Title of Invention

AN IMPROVED GAS INSULATED SUBSTATION (GIS) DISCONNECTOR SWITCH

Abstract An improved gas insulated substation (GIS) disconnector switch (DS) comprising of : a fixed contact shield (04) covering a fixed contact (FC) (01), a moving contact shield (06) surrounding a moving contact (MC) (05), wherein both the FC shield and MC shield are insulated from a grounded metallic enclosure (09) by means of SF6 gas with appropriate density which fills the enclosure (09), and MC shield is separated from FC shield be a distance D which is proportional to the system voltage and SF6 gas density, characterized in that the E-field around the contact system is made uniform by profiling the fixed contact and moving contact shields and the axial E-field between the MC and the FC shield is made uniform by keeping radius of curvature of moving contact main body (R1) greater than the radius of curvature (R2) at the throat of the moving contact while keeping the outer radius of curvature of the FC shield (R3) higher than the radius of curvature (R4) of the FC Shield around the central axis .
Full Text Field of the Invention:
The present invention relates to an improved Gas Insulated
Substation (GIS) Dis-connector Switch. Disconnector switch (DS) is
primarily used to isolate sections of high voltage installations. When a
DS is closed, the capacitive charging current flows through the
contacts of the disconnector in proportion to the line voltage and the
line length. The disconnector during switching operation suffers re-
strikes, leading to arc breakouts. The phenomena of the arc
breakouts is associated to Very Fast Transient Over-Voltages (VFTOs)
generated during this operation. Any development in high voltage
disconnector switch is to meet the IEC procedures to establish such
conditions in a test laboratory, for evaluation and certification of
disconnector switch performance.
Background of the Invention
Very fast transient over-voltages (VFTOs) are common to
disconnector switch operation and are result of rapid dielectric
breakdown under severe electrostatic stresses experienced by the
insulating media (SF6) for relatively slow operating speeds of the
disconnector switch. Some times these breakdowns lead to
secondary breakdowns such as arc breakouts. The voltage collapse
across switching contacts take place in a time duration of 3-20 ns

depending on line voltage, electric field non-uniformity and SF6 gas
density. This resultant microwave emission propagating from switching contacts travel
along the gas insulated bus. The wave is reflected back from terminations and
modulates the principal wave in magnitude and time, which is expressed as VFTOs. The
wave-shape of these transients to a great extent depends on the configuration of the
gas-insulated circuit and associated terminations.
The number of VFTOs generated during a disconnector switch operation is considerably
high compared to the other fast acting switches. The slow moving contact sees many
voltage peaks before the DS operation as well as the interruption is completed. The
operating speeds of the moving contact and inter-electrode gap are the vital
parameters for a SF6 gas insulated disconnector switch.
Disconnectors are employed in a system to interrupt / make capacitive currents in
principle. When the capacitive current is interrupted a spark is formed, which shunts
the potentials on the two electrodes. When this spark extinguish, a few micro seconds
later, results in different potentials on the source side and the load side of the
disconnector.
US patent No.4,413,166 discloses a disconnect switch and grounding apparatus
therefor particularly adopted for use in gas insulated substations.

The disconnect switch disclosed in this document has fixed and moving contacts
insulated with SF6, but it does not make any mention about controlling the axial and
radial E-fields during operation of the switch, nor about profiling of contacts or shields.
US 5,177,664 discloses a three-phase "lumped together" gas insulated switchgear,
where the object of the invention is to achieve a small-sized and simply constructed
unit which includes disconnectors. This document too does not have any reference to
control of the E-fields to eliminate arc breakouts, as is disclosed in the present
invention.
US 7,091,493 B2 discloses an SF6 filled device which contains an isolator, but this
document also does not mention anything about the E-fields or their control through
profiling of contacts or their shields.

