Distributed impedance injection module for mitigation of the Ferranti effect

Information

  • Patent Grant
  • 10180696
  • Patent Number
    10,180,696
  • Date Filed
    Monday, November 7, 2016
    7 years ago
  • Date Issued
    Tuesday, January 15, 2019
    5 years ago
Abstract
Disclosed is a method for reducing the variation in voltage, due to Ferranti effect, using the impedance injection capability of distributed impedance injection modules. The Ferranti effect is an increase in voltage occurring at the receiving end of a long transmission line in comparison to the voltage at the sending end. This effect is more pronounced on longer lies and underground lines when the high-voltage power lines are energized with a very low load, when there is a change from a high load to a very light load, or the load is disconnected from the high-voltage power lines of the power grid. This effect creates a problem for voltage control at the distribution end of the power grid.
Description
BACKGROUND OF THE INVENTION

1. Field of the Invention


The present invention relates to systems and methods for distributed control of the inductive and capacitive loading of high voltage power transmission lines by using online injection modules that hang on or are connected to the power lines and are enabled for line balancing and distributed control.


2. Prior Art


Long transmission lines 102 of the power transmission system 100 shown in FIG. 1 are hung from transmission towers 101 and are used to transfer power, schematically shown as transferring power from generator 103 to load 104. These transmission lines, if long, can have a considerable shunt capacitance and series inductance, together with the transmission line resistance, which are distributed along the entire length of the line. Under these conditions, when the receiving-end power load is very small, or the circuit is open, the voltage at the receiving-end of the transmission line can rise to a level substantially higher than the voltage at the supply-end of the transmission line.


The foregoing effect is referred to as the Ferranti effect, and is caused by the combined effects of the distributed shunt capacitance and series inductance giving rise to a charging current in the transmission line. In particular, the transmission line 102 of FIG. 1 can be represented by the distributed π-model 200 shown in FIG. 2. FIG. 2 illustrates the power line with distributed resistance R 204 and inductance L 205 per unit length segment 201. Capacitance C 203 represents a shunt capacitance between the neighboring lines and ground.


Consider the lumped model of FIG. 3 which illustrates a lumped RLC circuit 300 representation of the distributed model 200 of the high voltage transmission line. FIG. 3 is a simplified representation of the high voltage transmission line drawing power from the supply side to the receiving side. Supply voltage {right arrow over (VR)} 206 has a shunt capacitance CS 302 and capacitive supply current {right arrow over (ICS)} 308 with ground. Receiving voltage {right arrow over (VR)} 207 has a shunt capacitance CR 303 and capacitive receiving current {right arrow over (ICR)} 309 with ground, in parallel with the LoadRL 312 having a load current {right arrow over (ILoad)} 311.


Now consider FIG. 4A, the phase diagram 400, and to most simply illustrate the Ferranti effect, consider the LoadRL 312 to be zero, that is the LoadRL 312 is open circuited (disconnected) with the load current {right arrow over (ILoad)} 311 equal to zero, then Vector {right arrow over (VR)} 207 represents the voltage at the receiving end of the transmission line, and appears across the capacitance CR 303. Because the AC current into a capacitor leads the AC voltage on the capacitor by 90 degrees, the AC current {right arrow over (ICR)} 309 in the transmission line leads the voltage on the capacitor CR, namely {right arrow over (VR)} 207, as shown in FIG. 4A. Thus the voltage drop in the line caused by the charging current for capacitor CR 303, being supplied through the line resistance R 304, is the voltage and {right arrow over (ΔVR)} 403 across resistor 304, is inphase with the charging current {right arrow over (ICR)} 309 as shown. That charging current also passes through the transmission line inductance L 305. Since the AC voltage in an inductor L leads the AC current on an inductor by 90 degrees, the voltage Δ{right arrow over (VL)} 404 across the inductor L is phase shifted another 90 degrees, as shown in the phase diagram 400. The net result is the voltage {right arrow over (VS)} 206, the voltage at the source end of the transmission line, which as can be seen in FIG. 4A, has a magnitude that is less than the voltage {right arrow over (VR)} 207 at the receiving end of the transmission line.


When the LoadRL 312 is not zero, the Ferranti effect does not disappear, but at least for substantial loads, the effects of the capacitive shunt current becomes masked by the dominance of the effects of the load current {right arrow over (ILoad)} 311, that is the resultant series inductive and resistive drops due the load current {right arrow over (ILoad)} 311 which is normally much larger than the drops due to the capacitive charging current at no-load conditions. The effects of the shunt capacitor charging current, under these conditions, tends to be lumped with the overall characteristics of the power distribution system for any corrections that may be attempted to maintain voltages, power factors, etc. within desirable limits.


It will be good to have an adaptive solution that can prevent or control the Ferranti effect from increasing the voltage at the receiving end of transmission lines when the load is reduced. What is proposed by the present invention is such a solution implemented using the distributed injection modules, which are also sometimes referred to as active impedance injection modules or distributed voltage/impedance injection modules that have been proposed by the parent applications of the current invention.





