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8/11/2019 Power Protecction course notes
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Examples
Problem 12.3
The problem requires us to find the three
currents Ia, Ib, and Ic, and also Vng.
The network is symmetric. Therefore, the
sequence circuits will be decoupled and we
can analyze them one at a time.
The zero sequence current must be zero
since the source is ungrounded and thereforeIa+Ib+Ic=.
!
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"ut the gi#en #oltages are unbalanced. $o
let%s hit them with an &'!to get the sequence
#oltages as follows(
=
=
+
)*.
),!-.
,)))).
!
!
!
!
!
!!!
)
!
*
*
jE
E
E
ecall that for loads and transmission lines,
/+=/'. $o we find the positi#e and negati#e
sequence currents using the below circuits.
0e obtain(=
=
+ !*+11+.*
),!-.
jI
=
= 2!**.
*
)*++.
jI
0e can then obtain the abc currents as
=
=
))).
.!3,!-.
.!31*-!.
2!**.
!*11.
!
!
!!!
*
*
c
b
a
I
I
I
4ow what about Vng5
*
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4otice from the positi#e and negati#e
sequence circuits that =+ngV and =ngV .
"ut consider ngV . The zero sequence circuit is
6rom the zero'sequence circuit, a 7V8equation results in
==
=+
,)))).,)))).
,)))).
ng
ng
V
V
4ow we ha#e all of the symmetrical
components of Vng, and we can therefore
obtain Vngas their sum(=++=++=
+,)))).,)))).
ngngngng VVVV
9larification( 0hen getting abc quantities
from +' quantities, we hit the +' quantities
with & :which contains terms in ; for the b'
and c'phase quantities
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quantities. &nd if we were to ha#e the c'
phase +' quantities, then the c'phase
quantity would ust be the sum of those c'phase +' quantities.
roblem 12.17
ecall that a 88> fault requires a parallel
combination of all three sequence networks.$o we must find all ) sequence networks.
?seful comments about the below networks.
0e get positi#e sequence phase shift of )@
going from low to highA negati#e sequence
of ')@ going from low to high.
The problem requires pre'fault, phase a
#oltage at the fault point be !.BC@.
- The positi#e sequence network is the
per'phase network for phase a. Therefore
this !.BC@ lies in the positi#e sequence
network.- Dre'fault implies no fault current, and
since we are ignoring load currents, there
is no current flow in the network.
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- In the teEt, FE.!*.1, because the fault
was on the line :in the middle of the
diagram! and >*,
the source #oltages had to be !BC')@.
- Gere, because the fault is at the
generator terminals, and therefore on the
same side of the phase shift as >!, >!
must be !BC@. "ecause there are equal andopposite phase shifts between the fault
point and >*, >* must also be !BC@.
The zero sequence network is
- to ground at each gen since both gens are
solidly grounded.
- open between each gen and the network
because of low side delta connection in the
Efmrs.
1
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The fault point, at the terminals of >! :on
the left
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sequence, and it will be the pre'fault #oltage
at the fault point, !BC@, for the positi#e
sequence network.
btaining the zero'sequence The#enin
network is also easy because of the open
circuit to the right of the fault pointA it is
shown below.
btaining positi#e, negati#e sequence The#.
impedances requires analyzing networks
with phase shifts. Gowe#er, because thephase shifts occur to #oltages and currents,
The#enin impedances may be computed
without consideration of phase shifts.
This is true for what your teEt calls normal
systems:see pp !1!'!1-
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$o the positi#e and negati#e sequence
networks to use in obtaining the The#enin
impedances are below. 4ote that the positi#e
sequence sources were idled.
These are identical networks. Therefore the
positi#e and negati#e sequence The#eninreatances are the same(
!*,.
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4ow we may draw the three The#enin
equi#alent networks.
&s mentioned at the beginning of thisproblem, a 88> fault requires a parallel
combination of all three sequence networks.
The connected circuits for analysis of a 88>
at the >! terminals is shown below.
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is easily done from the The#enin circuits
and knowledge of the fault currents, as seen
below.
&s a check on this work, let%s take a look at
the abc #oltages at the fault point.
!!
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=
=
=
23+2.
**3*.
**3*.
**3*.
!
!
!!!
*
*
c
b
a
V
V
V
Then we would use the sequence #oltages at
the fault point, in each sequence network, tocompute the currents in the #arious
elements. To do this, we would need to go
back to circuits with the phase shifts :see
page 2