Double Tuned Filters
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lgorithm for the Parameters
of
Double Tuned Filter
Xiao Yao
Hubei Electric Power Test & Research Institute
Wuhan, P.
R.
China
Abstract: On the basis of analyzing the characteristics of the
simplest and the basic type
of
double tuned filter,
an
algorithm
for
precisely determining its parameters is presented here. Using this
method, the inductances and the capacitances of the filter can be
calculated h m he
known
data such as the reactive compensation
capacity, the tuned freque ncies and the parallel resonant frequency,
etc.
There are various damped types of double tuned filters, they
have three pain of tuned frequencies under the conditions
of
i) the
equivalent impedance being minimum;
ii)
the total
reactance
being
zero; iii) when the damping resistorsare out
of
service. Usually the
tuned frequencies of condition i) or ii) are
selected
to determine
the parameters of the filter in designing process. The diagram for
determining the parameters
of
damped-types s also developed.
Keywords:
powersystemharmonics, power filter, filter
I.
INTRODUCTION
There are m any types of doub le tuned filters. The simplest
and the basic one is shown
as
Fig.
1,
others are damped types
illustrated in Fig.
2.
They a re widely used in HVDC projects
[l ] [2]. Besides bypassing the appointed harmonic currents
near the tuned frequencies, the filter also provide the
fundamental reactive power needed by the converter.
Compared to the single tuned filters with same performance,
they enjoy a lot of advantages such
as
only one reactor is
subjected to full line voltage, occupies less site, and only
one switchgear is needed, etc.
The parameters of the doub le tuned filter estimated from
two
banks of single tuned filters has been introduced in [3],
which is subject to that their equivalent impedance near the
resonant frequencies are approximately equal, but this is not a
pragmatical method. How to calculate the parameters of
double tuned filters accurately and directly from the known
data such
as
the tuned frequencies, the reactive capacity of
the filter, and the rated voltage of the
system
has not been
introduced in detail so far.
The relationships among the parameters of basic type
double tuned filter (Fig.
1
are analyzed,
so
an algorithm for
precise calculating the parameters of it according to the
known data is conducted in this paper.
Based
on
he analyzing of relationships among the
Paper accepted
for
presentation
at the 8u International
Conference on Harmonics and Qualio of Power
ICHQP
98,
ointly organized
by IEEEPES
and
NTUA,
Athens Greece October
1416,1998
0-7803-5105-3/98/ 10.00 1998 EEE
parameters of the simplest filter, the characteristics
of
the
damped-type filters are discussed. There are three pairs of
tuned frequencies
on
the damped-type filters under the
conditions o f (i) the total impedance being minimum;
(ii)
the
total reactance being zero; (iii) the damping resistors being
out of service. Usually tuned frequencies of condition
i)
or
(ii)
are
selected to determine the parameters of the filters in
designing process. The diagram for determining the
parameters of them is also developed accordingly.
11.
THE RELATIONSHIPSAMONG THE PARAMETERS
OF
THE BASIC DOUBLE
TUNED
FILTER
The configuration of the basic do uble tuned filter is shown
as Fig. 1, which is the combination of a series resonant circuit
L,,
,)
nd a parallel resonant circuit
L,
z).
Under the conditions of ignoring the resistance in reactors
and dielectric losses
in
capacitors, the impedance of the series
circuit is
1)
1
where w is the angu lar frequency in radians, therefore the
ZJW =Ad - 1,
cut,
Fig.
1
The configurationof the basic double tuned filter
-.
(4
(4
Fig.
2 Variousdampedtypes of double tuned filters
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a?
a4 f n q u e w J
c )
Fig 3
The characteristicsofthe simplest doubletuned
Filter,
a) series
circuit;
b)
parallel
circuit; c)
total
impedance
of
the
filter
l
series resonant frequency is
w ,=m
When w
<a,, z s w
is capacitive; and
w >
w ,
, w
is inductive. The impedance of the parallel
circuit is
3)
and
its
parallel resonant frequency is
up=JG 4)
When
w < w p , z p w )
is inductive; and CI )
> u p ,
z p w ) is
capacitive. The curves of the impedance versus
frequency z w and
z , w)
are show n in Fig.3 (a) and (b)
respectively. Fig.3 (c)
is
the series combination
characteristicsof the above two circuits, From which, another
two resonant frequencies 4,), that
is
the tuned
frequencies of the filter can be seen clearly. At the tuned
fkquencies, the total impedance of the filter is zero.
frequencies will
be
derived from the following equation:
If the parameters L,,C, and
L, C ,
are given, the tuned
z 0 )
=
ZS(@)
+
Z p ( @
This equation can be rewritten
as
o4L1L2C1C2 - tu2(L2C1 + LlCl + L 2 C 2) + 1 = 0 . ( 6)
Two real roots and y
of
equation 6) are tuned
frequencies of the do uble tuned filter. According to V ida s
theory, the relationship between the roots and the coefficients
of
the equation 6)
is
i.e.