BRIEF DESCRIPTION OF THE DRAWINGS

The drawings are made to point out and distinguish the invention from the prior art. The objects, features, and advantages of the invention are detailed in the description taken together with the drawings.



FIG. 1 is a block diagram of the transmission line as per the prior art.



FIG. 2 is a schematic representation of the (distributed it-model) equivalent circuit of the transmission line of FIG. 1 showing the distributed nature of the resistance, inductance, and capacitance associated with the transmission line.



FIG. 3 is a schematic representation of the lumped constant (π-model) equivalent circuit of the transmission line of FIGS. 1 and 2.



FIG. 4A is a phase diagram of the current-voltage relationships illustrating the Ferranti effect and its cause.



FIG. 4B is a phase diagram 410 of the current-voltage relationship after correction voltage has been applied to mitigate Ferranti effect.



FIG. 5 is a block diagram of a first embodiment of a distributed Voltage/Impedance injection module with a multi-turn primary winding.



FIG. 6 is a block diagram of a second embodiment of a distributed voltage/impedance injection module having a plurality of single turn primary windings.



FIG. 7 is a block diagram of the transmission line with distributed voltage/impedance injection modules attached directly to the HV-transmission-lines.



FIG. 8 shows a block diagram representation of a long HV transmission line showing the distributed voltage/impedance injection modules covering each segment of the HV transmission line.





DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

The invention disclosed herein is generally directed at providing a system and method for controlling or limiting the increase in voltage at the load end of a long transmission line by using impedance/voltage injection modules, such as, but not limited to, those disclosed in U.S. Pat. No. 7,105,952.


A plurality of implementations of injection modules has been proposed by the present inventors to allow balancing of the power transferred over a transmission line by changing the line impedance locally. By making these injection modules intelligent, self-aware, and with local intercommunication capability, it is possible to monitor locally and control the power flow over the high-voltage transmission (HV transmission) lines of the power grid. The distributed injection modules are enabled to recognize changes in the power flow characteristics and inject impedances to compensate for the unwanted changes in the high-voltage (HV) transmission lines.


While these injection modules could be directly connected in series with the transmission line with ground connection, this is not normally done because of the need to provide insulation that can sustain high line voltage differences to ground at each module, which will become prohibitively expensive and also make the modules heavy. In practice, the impedance modules are can be electrically and mechanically connected to the transmission line, and are at line potential, or alternatively only magnetically coupled to the transmission line, but in either case, they are enabled to respond to transmission line current variations. These impedance injection modules are ideal candidates for distributed implementation, as existing high voltage power transmission systems can be retrofitted without disturbing the transmission line itself, though alternate implementation of impedance/voltage injection module installations using movable and other support structures are also usable for correcting the Ferranti effect. (The distributed impedance/voltage injection is described in detail as it is the preferred mode for this application). Thus in substantially all cases, the impedance/voltage injection modules respond to transmission line current and not transmission line voltage. Any transmission line corrections that require line voltage information such as corrections in voltage and power factor by each injection module are made by instructions received by wireless, wireline or power line communication to the module based on current measurements made by that module, other communicably linked modules or other line current measurement capability coupled to the high voltage power lines and again communicably linked to the impedance/voltage injection modules, and voltage measurements made at the next line voltage measurement facility, typically at the next substation.


As previously described, phase diagram FIG. 4A illustrates the Ferranti effect. As can be seen from that FIG. 4A, the Ferranti effect arises from the AC-charging current in the line inductance L (FIG. 3). Accordingly, injection of a correcting impedance/voltage onto the line can reduce or eliminate this component, leaving the Δ{right arrow over (VR)} 403 component, which can be considered a load characteristic and handled as part of a power factor correction.



FIG. 4B shows the voltage-current vector relationship 410 with the correction voltage vector {right arrow over (VCor)} 402 applied to correct the increase in voltage due to Ferranti effect. The resultant voltage vector at the receiver {right arrow over (VR)}, new 407 is the compensated voltage across the capacitor CR 303 when the LoadRL 312 is not present or is very low.



FIG. 5 shows an injection module 500 previously disclosed (U.S. patent application Ser. No. 15/055,422) having a transformer 501 with a multi-turn primary winding which is attached to the transmission line by cutting the line and splicing the module in series with the transmission line. The injection module 500 has a controller 504 that senses the changes in current transmitted over the transmission line 102 and voltage information transmitted to the module, and uses them to control the output of a converter 503. Alternatively, the injection module may wirelessly communicate current measurements to the next substation, and the substation, or a separate control station (not shown) wirelessly send specific instructions to the injection module 500 and similar injection modules on the transmission line. The converter 503 generates an impedance (or voltage) that when impressed in a distributed fashion on the transmission line via the transformer 501, can compensate for the changes on the transmission line 102. In this configuration, the module 500 can be electrically connected directly to the power transmission line 102, if desired, and insulated from ground, or allowed to float with respect to the transmission line. The power for the controller is also extracted from the transmission line by a second transformer 502 connected to a power supply module. Any transmission line voltages needed for transmission line control are measured at one or more substations and wirelessly transmitted to the injection modules, or the current measured by the injection modules transmitted to a control location also having the transmission line voltage measurements and the control location transmitting instructions to the injection modules for the desired injection module response.



