PSE Lecture 07
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Transcript of PSE Lecture 07
Performance of Transmission Line
Line Parameters-Part 2
Introduction
Performance Parameters
Efficiency
Regulation
VoltageloadFull
VoltageloadFullVoltageLoadNo
RIP
P
LossesOutput
OutputEfficiency
r
Regulation%
1003
100%2
FLR
FLRNLR
V
VV
_
__
Distributed and Lumped Parameters
Transmission line with uniformly distributed line parameters (R, L, C, G)
Small section ∆x
I(x)z ∆x
y ∆x V(x)
V(x+ ∆x)
I(x+ ∆x)
Vs
Is
Vr
Ir
z = Series impedance /unit length/phase
y = Shunt admittance / unit length/phase
l = Length of transmission line Z = Total series impedance/
phase Y = Total shunt impedance/
phase
Transmission Line Models
Short line : Length less than 80 km. Shunt admittance is neglected Lumped parameter model
Medium line: Length between 80 km to 200 km. Shunt admittance needs to be considered Lumped parameter model
Nominal π model Nominal T model
Long line: Length longer than 200 km. Distributed parameter model Shunt admittance effect is important Equivalent π or T equivalent can be derived
ABCD Parameters of Transmission Line
R
R
S
S
I
V
DC
BA
I
V
Matrix Format
DA
BCAD
1
Passive, Linear, bilateral
Short Transmission Line
R
R
S
S
I
VZ
I
V
10
1Matrix Format
A=1, B=Z, C=0, D=1
Regulation of Short Transmission Line
I=IR=IS
VS
VR
IR
IXIZ
ϕ
22sincos XIVRIVV RRS
sin2sinsin2cos 22222222 XIVXIVRIVRIVV RRRRS
2222 sin2sin2 XRIIXVIRVVV RRRS
2
222sin2sin21
RRRRS V
XRI
V
IX
V
IRVV
Small quantity
Regulation of Short Transmission Line
RRRS V
IX
V
IRVV
sin2sin21
.......1682
1132
xxx
x
RRRS V
IX
V
IRVV
sinsin1
sinsin IXIRVV RS
RR
R
RS
V
XI
V
RI
V
VV
sinsinRegulation
Regulation
1003
%2
RIP
P
Medium Transmission Line
Medium transmission lines are modelled with lumped series impedance and shunt admittance.
Nominal π Representation
Nominal T Representation
Nominal π Representation
Nominal π Representation
Therefore A, B, C, D parameters
Nominal T Representation
MMRRM YVIIZ
VV and2
IM
RRRRRS II
ZVY
ZI
ZVV
222
Nominal T Representation
Therefore A, B, C, D parameters
Long Line Model
x 0
x 0
Long Line Model
And
Again differentiating with respect to x
Solution of the differential Eqn.
Long Line Model
Differentiating with respect to x
We know that
Therefore
Long Line Model
Long Line Model
At x = 0.
V = VR and I = IR
And
Solving for A1 and A2
Long Line Model
R
ll
R
ll
CS
R
ll
CR
ll
S
Iee
Vee
ZI
Iee
ZVee
V
22
1
22
We are interested in terminal conditions: x = l we have V = Vs and I = IS
Long Line Model
R
ll
R
ll
CS
R
ll
CR
ll
S
Iee
Vee
ZI
Iee
ZVee
V
22
1
22
RRC
S
RCRS
IlVlZ
I
IlZVlV
coshsinh1
sinhcosh
Long Line Model
RRC
S
RCRS
IlVlZ
I
IlZVlV
coshsinh1
sinhcosh
The ABCD parameters of the long transmission line