During evaluation of a disconnector switch (for bus charging current
test) the moving contact of the disconnector switch is kept at a DC
potentiai of -1.1 p.u., while the fixed contact is maintained at a AC
voitage equal to 1.1 times of the system voltage. When contacts of a
disconnector switch separate, several restrikes (spark/discharge) take
place, causing transition of E-field distribution from axial to radial
direction. This process tends to influence the axial discharges,
deflecting it towards the grounded metallic enclosure. This recurrent
phenomenon at times leads to secondary breakdowns (arc breakout)
to the grounded enclosure. The VFTOs magnitude at / near the
disconnector switch contacts during its operatbn may also lead to
voltage multiplication as high as three times depending on the
observation point and the substation configuration. Intense VFTOs
may result to the voltage close to basic insulation levels (BIL) leading
to frequent VFTO lead breakouts in very high voltage systems.
To meet the above disasters Conventional disconnector switches
were employed primarily constituted by a fixed contact, a moving
contact and an inter-electrode gap. A metallic grounded enclosure
was used to contain SF6 gas insulation at specified density. The
system was designed for minimum average electrostatic fields,
without considering the impact of axial and radial electrostatic fields.
The switching (transition) of electrostatic fields during presence of a

spark/discharge due to restrikes was also seldom considered. The
conventional disconnector switch in above situation suffered the
following deficiencies:
1. Highest magnitude of VFTOs around DS contacts
2. Field non-uniformity between/surrounding the contacts during
discharges
3. Long discharge lengths/lnter-electrode gap.
4. Requirement of higher operating densities for SF6 gas.
5. Voluminous designs
Description of the Invention
The main objective of the Invention to overcome the prior art
difficulties is developing a secondary break-down free gas insulated
disconnector switch by controlling the radial electric field around the
contact system during a discharge between the contacts.

According to another objective of the invention the conventional
contact system of the disconnector switch is replaced by an improved
arrangement to achieve optimized electrostatic fields in the electrode
gap.
According to a further objective of the invention the discharge
length/inter-electrode gap is optimized.
According to a still further objective of the invention radial E-field
between the contact system of the disconnector switch and the
metallic grounded enclosure is improved.
According to yet another objective of the invention specific profile of
electrostatic shields for contacts of disconnector switch is developed.
The proposed Invention has designed constructional features of the
fixed contact (Fc) and moving contact (Mc) of the disconnector
switch to meet the following requirements.
1. Axial E-field must be uniform between the contact shields,
when DS is in fully open condition.
2. Axial E-field must also be uniform between moving contact and
fixed contact shield during DS is in operation.

3. During contact movement, axial E-field should be highest
between FC shield and the moving contact around the central axis.
4. During a discharge between the contacts, the radial E-field
from the moving contact tip / discharge towards grounded metallic
enclosure shall be controlled with suitable profiles of FC and MC
shields.
To comply with the above requirements to maintain optimal efficiency
of the switch without arc breakout and VFTO lead breakouts the fixed
contact covered by a fixed contact shield is maintained axial with
annular space between the fixed contacts shield to control the axial
field between the fixed and moving contact shields. The entire
contact system is insulated from a grounded metallic enclosure
maintained with SF6 gas with appropriate density and the moving
contact is located in a MC housing.
A gap proportional to system voltage and SF6 gas density is
maintained between the moving contact shield and fixed contact
shield.
The maintenance of discharged length and axial E-field between the
Mc and Fc shield is made uniform and keeping the highest axial E-

field at the central axis and not on the surface of the tip is carried out
by using well profiled FC shield and the moving contact keeping
radius of curvature of the moving contact main body higher than the
radius of curvature at the throat of moving contact. The outer radius
of curvature of the FC shield is maintained much higher than the
radius of curvature of the FC shield around the central axis.
According to the invention there is provided a GIS disconnector
switch (DS) comprising of a fixed contact shield covering a fixed
contact (FC) and a moving contact shield surrounding a moving
contact (MC), both the FC shield and MC shield for DS operation
being Insulated from a grounded metallic enclosure filled with
appropriate SF6 gas density wherein MC shield is separated from FC
shield by a distance 'D' proportional to the system voltage and SF6
gas density, the highest discharge length and radial E-field from the
discharge are controlled by profiling fixed contact shield around the
central axis of the DS moving contact shield and high voltage shield
around the fixed contact in which discharge length, uniform axial E-
field between the MC and FC by keeping radius of curvature of
moving contact main body (R1) higher than the radius of curvature
(R2) at the throat of the moving contact, keeping the outer radius of
curvature of the FC shield (R3) much higher than the radius of
curvature (R4) of the FC shield around the central axis, the said R1,
R2, R3 & R4 are being maintained with correlated relationship with
diameter (D1) of the MC and diameter (D3) of the FC shield.