FIG. 6 shows a second embodiment of intelligent and self-aware injection module 600 previously disclosed (U.S. patent application Ser. No. 15/069,785) that uses a plurality of single turn primary transformers 601 to couple the output produced by the converters 603 to couple the control voltage to the power line 102. A sensor and power supply module 602 that couples to the power transmission line is used to sense the changes in current in the transmission line 102 and feed it to the controller 604. The controller 604 then provides the necessary instructions to the converters 603 coupled to it. The sensor and power supply module 602 also extracts power from the transmission line to supply to the controller 604 and the other electronic control circuits of the module. This magnetic coupling requires no direct connection to the high voltage transmission line and/or cutting and splicing thereof, and therefore is better suited for a retrofit of existing transmission systems, and even for new installations, should be less costly to implement. The only consideration is the support and insulation for the injection module. In that regard, modules that are only magnetically coupled to the high voltage transmission line are not grounded, but allowed to electrically float with the respect to the transmission line so must be supported using the required insulative characteristics, though usually adequate support and insulation are already available at the support towers, provided the size and weight of the injection modules is appropriately chosen by design.



FIG. 7 is a schematic illustration 700 of a long distribution line where the intelligent and self-aware injection modules 701 are distributed over the transmission line 102 at the towers 101 to monitor and control the impedance of the line and provide line balancing and power transfer control capability from the generators 103 to the load 104. These injection modules 701 can also be effectively used to reduce or eliminate the Ferranti effect by injecting a corrective inductance in the high voltage line to reduce or eliminate the Δ{right arrow over (VL)} 404 voltage component in FIG. 4A which gives rise to the Ferranti effect. Instead or in addition, a corrective capacitance could be injected by the injection modules 701 which would reduce the transmission line current {right arrow over (IRL)} 310 charging capacitor CR 303 and thus reduce the current through and hence the voltage Δ{right arrow over (VL)} 404 across the inductance L 305 (FIG. 3).


As discussed earlier, concerning the phase diagram 400 in FIG. 4A, the Ferranti effect is produced when the load current on the transmission lines is very low, the load is removed, or the line is open-circuited. These scenarios result in the current of the high voltage transmission line comprising mainly the current in the distributed shunt capacitor of the high voltage transmission line. This capacitive current produces voltage drops in the distributed series inductors L 205 and the distributed resistors R 204 of the high voltage transmission line. The phasor diagram of FIG. 4A illustrates that due to the phase differences introduced by the capacitive current {right arrow over (ICR)} 309 flowing in the line inductance L 305, an additional voltage drop is produced, shown by the phasor Δ{right arrow over (VL)} 404. This additional voltage drop is 180 degrees out of phase with the received voltage VR 207 at the receiving end of the transmission line. This combined with the inphase resistive drop {right arrow over (ΔVR)} 403, in the line resistance R 304, produces the resultant Ferranti effect voltage vector {right arrow over (VS)}-{right arrow over (VR)} 401 that makes the magnitude of sending end voltage {right arrow over (VS)} 206 illustrated in FIG. 4A smaller than the magnitude of the voltage at the receiving end {right arrow over (VR)} 207 of FIG. 4A.


Since the voltage rise is a distributed function that is cumulative over the length of the HV transmission line, it is possible to introduce corrective changes by the preferred method of injecting the correct voltage (impedance) values by the voltage/impedance injection modules distributed over the HV transmission line. Alternately the correction can be applied, as injected voltages to correct the cumulative effect over sections of the high voltage transmission line by using groups of impedance/voltage injection modules, at different points in the line. Both such corrections will be very effective in overcoming the Ferranti effect.



FIG. 8 shows each of the distributed segments 801-1 and 801-2 of the HV transmission line 102. At least one injection module 701 is attached to or suspended from and used to provide a transmission line balancing capability. The distributed segments 801 of the HV transmission line are represented by the distributed impedance diagram 201 of FIG. 2. The injection modules 701 receive wireless control signals from the receiving substation, or from separate localized intelligent centers which themselves receive the needed information from the receiving substation (not shown). Since a long transmission line is involved, the transmission line length may exceed the capabilities of the wireless communication, though the needed control information may easily be sequentially relayed by the injection modules themselves, or by the localized intelligent centers previously referred to. In that regard, note that it is not a disturbance that is being corrected, but a characteristic of the transmission line itself. Consequently, the injection modules themselves, having a transmission line current sensing capability, can be programmed to use a default Ferranti effect correction when they sense the low transmission line current characteristic of an unloaded transmission line, which default correction can then be adjusted for any changes in transmission line characteristics due to weather, etc., based on the actual voltage measurements at the receiving end of the transmission line.


