‘Žπ‘π‘Žπ‘π‘–π‘‘π‘¦
Capacity factor = Load factor ×
Utilization factor
Tidal power output P = Q𝜌gH Watts
Type
of
Load
Capacity factor =
Capacity factor =
Specific speed 𝑁𝑠 = 𝐻1.25
2)
Peak diversity factor
π‘€π‘Žπ‘₯π‘–π‘šπ‘’π‘š π‘‘π‘’π‘šπ‘Žπ‘›π‘‘
π‘œπ‘“ π‘Ž π‘π‘œπ‘›π‘ π‘’π‘šπ‘’π‘Ÿ π‘”π‘Ÿπ‘œπ‘’π‘
=
π·π‘’π‘šπ‘Žπ‘›π‘‘ π‘œπ‘“ π‘‘β„Žπ‘’ π‘π‘œπ‘›π‘ π‘’π‘šπ‘’π‘Ÿ π‘”π‘Ÿπ‘œπ‘’π‘
π‘Žπ‘‘ π‘‘β„Žπ‘’ π‘‘π‘–π‘šπ‘’ π‘œπ‘“ π‘π‘’π‘Žπ‘˜ π‘‘π‘’π‘šπ‘Žπ‘›π‘‘
1
available
area × Annual
per annum
Rainfall
POWER SYSTEMS
MADURA COACHING
#62, Rakame Complex,
T.P.K Road, Madurai-625011
______________________________________________________________________________
iv. Electric energy
= weight × head
generated
× overall πœ‚
7)
Gas turbine power plant:
i. Engine efficiency πœ‚π‘’π‘›π‘”π‘–π‘›π‘’π‘  =
πœ‚π‘œπ‘£π‘’π‘Ÿ π‘Žπ‘™π‘™
πœ‚π‘Žπ‘™π‘‘
ii. Heat produced by = coal consumption
𝐷𝑠 =
per day × calorific
fuel per day
9
√(𝐷𝑠 . 𝑑. 𝑑)3 = 3√(𝐷𝑠 . 𝑑)2
iii. For four conductor arrangement
value
Unit - II Transmission and
distribution
1)
String efficiency
π‘‰π‘œπ‘™π‘‘π‘Žπ‘”π‘’ π‘Žπ‘π‘Ÿπ‘œπ‘ π‘  π‘‘β„Žπ‘’
π‘€β„Žπ‘œπ‘™π‘’ π‘ π‘‘π‘Ÿπ‘–π‘›π‘”
=
𝑛 × π‘‰π‘œπ‘™π‘‘π‘Žπ‘”π‘’ π‘Žπ‘π‘Ÿπ‘œπ‘ π‘  π‘‘β„Žπ‘’ 𝑒𝑛𝑖𝑑
π‘Žπ‘‘π‘—π‘Žπ‘π‘’π‘›π‘‘ π‘‘π‘œ 𝑙𝑖𝑛𝑒
π‘π‘œπ‘›π‘‘π‘’π‘π‘‘π‘œπ‘Ÿπ‘ )
16
𝐷𝑠 = √(𝐷𝑠 . 𝑑. 𝑑. 𝑑√2)
4
= 1.09 × √𝐷𝑠 . 𝑑3
6)
n→number of insulator discs in the
string
2)
Capacitance canculation:
i. Capacitance of Two wire line
–q
b
+q
a
Inductance of a single phase two wire
line
D
𝐷
π‘Ÿ
L = 4× 10−7 𝑙𝑛 ( 1 ) H/m
3)
πΆπ‘Žπ‘ =
Inductance of composite Conductor
lines
ii. Line to neutral capacitance
−7
𝐷
π‘Ÿ
π‘™π‘œπ‘”( )
πœ‡πΉ/π‘˜π‘š
πΆπ‘Žπ‘› =𝐢𝑏𝑛 =2πΆπ‘Žπ‘
𝐺𝑀𝐷
𝑙𝑛 (𝐺𝑀𝑅 )
iii. Capacitance of 3πœ™ line with
οƒ˜ equilateral spacing 𝐢𝑛 =
Inductance of 3Ο• line with equivalent
spacing
0.02412
𝐷
π‘Ÿ
log( )
πœ‡πΉ/π‘˜π‘š
οƒ˜ asymmetrical spacing 𝐢𝑛 =
𝐷
πΏπ‘Ž = 2× 10−7 𝑙𝑛 (π‘Ÿ1 ) H/m
D = Distance between any two phases
5)
0.01206
Where, π‘Ÿ ′ = 0.7788r
L = 2× 10
4)
4
πœ‡πΉ/π‘˜π‘š
Inductance of Bundled conductors
line]
0.02412
log(
π·π‘’π‘ž
)
π‘Ÿ
π·π‘’π‘ž = 3√𝐷12 𝐷23 𝐷31
2
i. For two conductor arrangement
D12
D23
4
𝐷𝑠 = √(𝐷𝑠 . 𝑑)2 = 𝐷𝑠 . 𝑑
1
ii. For three conductor arrangement
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2
D31
3
POWER SYSTEMS
MADURA COACHING
#62, Rakame Complex,
T.P.K Road, Madurai-625011
______________________________________________________________________________
iv.