The invention will be better understood by description with the help
of the accompanying drawings which
Figure 1 represents the conventional contact system for the gas
insulated disconnector switch.
Figure 2 represents the invented moving contact for the secondary
breakdown-free disconnector switch.
Figure 3 represents the invented fixed contact shield for the
secondary breakdown-free disconnector switch.
Figure 4 represents the Fixed contact assembly with shield for the
invented gas insulated disconnector switch.
Figure 5 represents the Assembly of the invented secondary
breakdown-free disconnector switch, (a) DS is in fully open condition
(b) DS Is under operation.
As shown in Figure 5 the fixed contact [01] of the disconnector
switch (DS) Is made of a high conductivity material with low erosion
refractory material tip held on a support insulator [02] with suitable
adapter [03]. The fixed contact is covered by a fixed contact shield

[04] with designed axial and annular space to control the axial field
between the fixed and moving contacts. The moving contact [05] Is
surrounded by a moving contact shield [06], when DS is in fully open
condition. The moving contact is located in housing called as MC
housing [07]. The DS operation is achieved by using an insulator
[08]. The entire contact system is insulated from the grounded
metallic enclosure [09] with designed SF6 gas density. The moving
contact shield is separated from the fixed contact shield by a distance
'D' proportional to the system voltage and the SF6 gas density. A
secondary breakdown-free disconnector switch shall meet the
following requirements:
The profile of the fixed contact and the moving contact shields are
designed in such a way that the E-field around the contact system is
highly uniform. This criterion must be met as long as the DS is in fully
open condition and is in closed condition.
The axial E-field between the MC and the FC shield (seen by moving
contact) is made uniform by using a well-profiled FC shield [04] and
the moving contact tip. The Moving contact is designed and
constructed in a manner so that the field shall be highest at the
central axis rather than on the surface of the tip. Figure 2 shows the
profile of moving contact. For keeping the highest axial E-field along

the central axis, R1 (radius of curvature of the moving contact main
body) must be much higher than R2 (radius of curvature of the throat
of moving contact). With this design, the highest axial field will be
close to the central axis Instead of near the outer surface of the
moving contact. Further, the discharge will be bound to the central
axis. Once the axial field is highest along the central axis, the
discharge length may not be the optimum value. The highest
discharge length is a function of the diameter (D1) of the moving
contact with respect to the FC shield. By using the highest possible
value of R1 for the moving contact (depending on diameter of the
moving contact and the throat of moving contact (D2) for gas flow),
optimum discharge length can be achieved.
Since highest discharge length can not be optimized beyond certain
extent, the radial E-field from the discharge is still a parameter to be
controlled. The diameter of the FC shield (D3) and its profile are
selected in such a way that the radial E-field around the discharge /
moving contact tip can not force the discharge from the central axis
towards the grounded enclosure of the disconnector switch. The
diameter of the shield is required to be at least 3 to 4 times highest
possible discharge length depending on the system voltage. When
moving contact is approaching the fixed contact during the DS
operation, the highest axial E-field is forced to be around the central

axis. This is possible by profiling the fixed contact shield around the
central axis, where moving contact enters and engage the fixed
contact. Figure 3 shows the profile of FC shield by meeting the above
features. Here, R3 is outer radius of the shield and R4 is radius of the
shield around the central axis. For optimal design of the shield, R3
must be much higher than R4. Moreover, R3 is comparable to the
diameter of the moving contact. Figure 4 shows the fixed contact
assembly for the gas insulated disconnector switch, according to the
proposed invention.
The Invention is illustrated with an exemplary illustration in Table 1.
Table 1
For 145 kV GIS, the dimensions as stated herein above are as
follows:
R1 = 12.0 mm
R2 = 2.0 mm
R3 = 35.0 mm
R4 = 2.0 mm
D1 = 45.0 mm
D2 = 8.0 mm
D3 = 125.0 mm
D = 60.0 mm