Note also that the Ferranti effect is not a “strong” effect in comparison to other conditions sought to be corrected by the injection modules (line balancing, power factor correction, etc.), but is a cumulative effect of a long transmission line 102. Consequently, the number of injection modules used for overall transmission line control may easily exceed the number needed simply for correction of the Ferranti effect, in which case one might use an equally spaced subset of the available modules for this purpose.


The injection modules are sometimes referred to as impedance/voltage injection modules, as the function of the modules for the present invention is the injection of an effect onto the transmission line with the proper phasing to achieve the desired result, specifically the diminishing or cancellation of the voltage {right arrow over (ΔVL)} 404 as shown in FIG. 4B. The injection might be considered an injection of an opposing voltage {right arrow over (VCor)} 402, or alternatively, the injection of a cancelling inductance, that counteract the line inductance L 305. Any power needed for the injection itself is also taken from the transmission line prior to the injection through the magnetic coupling from and to the transmission line.


Even though the invention disclosed is described using specific implementations, circuits, and components, it is intended only to be exemplary and non-limiting. The practitioners of the art will be able to understand and modify the same based on new innovations and concepts, as they are made available. The invention is intended to encompass these modifications.

Claims
  • 1. A method of reducing or eliminating a Ferranti effect in a high voltage transmission line comprising: coupling impedance/voltage injection modules to the high voltage transmission lineat spaced apart locations along the high voltage transmission line, the impedance/voltage injection modules each being powered from the high voltage transmission line and having a high voltage transmission line current sensing capability, an impedance/voltage injection capability and a communication capability; andusing at least a subset of the impedance/voltage injection modules, sensing current in the high voltage transmission line; andwhen the high voltage transmission line current indicates that a high voltage transmission line load at a receiving end of the high voltage transmission line is low or zero, injecting an impedance/voltage onto the high voltage transmission line at spaced apart locations along the high voltage transmission line to collectively reduce or cancel a voltage generated by a current charging a line capacitance passing through a line impedance.
  • 2. The method of claim 1 wherein all impedance/voltage injection modules are used to inject the impedance/voltage onto the high voltage transmission line to reduce or cancel the voltage generated by the current charging the line capacitance passing through the line impedance when the high voltage transmission line current indicates that the high voltage transmission line load at a receiving end of the transmission line is low or zero.
  • 3. The method of claim 1 wherein the at least a subset of the impedance/voltage injection modules sense the current in the high voltage transmission line and automatically inject the impedance/voltage onto the high voltage transmission line at spaced apart locations along the high voltage transmission line to collectively reduce or cancel the voltage generated by the current charging the line capacitance passing through the line impedance when the current in the high voltage transmission line indicates that the high voltage transmission line load at the receiving end of the high voltage transmission line is low or zero.
  • 4. The method of claim 3 further comprising receiving information relative to the voltage on the high voltage transmission line at the receiving end of the high voltage transmission line and adjusting the injection of an impedance/voltage onto the high voltage transmission line at spaced apart locations along the high voltage transmission line to further control the voltage at the receiving end of the high voltage transmission line.
  • 5. A method of reducing or eliminating a Ferranti effect in a high voltage transmission line comprising: identifying a low current in the high voltage transmission line using a current sense device within at least a distributed impedance/voltage injection module coupled to the high voltage transmission line;determining an increase in line voltage, due to the Ferranti effect, at a load or substation end due to the low current in the high voltage transmission line;injecting a voltage using at least a selected number of distributed impedance/voltage injection modules to compensate for the increase in line voltage at the load or substation end;thereby correcting the Ferranti effect on the high voltage transmission line.
  • 6. The method of claim 5, wherein the distributed impedance/voltage injection modules are powered from a power drawn from the high voltage transmission line.