8)
The hannonic currents at tuned frequenciesq nd y will
be bypassed by the filter. According to the project
requirement, the tuned frequencies are defined at
first
and
then the parameters
L,,
C, and L f , Cf will be derived. The
filter impedan ce is infinite at the parallel fiequen cy CO= , To
prevent some harmonic currents near
w
rom being severely
amplified, engineers should take account
of
the network
impedance-fkequency characteristics and select a parallel
resonant frequency properly in the designing process. If
CUI
0 2 and w s determined, is certainly defined by
equation 8). Substituting equations
2)
and 4) into equation
(6) yields
1
1
@ p
w , w 2
=
E
Forwlbeing one
of
the solutions
of
equation
9) ,
substituting w by
w 1
, the relationship between the
capacitances C , and
C,
can be obtained:
10)
There are other two relationships between
L,
nd C , ,
L,
and
C2
etermined by equation ( 2 ) and equation 4), which
can be rewritten as:
--, -4
4
m i -
2
c2
U S
Besides bypassing the harmonic current, the double tuned
filter has another performance
of
supplying the reactive
compensation power. If the network findamental rated
voltage is
U,
nd the hdamental reactive power supplied by
the filter is Q, then the impedance
of
the filter at hndamental
frequency
is
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From equation
5 ) ,
the impedance of the filter at the
fundamental frequency has a nother form:
where OF
is
the fundamental frequency
in
radians. From
above two equations, the follow ing equation is obtained:
15)
By equations 1
0)
to 1 2) and I
5) ,
if
wI
nd
Q
are
given, and
a+,
is determined at first, the parameters of the
basic double tuned filter can be obtained imm ediately.
By
scanning the impedance frequency characteristics of
the double tuned filter after getting its parameters, it can be
seen that the tuned frequencies
are
just expected, and the
fimdamental reactive capac ity is the same as the given one.
111.
A SPECIAL CASE
Specifically, if os w p = wo =6 he
retationships among the parameters can be simplified as the
following:
(16)
,
I c, = (h2 - h , )2 (h lh2)
1 9 )
IV. THE FEATURE
OF
THE DAMPED-TYPE
DOUBLE TUNED FILTERS
The impedance
of
the simplest double tuned filter is
almost pure inductive or capacitive over the whole
frequencies. If the impedance of the system
is
approximately
equal and opposite to that of the filter at some harmonic
frequencies, the resonance will be resulted in, which in
turn
leads to the harmon ic currents being seve rely amplified with
harmonic overvoltage of the components in the filter and
in
system.
To
prevent such a phenomenon, dam ping resistors are
added to it in different ways, therefore various damped types
of double tuned filters are con figurated in Fig. 2.
The Gezhouba-Nanqiao
HVDC
project
is
the first long
distance (=1045.7km) transmission scheme
in
China. Fig.
4
illustrates one pole of this f 00kV DC bipolar scheme from
Gezhouba (rectifier station) located in Central China to
n n
DC ine
5OmH
I5OmH
I I
38.93mH
b
71.0bmH
9
+ 23uF
Filter A
Filter
B
12/24 12/36
Fig.
4 ConfigurationofDCside in Gezhouba-Shanghai
HVDC
transmission
projects
Nanqiao (inverter station) located in Shanghai area with its
DC filter being the basic type of double tuned filters at first.
When
it
was put into operation in 1990, the equivalent
disturbing currents in DC line e xceede d 450mA and reached
to the level of 2618.2mA two levels are specified for the
equivalent disturbing current, level A: 500mA for bipolar,
1500mA for monopolar; level B: 150mA or bipolar, 450mA
for monopolar). One of the reasons is the resonance between
the filter A and the smoothing reactors at 181h harmonic.
Finally, a resistor of 500R was added to filter A in the way
illustrated
as
Fig. 2(a) to weaken the resonance, which
efficiently reduces
181h
harmonic current in DC line and so
reduces the equivalent disturbing current to 947mA in
monopolar operation.