The said dimensions change with voltage class. However, the relation
between these parameters will be maintained in the similar manner.
The highest discharge length for 145 kV GIS is in the order of 30 mm
and is in the same level as R3. This value is again in the same order
as that of diameter of moving contact (40 to 45 mm).
The diameter of FC shield is 3 to 4 times of the highest discharge
length. As stated herein above, the profile of FC shield is function of
highest discharge length.
It is important to optimize the highest discharge length during the
disconnnector switch operation. The greater the distance between
the contacts at the moment of strike, the greater the radial E-field
driving the discharge towards the grounded enclosure. Hence, while
designing and constructing high voltage gas insulated disconnector
switch, it is essential to consider the highest radial E-field level during
Its operation (i.e. in the presence of discharge between the contacts).
Figure 5 shows the secondary breakdown-free disconnector switch
during its fully open condition and in operation.
The invention as herein described above should not be read in a
restrictive manner as various modifications, alterations and changes
are possible within the scope and limit of the invention as
encampused within the appended claims.

WE CLAIM:
1. An improved gas insulated substation (GIS) disconnector switch (DS) comprising of:
a fixed contact shield (04) covering a fixed contact (FC) (01),
a moving contact shield (06) surrounding a moving contact (MC) (05),
wherein both the FC shield and MC shield are insulated from a grounded metallic enclosure (09) by
means of SF6 gas with appropriate density which fills the enclosure (09), and MC shield is separated
from FC shield be a distance D which is proportional to the system voltage and SF6 gas density,
characterized in that the E-field around the contact system is made uniform by profiling the fixed
contact and moving contact shields and the axial E-field between the MC and the FC shield is made
uniform by keeping radius of curvature of moving contact main body (R1) greater than the radius of
curvature (R2) at the throat of the moving contact while keeping the outer radius of curvature of
the FC shield (R3) higher than the radius of curvature (R4) of the FC Shield around the central axis .
2. A GIS disconnector switch as claimed in claim 1 wherein the axial E-field between the MC
and FC shield is made uniform by using a well profiled FC shield (4) and the moving contact tip.

3. A GIS disconnector switch as claimed in claim 1 wherein the MC
is designed and profiled in such a way that the field is always
maintained highest at the central axis rather than on the surface of
the tip.
4. A GIS disconnector switch as claimed in claim 1 wherein for
keeping the highest axial E-field along the central axis radlus of
curvature of the moving contact main body (R1) is maintained much
higher than radius of curvature of the throat of MC (R2).
5. A GIS disconnector switch as claimed in the proceeding claims
wherein the highest discharge length is a function of diameter (D1) of
the MC with respect to FC shield and by using the highest possible
value of R1 for the moving contact (depending on diameters of the
moving contact and the throat of the moving contact (D2) for gas
flow), optimum discharge length is achieved.
6. A GIS disconnector switch as claimed in the preceeding claims
wherein the diameter of the FC shield (D3) and its profile are selected
in such a way that the radial E-field around the discharge/moving
contact tip cannot force the discharge from the central axis towards
the grounded enclosure of the DS.
7. A GIS disconnector switch as claimed in claim 6 wherein the
diameter of the shield is kept 3 to 4 times the highest possible
discharge length depending on the system voltage.

8. A GIS disconnector switch as claimed in the preceeding claims
wherein R3 is maintained much higher than R4 and R3 is comparable
to the diameter of the moving contact.
9. A GIS disconnector switch as claimed in the preceeding claims
wherein for a 145 kV GIS the dimensions of the disconnector switch
are as follows
R1 = 12.0 mm
R2 = 2.0 mm
R3 = 35.0 mm
R4 = 2.0 mm
D1 = 45.0 mm
D2 = 8.0 mm
D3 = 125.0 mm
D = 60.0 mm
10. A GIS disconnector switch as herein described and illustrated.