  • 7. The method of claim 5, wherein the distributed impedance/voltage injection modules are suspended from the high voltage transmission line and are at a line potential of the transmission line.
  • 8. The method of claim 5, wherein the determined increase in line voltage at the load end of the line due to the Ferranti effect is corrected by a cumulative incremental distributed voltage injection by the distributed impedance/voltage injection modules coupled to the high voltage transmission line.
  • 9. A system for controlling a voltage increase in a high voltage transmission line due to a Ferranti effect, the system comprising: a plurality of distributed impedance/voltage injection modules coupled to the high voltage transmission line;a line current sensing circuit associated with each impedance/voltage injection module;an impedance/voltage injection circuit associated with each impedance/voltage injection module;a voltage sensing and comparison capability at a load/substation end of the high voltage transmission line; anda communication channel from the load/substation end of the high voltage transmission line to the distributed impedance/voltage injection modules for transferring information regarding a voltage sensed at the load/substation end of the high voltage transmission line;wherein when a low current is sensed by the plurality of distributed impedance injection modules and an intimation of over voltage is received over the communication channel, each of the plurality of impedance/voltage injection modules generate and inject an incremental voltage on to the high voltage transmission line in a manner that a cumulative injected voltage from the plurality of impedance/voltage injection modules is sufficient to reduce or overcome the increase in voltage due to the Ferranti effect at the load/substation end of the high voltage transmission line.
  • 10. The system of claim 9, wherein a voltage correction is by equal distributed incremental voltage by each of the plurality of impedance/voltage injection modules.
  • 11. The method of claim 1, wherein the communication capability is any one of a wireless communication capability, a wire line communication capability or a power line communication capability.
  • 12. A method of reducing or eliminating a Ferranti effect in a high voltage transmission line comprising: coupling a plurality of impedance/voltage injection modules to the high voltage transmission line, the impedance/voltage injection modules each being powered from the high voltage transmission line and having an impedance/voltage injection capability and a communication capability; andusing at least a current sensing capability available on the high voltage transmission line, sensing a current in the high voltage transmission line; andwhen the high voltage transmission line current indicates that a high voltage transmission line load at a receiving end of the high voltage transmission line is low or zero, injecting an impedance/voltage onto the high voltage transmission line using the impedance/voltage injection modules to collectively reduce or cancel a voltage generated by a current charging a line capacitance passing through a line impedance.
  • 13. A system for controlling a voltage increase in a high voltage transmission line due to a Ferranti effect, the system comprising: a plurality of distributed impedance/voltage injection modules coupled to the high voltage transmission line;a line current sensing capability coupled to the high voltage transmission line and communicably linked to the impedance/voltage injection modules;a voltage sensing and comparison capability at a load/substation end of the high voltage transmission line; anda communication channel from the load/substation end of the high voltage transmission line to the distributed impedance/voltage injection modules for transferring information regarding a voltage sensed at the load/substation end of the high voltage transmission line;wherein when a low current is sensed by the line current sensing capability and an intimation of over voltage is received over the communication channel, each of a subset of the plurality of impedance/voltage injection modules generate and inject an incremental voltage on to the high voltage transmission line in a manner that a cumulative injected voltage from the plurality of impedance/voltage injection modules is sufficient to reduce or overcome the increase in voltage due to the Ferranti effect at the load/substation end of the high voltage transmission line.
CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation-in-part of U.S. patent application Ser. No. 15/055,422 filed Feb. 26, 2016, which claims the benefit of U.S. Provisional Patent Application No. 62/264,739 filed Dec. 8, 2015, and is a continuation-in-part of U.S. patent application Ser. No. 15/069,785 filed Mar. 14, 2016, which claims the benefit of U.S. Provisional Application No. 62/264,744 filed Dec. 8, 2015, and this application also claims the benefit of U.S. Provisional Patent Application No. 62/359,885 filed Jul. 8, 2016.