Capacitance of Bundled
1 𝑍 π‘‰π‘Ÿ
=[
][ ]
0 1 πΌπ‘Ÿ
0.02412
Conductor lines 𝐢𝑛 =
π·π‘’π‘ž πœ‡πΉ/π‘˜π‘š
log(
)
So A = 1, B = Z, C = 0, D = 1
√π‘Ÿπ‘‘
v.
For a two conductor bundle D = √π‘Ÿπ‘‘
10)
For a three conductor bundle
D=
√π‘Ÿπ‘‘2
condition
π‘‰π‘Ÿ = Receiving end voltage under full load
4
condition
D = 1.09 √π‘Ÿπ‘‘3
Ground
line
(method of images)
capacitance
11)
πΆπ‘Žπ‘› = 2 πΆπ‘Žπ‘ =
Regulation =
πΌπ‘Ÿ π‘…π‘π‘œπ‘ πœ™π‘Ÿ ± πΌπ‘Ÿ π‘‹π‘ π‘–π‘›πœ™π‘Ÿ
𝑉𝑅
+ → For lag PF
for 1Ο• line
0.02412
𝐷
log( ′)
π‘Ÿ
- → For lead PF
πœ‡πΉ/π‘˜π‘š
i. Max voltage regulation πœ™π‘Ÿ = πœƒ
𝑋
πœƒ = π‘‘π‘Žπ‘›−1 𝑅
𝐷
2𝐻
π‘Ÿ ′ = r √1 + ( )2
ii. Zero regulation
πœ‹
πœ™π‘Ÿ + πœƒ =
8.a) Performance of Tr.line
Type of
Tr.line
Classifi-cation based
on f × l
Short
line
<4000Hz km
Medium
line
4000
<
fl
12000Hz km
long
line
fl=12000 Hz km
<
12)
For nominal T-circuit
𝑉
[ 𝑠]
𝐼𝑠
l >240km
Effect of capacitance
Short
line
0-20 kv
neglected
Medium
line
20-100 kv
capacitance is lumped
and constant
long line
>100 kv
capacitance
is
uniformly distributed
1+
π‘Œπ‘
2
π‘Œπ‘
+ 4)
1+
=[
π‘Œ(1
π‘Œπ‘
)
2
π‘Œπ‘ ]
2
𝑍
1+
π‘Œπ‘]
2
𝑉
[ π‘Ÿ]
πΌπ‘Ÿ
𝑉
[ π‘Ÿ]
πΌπ‘Ÿ
Long Tr.line
𝑉
[ 𝑠]
𝐼𝑠
πΆπ‘œπ‘ β„Žπ›Ύπ‘™
= [1
π‘ π‘–π‘›β„Žπ›Ύπ‘™
𝑍
𝑐
𝑍𝑐 π‘ π‘–π‘›β„Žπ›Ύπ‘™
cos β„Žπ›Ύπ‘™
𝑉
] [ π‘Ÿ]
πΌπ‘Ÿ
𝛾 = √𝑧𝑦
𝛾 = ∝ + j𝛽
𝛽 = πœ”√𝐿𝑐
l→length of Tr line
∝→ attention constant Neper/sec
𝛽 → phase constant in rad/km
For short transmission lines
73 73 00 77 34
𝑍(1 +
𝑉
[ 𝑠]
𝐼𝑠
8.b)
𝐴
=[
𝐢
π‘Œπ‘
2
80km<l<
240km
13)
𝑉
[ 𝑠]
𝐼𝑠
1+
=[
π‘Œ
For nominal πœ‹-circuit
Based on
operating
voltage
when
Medium length Tr.line
l < 80 km
Type of
Tr.line
occur
2
Classification
based
on
length of line
(i.e)
power
line i.e
f = 50Hz
9)
𝑉 ′ π‘Ÿ − π‘‰π‘Ÿ
π‘‰π‘Ÿ
𝑉 ′ π‘Ÿ = Receiving end voltage under no load
3
For a four conductor bundle
7)
Voltage Regulation =
𝐡 π‘‰π‘Ÿ
][ ]
𝐷 πΌπ‘Ÿ
Sin 𝛾𝑙 = √𝑦𝑧 [1 +
3
𝑦𝑧
3!
+
(𝑦𝑧)2
5!