Documents:

00883-kol-2006-abstract.pdf

00883-kol-2006-claims.pdf

00883-kol-2006-correspondence others.pdf

00883-kol-2006-description(complete).pdf

00883-kol-2006-drawings.pdf

00883-kol-2006-form-1.pdf

00883-kol-2006-form-2.pdf

00883-kol-2006-form-3.pdf

00883-kol-2006-g.p.a.pdf

883-KOL-2006-ABSTRACT.1.1.pdf

883-KOL-2006-CANCELLED PAGES.pdf

883-KOL-2006-CLAIMS.1.1.pdf

883-KOL-2006-CORRESPONDENCE-1.1.pdf

883-KOL-2006-CORRESPONDENCE.pdf

883-KOL-2006-DESCRIPTION (COMPLETE).1.1.pdf

883-KOL-2006-DRAWINGS.1.1.pdf

883-kol-2006-examination report.pdf

883-KOL-2006-FORM 1-1.2.pdf

883-KOL-2006-FORM 1.1.1.pdf

883-kol-2006-form 18.pdf

883-KOL-2006-FORM 2.1.1.pdf

883-KOL-2006-FORM 3.1.1.pdf

883-kol-2006-form 3.pdf

883-KOL-2006-FORM 5.pdf

883-KOL-2006-FORM-27.pdf

883-kol-2006-gpa.pdf

883-kol-2006-granted-abstract.pdf

883-kol-2006-granted-claims.pdf

883-kol-2006-granted-description (complete).pdf

883-kol-2006-granted-drawings.pdf

883-kol-2006-granted-form 1-1.1.pdf

883-kol-2006-granted-form 1.pdf

883-kol-2006-granted-form 2.pdf

883-kol-2006-granted-specification.pdf

883-kol-2006-reply to examination report-1.1.pdf

883-KOL-2006-REPLY TO EXAMINATION REPORT.pdf

abstract-00883-kol-2006.jpg


Patent Number 247999
Indian Patent Application Number 883/KOL/2006
PG Journal Number 23/2011
Publication Date 10-Jun-2011
Grant Date 08-Jun-2011
Date of Filing 31-Aug-2006
Name of Patentee BHARAT HEAVY ELECTRICALS LIMITED
Applicant Address REGIONAL OPERATIONS DIVISION(ROD),PLOT NO.9/1, DJBLOCK, 3RD FLOOR KARUNAMOYEE, SALT LAKE CITY, KOLKATA-700091, HAVING ITS REGISTERED OFFICE AT BHEL HOUSE, SIRIFORT, NEW DELHI-110049, INDIA
Inventors:
# Inventor's Name Inventor's Address
1 DR. MANDAVA MOHANA RAO C/O BHARAT HEAVY ELECTRICALS LIMITED, WITH ONE OF ITS REGIONAL OFFICES AT REGIONAL OPERATIONS DIVISION(ROD),PLOT NO.9/1, DJBLOCK, 3RD FLOOR KARUNAMOYEE, SALT LAKE CITY, KOLKATA-700091, HAVING ITS REGISTERED OFFICE AT BHEL HOUSE, SIRIFORT, NEW DELHI-110049, INDIA
2 DR HARI SHANKAR JAIN C/O BHARAT HEAVY ELECTRICALS LIMITED, WITH ONE OF ITS REGIONAL OFFICES AT REGIONAL OPERATIONS DIVISION(ROD),PLOT NO.9/1, DJBLOCK, 3RD FLOOR KARUNAMOYEE, SALT LAKE CITY, KOLKATA-700091, HAVING ITS REGISTERED OFFICE AT BHEL HOUSE, SIRIFORT, NEW DELHI-110049, INDIA
PCT International Classification Number H01H 3/30
PCT International Application Number N/A
PCT International Filing date
PCT Conventions:
# PCT Application Number Date of Convention Priority Country
1 NA