US Referenced Citations (158)
Number Name Date Kind
2237812 De Blieux Apr 1941 A
2551841 Kepple et al. May 1951 A
3556310 Loukotsky Jan 1971 A
3704001 Sloop Nov 1972 A
3750992 Johnson Aug 1973 A
3913003 Felkel Oct 1975 A
4025824 Cheatham May 1977 A
4057736 Jeppson Nov 1977 A
4103853 Bannan Aug 1978 A
4164345 Arnold et al. Aug 1979 A
4200899 Volman et al. Apr 1980 A
4277639 Olsson Jul 1981 A
4286207 Spreadbury et al. Aug 1981 A
4323722 Winkelman Apr 1982 A
4367512 Fujita Jan 1983 A
4514950 Goodson, Jr. May 1985 A
4562360 Fujimoto Dec 1985 A
4577826 Bergstrom et al. Mar 1986 A
4710850 Jahn et al. Dec 1987 A
4821138 Nakano et al. Apr 1989 A
4903927 Farmer Feb 1990 A
5006846 Granville et al. Apr 1991 A
5023768 Collier Jun 1991 A
5032738 Vithayathil Jul 1991 A
5193774 Rogers Mar 1993 A
5461300 Kappenman Oct 1995 A
5469044 Gyugyi et al. Nov 1995 A
5610501 Nelson et al. Mar 1997 A
5648888 Le Francois et al. Jul 1997 A
5844462 Rapoport et al. Dec 1998 A
5884886 Hageli Mar 1999 A
5886888 Akamatsu et al. Mar 1999 A
5986617 McLellan Nov 1999 A
6088249 Adamson Jul 2000 A
6134105 Lueker Oct 2000 A
6147581 Rancourt et al. Nov 2000 A
6215653 Cochran et al. Apr 2001 B1
6233137 Kolos et al. May 2001 B1
6335613 Sen et al. Jan 2002 B1
6486569 Couture Nov 2002 B2
6727604 Couture Apr 2004 B2
6831377 Yampolsky et al. Dec 2004 B2
6895373 Garcia et al. May 2005 B2
6914195 Archambault et al. Jul 2005 B2
7090176 Chavot et al. Aug 2006 B2
7091703 Folts et al. Aug 2006 B2
7105952 Divan et al. Sep 2006 B2
7193338 Ghali Mar 2007 B2
7352564 Courtney Apr 2008 B2
7460931 Jacobson Dec 2008 B2
7642757 Yoon et al. Jan 2010 B2
7688043 Toki et al. Mar 2010 B2
7834736 Johnson et al. Nov 2010 B1
7835128 Divan et al. Nov 2010 B2
7932621 Spellman Apr 2011 B1
8019484 Korba et al. Sep 2011 B2
8249836 Yoon et al. Aug 2012 B2
8270558 Dielissen Sep 2012 B2
8310099 Engel et al. Nov 2012 B2
8401709 Cherian et al. Mar 2013 B2
8441778 Ashmore May 2013 B1
8497592 Jones Jul 2013 B1
8680720 Schauder et al. Mar 2014 B2
8681479 Englert et al. Mar 2014 B2
8816527 Ramsay et al. Aug 2014 B1
8825218 Cherian et al. Sep 2014 B2
8867244 Trainer et al. Oct 2014 B2
8872366 Campion et al. Oct 2014 B2
8890373 Savolainen Nov 2014 B2
8896988 Subbaiahthever et al. Nov 2014 B2
8922038 Bywaters et al. Dec 2014 B2
8957752 Sharma et al. Feb 2015 B2
8996183 Forbes, Jr. Mar 2015 B2
9099893 Schmiegel et al. Aug 2015 B2
9124100 Ukai et al. Sep 2015 B2
9124138 Mori et al. Sep 2015 B2
9130458 Crookes et al. Sep 2015 B2
9172246 Ramsay Oct 2015 B2
9178456 Smith et al. Nov 2015 B2
9185000 Mabilleau et al. Nov 2015 B2
9207698 Forbes, Jr. Dec 2015 B2
9217762 Kreikebaum et al. Dec 2015 B2
9246325 Coca Figuerola et al. Jan 2016 B2
9325173 Varma et al. Apr 2016 B2
9331482 Huang May 2016 B2
9659114 He et al. May 2017 B2
9843176 Gibson Dec 2017 B2
20020005668 Couture Jan 2002 A1
20020042696 Garcia et al. Apr 2002 A1
20030006652 Couture Jan 2003 A1
20030098768 Hoffmann et al. May 2003 A1
20040217836 Archambault et al. Nov 2004 A1
20050052801 Ghali Mar 2005 A1
20050073200 Divan et al. Apr 2005 A1
20050194944 Folts et al. Sep 2005 A1
20050205726 Chavot et al. Sep 2005 A1
20060085097 Courtney Apr 2006 A1
20070135972 Jacobson Jun 2007 A1
20070250217 Yoon et al. Oct 2007 A1
20080103737 Yoon et al. May 2008 A1
20080157728 Toki et al. Jul 2008 A1
20080177425 Korba et al. Jul 2008 A1
20080278976 Schneider et al. Nov 2008 A1
20080310069 Divan et al. Dec 2008 A1
20090243876 Lilien et al. Oct 2009 A1
20090281679 Taft et al. Nov 2009 A1
20100026275 Walton Feb 2010 A1
20100177450 Holcomb et al. Jul 2010 A1
20100213765 Engel et al. Aug 2010 A1
20100302744 Englert et al. Dec 2010 A1
20110060474 Schmiegel et al. Mar 2011 A1
20110095162 Parduhn et al. Apr 2011 A1
20110106321 Cherian et al. May 2011 A1
20110172837 Forbes, Jr. Jul 2011 A1
20120105023 Schauder et al. May 2012 A1
20120146335 Bywaters et al. Jun 2012 A1
20120205981 Varma et al. Aug 2012 A1
20120242150 Ukai et al. Sep 2012 A1
20120255920 Shaw et al. Oct 2012 A1
20120293920 Subbaiahthever et al. Nov 2012 A1
20130002032 Mori et al. Jan 2013 A1
20130033103 McJunkin et al. Feb 2013 A1
20130044407 Byeon et al. Feb 2013 A1