+ …]
POWER SYSTEMS
MADURA COACHING
#62, Rakame Complex,
T.P.K Road, Madurai-625011
______________________________________________________________________________
𝑦
(𝑦𝑧)2
17)
Surge Impedance
Cos 𝛾𝑙 = 1 + 𝑧 +
+…
2!
14)
4!
𝑧
2πœ‹
Velocity of wave propagation 𝑉𝑐 = f πœ†
15)
𝑅+𝑗𝑀𝐿
𝑍𝑐 = √𝑦 = √𝐺+𝑗𝑀𝐢
Wave length (πœ†) πœ†= 𝛽
𝐡
𝑍𝑐 = √𝐢 = √π‘π‘œπ‘ . 𝑍𝑠𝑐
Equivalent πœ‹-ckt using ABCD
parameters
For loss less transmission line, R=0, G=0
𝐿
𝑍𝑠 = √𝐢
Note:
𝑍𝑐 = 400 Ω for transmission line
𝑍𝑐 = 40 Ω for cable
π‘Œ′𝑍′
𝑧
𝑉
π‘‰π‘Ÿ
2
[ 𝑠] =
′ ′
′ ′ [ ]
π‘Œ
𝑍
π‘Œ
𝑍
𝐼𝑠
πΌπ‘Ÿ
π‘Œ ′ (1 +
) 1+
4
2 ]
[
18)
1+
SIL =
𝛾𝑙
tanh(𝛾𝑙/2)
(𝛾𝑙/2)
Y’ = 𝑧 tan h 2 = y
𝑐
19)
Equivalent T-ckt using ABCD parameter
i)
𝑦"𝑧"
1+ 2
𝑉
[ 𝑠] = [
𝐼𝑠
𝑦"
𝑧"
2
cos β„Žπ›Ύπ‘™−1
)
sin h𝛾𝑙
= 𝑧𝑐 (
1
=
(𝐾𝑉)2
𝑍𝑠
MW
Tr.line connected in series
𝑉
𝐴
[ 𝑠] = [ 1
𝐼𝑠
𝐢1
𝐡1 𝐴2
][
𝐷1 𝐢2
𝑧 tan β„Ž(𝛾𝑙/2)
𝛾𝑙/2
iii)
𝐡2 𝑉𝑅
][ ]
𝐷2 𝐼𝑅
Tr.line connected in cascade
𝑉
𝐴 𝐴 + 𝐡1 𝐢2
[ 𝑆] = [ 1 2
𝐼𝑆
𝐢1 𝐴2 + 𝐷1 𝐢2
=2
Y” = 𝑧𝑐 sin h𝛾𝑙 = 𝑦
16)
ii)
𝑧"𝑦"
) π‘‰π‘Ÿ
4
][ ]
𝑦"𝑧"
πΌπ‘Ÿ
+ 2
𝑧"(1 +
1
𝑉𝑆 𝑉𝑅
𝑍𝑠
οƒ˜ loading <SIL→PF will be leading
οƒ˜ Loading>SIL→Pf will be lagging
οƒ˜ Loading = SIL →PF will be unity
π‘ π‘–π‘›β„Žπ›Ύπ‘™
𝛾𝑙
𝑧′ = 𝑧𝑐 sin h𝛾𝑙 = z
2
Surge impendence loading
𝐴1 𝐡1 + 𝐡1 𝐷2 𝑉𝑅
][ ]
𝐢1 𝐡2 + 𝐷1 𝐷2 𝐼𝑅
Tr.line connected in parallel
sin 𝛾𝑙
𝛾𝑙
𝑉𝑠 = |𝑉𝑠 |<𝛿, π‘‰π‘Ÿ = |π‘‰π‘Ÿ |<0
D = A = |A|<𝛼, B = |B| <𝛽
π‘†π‘Ÿ =
|𝑉𝑠 ||π‘‰π‘Ÿ |
|𝐡|
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<(𝛽 − 𝛿) –
|𝐴||π‘‰π‘Ÿ |2
|𝐡|
< (𝛽 − 𝛼)
4
POWER SYSTEMS
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______________________________________________________________________________
2𝑧