The performance of each damped type of double tuned
filter is slightly differ from the others. The impedance of
Filter 2(a) at w p is on the order of R; the impedance of filter
2(b) takes R as asymptotic line when o s above q he
parameters in filter 2(c) should meet the relationship of
R
>,/m,
ts
impedance at is very large , but the
impedance above
w
is on the order of
R;
Fig. 2(d)
i s i n
fact
an third order filter being in series connection with a reactor,
it behaves as a high pass filter above
y;
ilter 2(e) has
limited impedance both at op and above y with its
parameters should meet the relationship of that
RI> m.
inally, the filter of Fig 2(f) with its
impedance both at oIJnd above are limited to the lower
value ofA, and
R2.
By scanning the impedance and frequency, it can be found
that there are three pairs
of
tuned frequenc ies on the damped-
type filters, they are:
(i) The frequencies
el
.., at which the impedance of the
filter are minimum;
(ii) The frequenciesel x2, at which the total reactance of
the filter equal zero.
(iii) Another is the solutions CO,,y f equation (6 ) , hey are
tuned frequencies of the simplest one. If damping
resistors are out of service, the filter will
be
tuned
at 01 andwz ;
Take Fig. 2(e) for example, the param eters of it are
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Inductance (mH)
LI ] U
3.16
I
4.39
Table
2 Frequencies relating
to
Fig. 2(e) and Table
1
Capacitance
pF)
Resistor (Q )
C I c 2 R I R 2
6.96 8.53 476 2744
I
f i (Hz ) h (Hz )
Solutions of Equ. (6) 797.5 2213.5
Minimum impedance I 248.5 1130.
Total rca c ta nc d
I
250.6 I
1264.
Select the type
of
damped dou ble tuned filter and input:
Q,he size of the filter
U,
the rated voltage of the system
,,,the parallel resonant frequency of the filter
q
.
o2
tuned frequencies ofth e filter
R,,Rz, esistance ofthe filter
terative precision
1
Select the
sorts
of tuned frequencies:
k m j =
min
or x ( c o ) = o
I
according to their relationships
El <E?
Calculate the pass band of the filter and
Fig 5 Diagram for determining the parameters of
damped double tuned filters
In designing process, the resistance of
R (RI
and
R 2 )
is
given, and so it is with the rated voltage of the system, the
compensation capacity and the tuned frequencies of the filter
prior to the calculation of
LI , L ,
and
CI,C,.
Parameters of
inductances and capacitances can be firstly calculated out
with the tuned frequencies given, then the resistance R R,
and
R2)
s added and the resistances in reactors
are
also taken
into account to calculate the actual tuned frequencies {
,az,,
wz2
} or
{
oxI,
w x 2 } by scanning. if the tuned frequencies
are not what demanded, recalculate
LI,
L, and C I ,
C
again by
adjusting 0 1 and
0 2 .
Finally the performance of the filter
should be inspected with the consideration of harmonic
impedance of the system and other filters to be installed. If
necessary, resistance
R ( R I
and R2)
should
be corrected and
repeat the calculating procedure s above.
The diagram for designing the damped-type double tuned
filters is as Fig. 5
IV. CONCLUSION
A simpler and accurate way to calculate the parameters of
the basic type of double tuned filter has been introduced in
this paper, and the diagram for determining the parameters of
damped-type double tuned filters
is
also developed. Other
parameters such
as
rated voltage, current and capacity of the
components
in
the filter can
be
further calculated after the
parameters R, L, C are determined.
A
software of this
algorithm for parameters of the filters is developed in
Visual Basic.
For
its advantages compa red to the single tuned
filter with same performance, the double tuned filter should
be cons idered at first
in
filtering projects.
V. REFERENCE
[ I
ClGR E WG 14.03, AC harmonic
filters
and reactive compensation for
HVDC,
general survey , Electra No.63, 1979
[2]
CIGRE
WG 14-03, AC harmonicjilrersandreactive compensation for
HVDC
w i th particular reference lo non-characferistic harmonics:
complemenr
to
the paper published in Electra
No.63 1979),ClGRE
report , une, 1990
[3] J. h i l l a g a , D. A. Bradley, P. S.Bodgcr,
Power Sysrem harmonics.
John Wiley & Sons, 985
VI.
BIOGRAPHY
Xiao
Yao,
was
born on
March, 28,
1960 in
Hubci Province, China.
He received
his
B.E. and M.E. degree in Electrical Engineering
from Tsinghua U niversity, China in 1983 and 1986nspectively. He
jointed Hubei Electric Power Test & Research Institute in china in
1986, and has been working in the field of power system harmonics
and quality ever since. He has some articles published in various
Chinese periodicals.
listed in Table 1, and the frequencies relating to above
conditions are listed in Table
2.
Usually, { w q , wz2 } or { w,yl,
o B
are selected to
absorb main harmonic currents, while frequencies {
w I
D
}
are used to determine the parameters
of LI, ,
and
C,,
C2 in
designing process.
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