20130094264 Crookes et al. Apr 2013 A1
20130128636 Trainer et al. May 2013 A1
20130166085 Cherian et al. Jun 2013 A1
20130169044 Stinessen et al. Jul 2013 A1
20130182355 Coca Figuerola et al. Jul 2013 A1
20130184894 Sakuma et al. Jul 2013 A1
20130200617 Smith et al. Aug 2013 A1
20130277082 Hyde et al. Oct 2013 A1
20130345888 Forbes, Jr. Dec 2013 A1
20140025217 Jin et al. Jan 2014 A1
20140032000 Chandrashekhara et al. Jan 2014 A1
20140111297 Earhart et al. Apr 2014 A1
20140129195 He et al. May 2014 A1
20140132229 Huang May 2014 A1
20140153383 Mabilleau et al. Jun 2014 A1
20140188689 Kalsi et al. Jul 2014 A1
20140203640 Stinessen Jul 2014 A1
20140210213 Campion et al. Jul 2014 A1
20140246914 Chopra et al. Sep 2014 A1
20140247554 Sharma et al. Sep 2014 A1
20140268458 Luciani et al. Sep 2014 A1
20140312859 Ramsay et al. Oct 2014 A1
20140327305 Ramsay et al. Nov 2014 A1
20140347158 Goeke et al. Nov 2014 A1
20150012146 Cherian et al. Jan 2015 A1
20150029764 Peng Jan 2015 A1
20150051744 Mitra Feb 2015 A1
20150184415 Bushore Jul 2015 A1
20150226772 Kreikebaum et al. Aug 2015 A1
20150244307 Cameron Aug 2015 A1
20150270689 Gibson et al. Sep 2015 A1
20160036231 Ramsay et al. Feb 2016 A1
20160036341 Jang et al. Feb 2016 A1
20170163036 Munguia et al. Jun 2017 A1
20170169928 Carrow et al. Jun 2017 A1
Foreign Referenced Citations (13)
Number Date Country
660094 Mar 1987 CH
103256337 Aug 2013 CN
203668968 Jun 2014 CN
2002-199563 Jul 2002 JP
2005-045888 Feb 2005 JP
2015-086692 May 2015 JP
10-1053514 Aug 2011 KR
WO-2008082820 Jul 2008 WO
WO-2014035881 Mar 2014 WO
WO-2014074956 May 2014 WO
WO-2014099876 Jun 2014 WO
WO-2015074538 May 2015 WO
WO-2015119789 Aug 2015 WO
Non-Patent Literature Citations (37)
Entry
“Office Action dated Nov. 3, 2017; U.S. Appl. No. 15/157,726”, Nov. 3, 2017.
“Office Action dated Jul. 26, 2017; U.S. Appl. No. 15/069,785”, (Jul. 26, 2017).
Amin, S. M., et al., “Toward a Smart Grid: Power Delivery for the 21st Century”, IEEE power & energy magazine, vol. 3, No. 5, (Sep./Oct. 2005), pp. 34-41.
Angeladas, Emmanouil , “High Voltage Substations Overview (part 1)”, Siemens, (Jan. 24, 2013), pp. 1-8.
Aquino-Lugo, Angel A., “Distributed and Decentralized Control of the Power Grid”, Ph.D. Dissertation, University of Illinois at Urbana-Champaign, (2010), 172 pp. total.
Dash, P. K., et al., “Digital Protection of Power Transmission Lines in the Presence of Series Connected FACTS Devices”, IEEE Power Engineering Society Winter Meeting, (2000), pp. 1967-1972.
Divan, D. M., “Nondissipative Switched Networks for High-Power Applications”, Electronics Letters, vol. 20, No. 7, (Mar. 29, 1984), pp. 277-279.
Funato, Hirohito , et al., “Realization of Negative Inductance Using Variable Active-Passive Reactance (VAPAR)”, IEEE Transactions on Power Electronics, vol. 12, No. 4, (Jul. 1997), pp. 589-596.
Gyugyi, Laszlo , et al., “Status Synchronous Series Compensator: A Solid-State Approach to the Series Compensation of Transmission Lines”, IEEE Transactions on Power Delivery, vol. 12, No. 1, (Jan. 1997), pp. 406-417.
Gyugyi, Laszlo , et al., “The Interline Power Flow Controller Concept: A New Approach to Power Flow Management in Transmission Systems”, IEEE Transactions on Power Delivery, vol. 14, No. 3, (Jul. 1999), pp. 1115-1123.
Kavitha, M. , et al., “Integration of FACTS into Energy Storage Systems for Future Power Systems Applications”, International Journal of Advanced Research in Electrical, Electronics and Instrumentation Engineering, vol. 2, Issue 2, (Feb. 2013), pp. 800-810.
Kumbhar, Mahesh M., et al., “Smart Grid: Advanced Electricity Distribution Network”, IOSR Journal of Engineering (IOSRJEN), vol. 2, Issue 6, (Jun. 2012), pp. 23-29.
Lambert, Frank C., “Power Flow Control”, ISGT Europe, 2014, Istanbul, Turkey, (Oct. 13, 2014), pp. 1-15.
Lehmkoster, Carsten , “Security Constrained Optimal Power Flow for an Economical Operation of FACTS-Devices in Liberalized Energy Markets”, IEEE Transactions on Power Delivery, vol. 17, No. 2, (Apr. 2002), pp. 603-608.