οƒ˜ Refraction coefficient = 𝑧 +𝑧
𝐿
οƒ˜ Reflection coefficient =
21)
𝑐
𝑍𝐿 −𝑍𝐢
𝑍𝐿 +𝑍𝐢
Parameter of single core cables;
i) Insulation Resistance
𝜌
𝑅
Rins =2πœ‹ln( π‘Ÿ ) ohms/metre
A=
𝐴1 𝐡2 +𝐴2 𝐡1
𝐡1 +𝐡2
𝐡 𝐡
B=𝐡 1+𝐡2
1
2
𝐷 −𝐷
C = (𝐢1 + 𝐢2 ) + 𝐡1+𝐡2
1
D=
20)
2
𝐷1 𝐡2 +𝐷2 𝐡1
𝐡1 +𝐡2
Where
resistance
Reflection and refraction of waves
Line terminated by impedance (z)
Rins→Insulation
𝜌 →Resistivity
material
of
insulating
R→inside radius of sheath
r→conductor radius
𝑉𝑑 =
ii)Insulation
2𝑧
𝑍𝐿 +𝑍𝐢
Resistance
∝
1
π‘™π‘’π‘›π‘”π‘‘β„Ž π‘œπ‘“ π‘π‘Žπ‘π‘™π‘’
𝑉𝑖
𝑉𝑑 = Transmitted (or) Refracted voltage
Rins∝
1
𝑙
𝑍 −𝑍
𝑉𝑅 = 𝑍𝐿 +𝑍𝐢 𝑉𝑖
𝐿
iii) Capacitance between core and
sheath
𝐢
𝑉𝑅 = Reflected voltage
𝑖𝑑 =
2
𝑍𝐿 +𝑍𝐢
2πœ‹∈ ∈
0 π‘Ÿ
c = 𝑙𝑛(𝑅/π‘Ÿ)
F/m
𝑉𝑖
πœ†
iv) Potential V = 2πœ‹πœ– 𝑙𝑛(𝑅/π‘Ÿ)
𝑉𝑖 = Incident voltage
𝑖𝑑 = transmitted current
r→radius of conductor
π‘–π‘Ÿ = reflected current
R→Inner radius of sheath
𝐼𝑖 = incident current
v) Gradient is maximum at the
𝑍 −𝑍
surface of conductor
𝑖𝑅 = 𝑍𝐢+𝑍𝐿 𝐼𝑖
𝐿
(or)
𝐢
π‘”π‘šπ‘Žπ‘₯ =
𝑍 −𝑍
− (𝑍𝐿 +𝑍𝐢 ) 𝐼𝑖
𝐿
𝐢
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𝑉
π‘Ÿ 𝑙𝑛
𝑅
π‘Ÿ
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𝑅
π‘‰π‘Ž
1 1
1 π‘‰π‘Ž0
= e = 2.718
π‘Ÿ
[𝑉𝑏 ] = [1 π‘˜ 2 π‘˜ ] [π‘‰π‘Ž1 ]
1 π‘˜ π‘˜ 2 π‘‰π‘Ž2
𝑉𝑐
vi)
Gradient is minimum at the inner
π‘‰π‘Ž0
1
1
[π‘‰π‘Ž1 ] = 3 [1
π‘‰π‘Ž2
1
radius of conductor
π‘”π‘šπ‘–π‘› =
𝑉
𝑅 𝑙𝑛
𝑅
π‘Ÿ
7)
Unit – III Symmetrical
Components and faults
1)
1 π‘‰π‘Ž
π‘˜ 2 ] [𝑉𝑏 ]
π‘˜ 𝑉𝑐
1
π‘˜
π‘˜2
Unsymmetrical faults:
i) Single line to ground fault
Per unit value=
π΄π‘π‘‘π‘’π‘Žπ‘™ π‘£π‘Žπ‘™π‘’π‘’ 𝑖𝑛 π‘ π‘œπ‘šπ‘’ 𝑒𝑛𝑖𝑑𝑠
π΅π‘Žπ‘ π‘’ (π‘œπ‘Ÿ)π‘Ÿπ‘’π‘“π‘’π‘Ÿπ‘’π‘›π‘π‘’ π‘£π‘Žπ‘™π‘’π‘’ 𝑖𝑛 π‘ π‘Žπ‘šπ‘’ 𝑒𝑛𝑖𝑑𝑠
2)
Base Current =
π΅π‘Žπ‘ π‘’ 𝐾𝑉𝐴
√3 ×π΅π‘Žπ‘ π‘’ 𝐾𝑉
A
Base impedence
=
𝐿𝑖𝑛𝑒 π‘‘π‘œ π‘›π‘’π‘’π‘‘π‘Ÿπ‘Žπ‘™ π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ π‘π‘Žπ‘ π‘’ π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’
π΅π‘Žπ‘ π‘’ π‘π‘’π‘Ÿπ‘Ÿπ‘’π‘›π‘‘
οƒ˜ 𝐼𝑅0 = 𝐼𝑅1 = 𝐼𝑅2 =
2
=
3)
π΅π‘Žπ‘ π‘’ 𝐾𝑉
Ω
π΅π‘Žπ‘ π‘’ 𝑀𝑉𝐴
𝐼
Per unit reactance 𝑋𝑝𝑒 = π‘‹π‘Žπ‘π‘‘π‘’π‘Žπ‘™ π‘‰π‘π‘Žπ‘ π‘’
1π‘’π‘ž +𝑍2π‘’π‘ž +𝑍0π‘’π‘ž
1π‘’π‘ž +𝑍2π‘’π‘ž +𝑍0π‘’π‘ž +3𝑧𝑓
οƒ˜ 𝐼𝐹 = 𝐼𝑅 =3𝐼𝑅0 = 3𝐼𝑅1
𝑆
3𝑉
√ 𝐿
3𝑀𝑉𝐴𝑏
𝑍1π‘’π‘ž +𝑍2π‘’π‘ž +𝑍0π‘’π‘ž
οƒ˜ Actual fault current 𝐼𝐿 =
2
οƒ˜ Short circuit MVA =
π΅π‘Žπ‘ π‘’π‘€π‘‰π΄
𝑍𝑝𝑒 old× [π΅π‘Žπ‘ π‘’ 𝐾𝑉 π‘œπ‘™π‘‘ ] × [ π΅π‘Žπ‘ π‘’π‘€π‘‰π΄π‘›π‘’π‘€ ]
𝑛𝑒𝑀
5)
3𝐸𝑅𝐼
οƒ˜ 𝐼𝐹 = 𝐼𝑅 = 𝑍
(𝑀𝑉𝐴)π‘π‘Žπ‘ π‘’
(𝐾𝑉)2 π‘π‘Žπ‘ π‘’
𝑍𝑝𝑒 new =
π΅π‘Žπ‘ π‘’ 𝐾𝑉
𝐸𝑅𝐼
οƒ˜ 𝐼𝑅1 = 𝑍
π‘π‘Žπ‘ π‘’
𝑋𝑝𝑒 = π‘‹π‘Žπ‘π‘‘π‘’π‘Žπ‘™
4)
οƒ˜ 𝑉𝑅1+𝑉𝑅2+𝑉𝑅0 = 0
οƒ˜ If 𝐼𝑅 = 3𝐼𝑅0
𝐼𝑅
3
οƒ˜ 𝑉𝑛 = 𝐼𝑛 𝑍𝑛 =3𝐼𝑅0 𝑍𝑛
π‘œπ‘™π‘‘
short circuit KVA =
ii) Line to line fault:
100
Rated (or) Base KVa× %𝑍
6)
Symmetrical components
π‘‰π‘Ž = π‘‰π‘Ž1 +π‘‰π‘Ž2 +π‘‰π‘Ž0
𝑉𝑏 = 𝑉𝑏1 +𝑉𝑏2 +𝑉𝑏0
𝑉𝑐 = 𝑉𝑐1 +𝑉𝑐2 +𝑉𝑐0
𝑉𝑏1 = 𝐾 2 π‘‰π‘Ž1
𝑉𝑏2 = 𝐾 π‘‰π‘Ž2
𝑉𝑏0 = π‘‰π‘Ž0
𝑉𝑐1 = Kπ‘‰π‘Ž1
𝑉𝑐2 = 𝐾 2 π‘‰π‘Ž2
𝑉𝑐0 = π‘‰π‘Ž0
Where K = 1∠120°
οƒ˜ 𝐼𝐹 = 𝐼𝑦 =-𝐼𝑅
οƒ˜ 𝐼𝑅 = 0
In matrix form
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οƒ˜ 𝐼𝑦 + 𝐼𝐡 = 0
οƒ˜ 𝐼𝑅2 = 𝐼𝑅1 , 𝑉𝑅1 = 𝑉𝑅2
Unit – IV Power System
Stability
𝐸𝑅1
+𝑍
1π‘’π‘ž
2π‘’π‘ž +𝑍𝐹
οƒ˜ 𝐼𝑅1 = 𝑍
𝐸𝑅1
οƒ˜ 𝐼𝐹 = √3𝐼𝑅1 𝐼𝐹 = √3 𝑍
1π‘’π‘ž +𝑍2π‘’π‘ž +𝑍𝐹
1) Synchronous Generator connected to
infinite bus
𝑉𝑛 = 0 (zero seq not present)
iii) Double line to ground fault
S=
|𝐸||𝑉|
|𝑋|
∟90° − 𝑆 -
|𝑉|2
∟90°
|𝑋|
Real power output