Mali, Bhairavanath N., et al., “Performance Study of Transmission Line Ferranti Effect and Fault Simulation Model Using MATLAB”, International Journal of Innovative Research in Electrical, Electronics, Instrumentation and Control Engineering, vol. 4, Issue 4, (Apr. 2016), pp. 49-52.
Mutale, Joseph , et al., “Transmission Network Reinforcement Versus FACTS: An Economic Assessment”, IEEE Transactions on Power Systems, vol. 15, No. 3, (Aug. 2000), pp. 961-967.
Ramchurn, Sarvapali D., et al., “Putting the ‘Smarts’ into the Smart Grid: A Grand Challenge for Artificial Intelligence”, Communications of the ACM, vol. 55, No. 4, (Apr. 2012), pp. 86-97.
Reddy, D. M., et al., “FACTS Controllers Implementation in Energy Storage Systems for Advanced Power Electronic Applications—A Solution”, American Journal of Sustainable Cities and Society, Issue 2, vol. 1, (Jan. 2013), pp. 36-63.
Renz, B. A., et al., “AEP Unified Power Flow Controller Performance”, IEEE Transactions on Power Delivery, vol. 14, No. 4, (Oct. 1999), pp. 1374-1381.
Ribeiro, P. , et al., “Energy Storage Systems”, Chapters 1-2.4 of Section entitled “Energy Storage Systems” in Electrical Engineering—vol. III, edited by Kit Po Wong, Encyclopedia of Life Support Systems (EOLSS) Publications, (Dec. 13, 2009), 11 pp. total.
Schauder, C. D., et al., “Operation of the Unified Power Flow Controller (UPFC) Under Practical Constraints”, IEEE Transactions on Power Delivery, vol. 13, No. 2, (Apr. 1998), pp. 630-639.
Siemens SAS, “Portable Power Solutions, “Plug and play” High Voltage E-Houses, skids and mobile high voltage substations up to 420 kV”, (Nov. 2015), 8 pp. total.
Swain, S. C., et al., “Design of Static Synchronous Series Compensator Based Damping Controller Employing Real Coded Genetic Algorithm”, International Journal of Electrical, Computer, Energetic, Electronic and Communication Engineering, vol. 5, No. 3, (2011), pp. 399-407.
Xue, Yiyan , et al., “Charging Current in Long Lines and High-Voltage Cables—Protection Application Considerations”, 67th Annual Georgia Tech Protective Relaying Conference, Atlanta, Georgia, (May 8-10, 2013), pp. 1-17.
“International Search Report and Written Opinion of the International Searching Authority dated Feb. 2, 2017; International Application No. PCT/US2016/062358”, (Feb. 2, 2017).
“International Search Report and Written Opinion of the International Searching Authority dated Feb. 2, 2017; International Application No. PCT/US2016/062620”, (Feb. 2, 2017).
“International Search Report and Written Opinion of the International Searching Authority dated Mar. 2, 2017; International Application No. PCT/US2016/061009”, (Mar. 2, 2017).
“Invitation of the International Searching Authority to Pay Additional Fees dated Dec. 15, 2016; International Application No. PCT/US2016/061009”, (Dec. 15, 2016).
“Notice of Allowance dated Feb. 22, 2018; U.S. Appl. No. 15/069,785”, Feb. 22, 2018.
“Office Action dated Apr. 6, 2018; U.S. Appl. No. 15/055,422”, Apr. 6, 2018.
“Office Action dated Apr. 6, 2018; U.S. Appl. No. 15/157,726”, Apr. 6, 2018.
“Office Action dated Jul. 27, 2018; U.S. Appl. No. 15/055,422”, Jul. 27, 2018.
Albasri, Fadhel A. et al., “Performance Comparison of Distance Protection Schemes for Shung-FACTS Compensated Transmission Lines”, IEEE Transactions on Power Delivery, vol. 22, No. 4, Oct. 2007, pp. 2116-2125.
Bhaskar, M. A. et al., “Impact of FACTS devices on distance protection in Transmission System”, 2014 IEEE National Conference on Emerging Trends in New & Renewable Energy Sources and Energy Management (NCET NRES EM), Dec. 16, 2014, pp. 52-58.
Samantaray, S. R. , “A Data-Mining Model for Protection of FACTS-Based Transmission Line”, IEEE Transactions on Power Delivery, vol. 28, No. 2, Apr. 2013, pp. 612-618.
“Notice of Allowance dated Sep. 24, 2018; U.S. Appl. No. 15/157,726”, Sep. 24, 2018.
“Office Action dated Oct. 4, 2018; U.S. Appl. No. 15/975,373”, Oct. 4, 2018.
Related Publications (1)
Number Date Country
20170160762 A1 Jun 2017 US
Provisional Applications (3)
Number Date Country
62359885 Jul 2016 US
62264744 Dec 2015 US
62264739 Dec 2015 US
Continuation in Parts (2)
Number Date Country
Parent 15069785 Mar 2016 US
Child 15345065 US
Parent 15055422 Feb 2016 US
Child 15069785 US