P=
|𝐸||𝑉|
|𝑋|
Sin 𝛿
P ∝ Sin S
Max Real power output
P = π‘ƒπ‘šπ‘Žπ‘₯ / 𝛿 = 90°
π‘ƒπ‘šπ‘Žπ‘₯ =
οƒ˜ 𝐼𝐹 = 𝐼𝑦 +𝐼𝐡 , 𝐼𝑅 = 0
οƒ˜ 𝑉𝑦 = 𝑉𝐡 = 0
οƒ˜ 𝑉𝑅0 = 𝑉𝑅1 = 𝑉𝑅2 =
οƒ˜ 𝐼𝑅1 =
𝐸𝑅1
𝑍1π‘’π‘ž +
𝑉𝑅
3
|𝑋|
P = π‘ƒπ‘šπ‘Žπ‘₯ Sin 𝛿
* 𝐼𝑅 = 0
𝛿 < 90° → machine is stable
𝑍2π‘’π‘ž 𝑍0π‘’π‘ž
𝑍2π‘’π‘ž +𝑍0π‘’π‘ž
οƒ˜ 𝐼𝑅2 = -𝐼𝑅1 𝑍
|𝐸||𝑉|
S > 90° → machine is unstable
𝑍0π‘’π‘ž
2π‘’π‘ž +𝑍0π‘’π‘ž
2)
οƒ˜ 𝐼𝑓 = 3𝐼𝑅0 = 𝐼𝑛
οƒ˜ 𝑉𝑛 = 𝐼𝑛 𝑍𝑛 = 3𝐼𝑅0 𝑍𝑛
8)
οƒ˜
οƒ˜
οƒ˜
οƒ˜
Syn Gen connected to load by Tr.line
𝑉𝑠 = π΄π‘‰π‘Ÿ + π΅πΌπ‘Ÿ
Symmetrical fault
𝐼𝑠 = πΆπ‘‰π‘Ÿ + π·πΌπ‘Ÿ
i) LLL fault
Polar form of ABCD
𝐼𝑓 = 𝐼𝑅 = 𝐼𝑦 = 𝐼𝐡
𝐼𝑅 + 𝐼𝑦 + 𝐼𝐡 = 0
𝑉𝑅 = 𝑉𝑦 = 𝑉𝐡
𝐼𝑓 = 𝐼𝑅 = 𝐼𝑅1 , 𝑉𝑅1 = 0
A = |A| ∟ ∝
𝑋
B = |B| ∟ 𝛽 → Imp angle = π‘‡π‘Žπ‘›−1 𝑅
C = |C| βˆŸπ›Ύ → admittance angle = 90°
𝐸𝑅𝐼
1π‘’π‘ž +𝑍𝐹
οƒ˜ 𝐼𝐹 = 𝑍
οƒ˜ Short circuit MVA =
D = |D| ∟ ∝
𝑀𝑉𝐴𝑏
π‘π‘’π‘ž
οƒ˜ 𝑉𝑛 = 𝐼𝑛 𝑍𝑛 = 0
Power at Receiving end:
π‘†π‘Ÿ =
ii) LLLG fault
|𝑉𝑠 ||π‘‰π‘Ÿ |
|𝐡|
βˆŸπ›½ − 𝛿 −
|𝐴|
|𝐡|
|π‘‰π‘Ÿ |2 βˆŸπ›½−∝
οƒ˜ 𝐼𝐹 = 𝐼𝑅 + πΌπ‘Œ + 𝐼𝐡 = 0
𝐸
οƒ˜ 𝐼𝐹 = 𝐼𝑅 = 𝐼𝑅1 = 𝑍 𝑅1 p.u
1π‘’π‘ž
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|B| = |Z| = |X|, 𝛽 = πœƒ = 90°
π‘ƒπ‘šπ‘Žπ‘₯ =
Real power o/p:
π‘ƒπ‘Ÿ =
|π‘‰π‘Ÿ ||𝑉𝑠 |
|𝐡|
|𝐴|
Cos (𝛽 − 𝛿) |𝐡| |π‘‰π‘Ÿ |2 Cos βˆŸπ›½−∝
π‘ƒπ‘šπ‘Žπ‘₯ =
Max Real power output:
3)
iii) Inertia constant
|𝐴|
𝑿
𝑹
(H) =
Ratio:
i) For short Tr. Line
H=
A = 1.0 = D
𝑀𝐽
𝑀𝑉𝐴
(or) sec
𝑆𝐻
M = 180𝑓 MJ – sec/elect deg
π‘ƒπ‘šπ‘Žπ‘₯ =
|𝑉𝑠 ||π‘‰π‘Ÿ |
|𝑧|
-
1.0
|𝑧|
Where,
|π‘‰π‘Ÿ |2 cos πœƒ
πœ” → angular velocity (rad/sec)
=0
∝ → angular acceleration (rad/𝑠𝑒𝑐 2)
X = √3R
M →angular momentum
𝛿 = 𝛽 = 60°
H → Inertia constant (sec)
ii) For long Tr. Line
S → Rating of syn m/c
π‘‰π‘Ÿπ‘œ > 𝑉𝑠 , |A| < 1.0, ∝ ≠ 0
Pa → accelerating power
𝑋
𝑅
I →moment of inertia (kg - π‘š2 )
=
2πœ‹π‘“πΏ ×𝑙
πœŒπ‘™/π‘Ž
𝑋Ω/π‘˜π‘š
= 𝑅Ω/π‘˜π‘š
7) Swing equation of two machines
Capacitor Compensation in the line:
𝑋
π‘€π‘’π‘ž
= 𝑋𝐢 p.u
𝐿
𝛿 = 𝛽 = π‘‡π‘Žπ‘›−1 (
5)
𝑆
𝑆𝐻
C=0
4)
1 2
πΌπœ”
2
π‘˜π‘–π‘›π‘’π‘‘π‘–π‘ π‘’π‘›π‘’π‘Ÿπ‘”π‘¦ π‘ π‘‘π‘œπ‘Ÿπ‘’π‘‘
𝑖𝑛 π‘‘β„Žπ‘’ 𝑠𝑦𝑛 π‘š/𝑐
π‘…π‘Žπ‘‘π‘–π‘›π‘” π‘œπ‘“ 𝑠𝑦𝑛 π‘š/𝑐
iv) M = πœ‹π‘“ MJ – sec/elect rad
B = Z, ∝ = 0°
π‘‘π‘ƒπ‘šπ‘Žπ‘₯
𝑑π‘₯
(𝑉𝑠 = π‘‰π‘Ÿ = 𝑉)
ii) M = Iπœ”
- |𝐡| |π‘‰π‘Ÿ |2 Cos (𝛽− ∝)
Calculation of
|𝑉|2
|𝑋|
i) Pa = M∝
𝛿 = 𝛽 = π‘‡π‘Žπ‘›−1(X / R)
|𝑉𝑠 ||π‘‰π‘Ÿ |
|𝐡|
|𝑋|
6) Transient stability:
π‘ƒπ‘Ÿ = π‘ƒπ‘šπ‘Žπ‘₯ = SSSL (Steady State Stability
Limit)
π‘ƒπ‘šπ‘Žπ‘₯ =
|𝑉𝑠 ||π‘‰π‘Ÿ |
= π‘ƒπ‘Žπ‘’π‘ž
i) If two m/c’s are swing together
𝑋𝐿 − 𝑋𝐢
)
𝑅
π‘€π‘’π‘ž = 𝑀1 + 𝑀2 π»π‘’π‘ž = 𝐻1 + 𝐻2
Approximate power transfer equation
ii) If two m/c’s are do not swing together
For loss less line
𝑀1𝑀2
π‘€π‘’π‘ž = 𝑀
|A| = 1,0, ∝= 0
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𝑑2 𝛿
𝑑𝑑 2
1
8
+ 𝑀2
𝐻1𝐻2
π»π‘’π‘ž = 𝐻
1
+ 𝐻2
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8)
Fault clearing angle:
4)
Incremental fuel rate
𝑑(𝑖𝑛𝑝𝑒𝑑)
𝑑𝐹
= 𝑑(π‘œπ‘’π‘‘π‘π‘’π‘‘) = 𝑑𝑃
𝛿𝑐 = π‘π‘œπ‘ 
−1
Where F → Fuel input (Btu/hr)
𝑃 (𝛿 − 𝛿 )+ 𝑃 cos 𝛿 −π‘ƒπ‘š2 cos 𝛿0
[ 𝑠 π‘š π‘Ÿ π‘ƒπ‘šπ‘šπ‘ − π‘ƒπ‘šπ‘Ÿ
]
3
2
P → Power output (W)
elect deg
𝑑𝑃
𝛿0 =
𝑃
𝑠𝑖𝑛−1 ( 𝑠 )
π‘ƒπ‘š1
π›Ώπ‘š = 180 -
οƒ˜ Incremental efficiency = 𝑑𝐹
𝑃
𝑠𝑖𝑛−1 ( 𝑠 )elett
π‘ƒπ‘š3
deg
5)
Where, 𝛿0 = initial angle
Penalty factor 𝐿𝑛 =
πœ•π‘ƒπΏ
πœ•π‘ƒπ‘›
π›Ώπ‘š = max swinging angle
1
1−
πœ•π‘ƒπΏ
πœ•π‘ƒπ‘›
→ Incremental transmission loss
at plant n.
π‘ƒπ‘š1 = max mech power before fault
Unit - VI Protective Relays
π‘ƒπ‘š2 = max mech power during fault
π‘ƒπ‘š3 = max mech power after fault
1)
Time Multiplier Settings (TMS)
TMS =
Unit - V Economic Load
Dispatch
π‘‘π‘Ÿπ‘’π‘žπ‘’π‘–π‘Ÿπ‘œπ‘‘
𝑑(𝑇𝑀𝑆=1)
π‘‘π‘Ÿπ‘’π‘žπ‘’π‘–π‘Ÿπ‘’π‘‘ = Required time of operation
𝑑(𝑇𝑀𝑆=1) = Time of operation when TMS =1
1)
KVA
loading
on
generator
2)
=√𝑃𝑝 2 + 𝑄𝑝 2
Plug setting Multiplier (PSM)
πΉπ‘Žπ‘’π‘™π‘‘ π‘π‘’π‘Ÿπ‘Ÿπ‘’π‘›π‘‘
PSM=π‘π‘’π‘Ÿπ‘Ÿπ‘’π‘›π‘‘ 𝑠𝑒𝑑𝑑𝑖𝑛𝑔×𝐢𝑇 π‘ π‘’π‘π‘œπ‘›π‘‘π‘Žπ‘Ÿπ‘¦ π‘Ÿπ‘Žπ‘‘π‘’π‘‘ π‘π‘’π‘Ÿπ‘Ÿπ‘’π‘›π‘‘
×𝐢.𝑇 π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘›
𝑃𝑝 = Generator active power
3)
𝑄𝑝 = Generator reactive power
2)
π‘ƒπ‘–π‘π‘˜ 𝑒𝑝 π‘π‘’π‘Ÿπ‘Ÿπ‘’π‘›π‘‘
= π‘…π‘Žπ‘‘π‘’π‘‘ π‘ π‘’π‘π‘œπ‘›π‘‘π‘Žπ‘Ÿπ‘¦ π‘π‘’π‘Ÿπ‘Ÿπ‘’π‘›π‘‘ × 100%
𝑃𝑝 2 + 𝑄𝑝 2 ≤ 𝐢𝑝 2
π‘œπ‘“ 𝐢.𝑇
𝐢𝑝 → pre specified value
3)
Current setting
4)
π‘ƒπ‘π‘šπ‘–π‘› ≤ 𝑃𝑝 ≤ π‘ƒπ‘π‘šπ‘Žπ‘₯
Torque equation
T = 𝐾1 𝐼 2 +𝐾2 𝑉 2 +𝐾3 VI cos(πœƒ-𝜏) + k
π‘ƒπ‘π‘šπ‘–π‘› , π‘ƒπ‘π‘šπ‘Žπ‘₯ → min and max active
power generation of a source
Where I→RMS value of current
V→ RMS value of voltage
π‘„π‘π‘šπ‘–π‘› ≤ 𝑄𝑝 ≤ π‘„π‘π‘šπ‘Žπ‘₯
πœƒ →angle b/w v and I
π‘„π‘π‘šπ‘–π‘› , π‘„π‘π‘šπ‘Žπ‘₯ → min and max reactive
power generation of a source
𝜏 → maximum torque angle
K→Restraining Torque
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6)
Resistance Switching
𝐾1, 𝐾2 , 𝐾3 →Relay constant
5)
i) Over current relay T = 𝐾1 𝐼 2 -K
ii) Directional relay = T = 𝐾3 VI cos(πœƒ-𝜏) – k
iii) Impedance relay T = 𝐾1 𝐼 2 -𝐾2 𝑉 2
1
For relay operation z =
𝑉
𝐼
1
f = 2πœ‹ √𝐿𝐢 −
𝐾
<√ 𝐾1
2
7)
1
4𝑅2 𝐢 2
Transient Oscillation
iv) Reactance relay
If Resistance connected across circuit
Breaker
T = 𝐾1 𝐼 2 -𝐾3 VI sinπœƒ; 𝜏 = 90°
𝑉
𝐾
For relay operation 𝐼 sinπœƒ = X < 𝐾1
v) Mho relay T = 𝐾3 VI cos(πœƒ-𝜏) –𝐾2 𝑉 2
𝑉
1
𝐿
1
𝐿
οƒ˜ R = 2 √𝐢 → No oscillation
3
οƒ˜ R > 2 √𝐢 → Oscillation
𝐾
For relay operation 𝐼 = Z< 𝐾3 cos(πœƒ-𝜏)
2
Unit - VII Circuit Breakers
1)
Restriking voltage V = E (1 – cos
2)
Maximum value of
1
)t)
√𝐿𝐢
= 2× πΈπ‘π‘’π‘Žπ‘˜
Restriking voltage
πΈπ‘π‘’π‘Žπ‘˜ = peak value of system voltage
3)
Natural frequency of oscillation
πœ”π‘› =
4)
1
√𝐿𝐢
Rate of rise of restriking voltage
RRRV = πΈπœ”π‘› sinπœ”π‘› 𝑑
5)
Maximum value of RRRV = πΈπ‘π‘’π‘Žπ‘˜ 𝑀𝑛
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10
POWER SYSTEMS
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