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Increased Security Rating of Overhead Transmission Circuits Using Compact Phase Design and High Phase Order Brian J. Pierre, Student Member, IEEE Abstract—In this paper the combination of compact phase design and high phase order (HPO), (e.g., ≥ three phase) is used to enhance the security ratings of overhead transmission circuits. The advantages of both technologies are used with the objectives of raising the power transmission capability, reducing right of way requirements, reducing the phase angle difference between the sending and receiving end voltages, and reducing the cost of bulk power transmission. Disadvantages of the proposed technology are also discussed. The main objectives of this paper are to: Discus the use of HPO to compact transmission lines Calculate HPO sequence reactances in terms of self and mutual reactances using properties of circulant matrices. Determine the increase in security rating for compact HPO vs. its three phase multicircuit counterpart. Index Terms—Power transmission, transmission engineering, high phase order, six phase, security rating, compact phase spacing, sequence components, sequence reactances, circulant matrices. I. INTRODUCTION IGH phase order has been proposed for overhead AC transmission for nearly 40 years. The literature of the field in the area of six-phase technology is copious including (as examples) the economics of six-phase [1], fault detection and analysis [2, 3], and electromagnetic impact [4]. An experimental six-phase line was constructed in the 1990s in Saratoga NY, and [5] describes results. The general study of HPO for higher phase order is less voluminous. Perhaps the seminal work on high phase order is that of Barnes [6], and references [7] and [8] are examples of other literature. The main advantages of HPO are the reduction of lineline (phase to phase) voltages, decrease of positive sequence reactance (X+), and reduction of electromagnetic interference of overhead power transmission lines. The advantage of HPO low phase to phase voltage is illustrated for the six phase case in which the phase to phase voltage magnitude is equal to the phase to neutral H The authors acknowledge the support of the Power Systems Engineering Research Center (PSerc) which is a Generation III National Science Foundation Industry University Cooperative Research Center, awards EEC-0001880, EEC-0968993. The authors also acknowledge the support of the U.S. Department of Energy for its PSerc future grid initiative. The authors are with the School of Electrical, Computer, and Energy Engineering at Arizona State University, Tempe, AZ 85287, and can be reached at {brian.pierre, heydt}@asu.edu. G. T. Heydt, Life Fellow, IEEE voltage magnitude. The lower phase to phase voltage allows the individual phases to be compacted, i.e., located closer together in space. This will be termed as compact HPO for purposes of this paper. The ultimate spacing limitations of the phase conductors are determined by codes (e.g., the National Electrical Safety Code [9]), consideration of the basic impulse level (BIL), the spacing required for live line maintenance, and physical interaction of the phase conductors. The compacted phases incur advantages such as the increase in mutual coupling between the phases. This decreases the X+ of the line. Since the active power level capability of the line for a given terminal voltage phase difference is inversely proportional to the X+ of the line (i.e., for „security limited‟ lines), compact HPO lines have higher security ratings than comparable three phase lines. To determine the security limit increase in compact HPO over comparable three phase construction, the X+ shall be evaluated. It should be noted that comparison of HPO lines with three phase circuits is complicated by issues of what parameters are to remain constant in the comparison. These parameters include the phase to phase voltage, phase to ground voltage, conductor size and ampacity, and cost. For purposes of this paper, voltage phase to phase and phase to phase spacing are the control parameters that are varied. The phase compaction is considered to be linearly related to the decrease in phase to phase voltage. As indicated above, phase to phase spacing is nominally limited by code requirements. The approach taken in the literature has been to examine modest compaction. As examples, references [10] and [11] relate to phase compaction in transmission engineering. II. USING HPO LOWER PHASE TO PHASE VOLTAGE TO COMPACT TRANSMISSION LINES The phase to phase and phase to neutral voltage magnitudes, |Vll|, |Vln| and the number of phases are related by, (1) ( √ ( where n is the number of phases. The |Vll| / |Vln| vs. the number of phases is depicted in Fig 1. The lower phase to phase voltage magnitude at higher phase orders allows for reduced insulation requirements between phases. In this sense, for HPO, a more compact line can be constructed. For the same phase ampacity in comparison circuits, a 500 kV double circuit 3φ line will carry the 2 same power as a 288.7 kV 6φ line. In addition, the 6φ line can be compacted thus decreasing the required right of way (ROW). 2 1.8 Vll if Vln is held at 1.0 V 1.6 1.4 1.2 ble. The general concept is attributed to Nikola Tesla [13]. Perhaps the simplest HPO technology is the 6φ case. Consider a 6φ transmission line on which the phases are arranged in a regular hexagon as shown in Fig. 3. Consider the line reactance matrix as a lumped parameter, lossless 6φ transmission line model, 1 0.8 0.6 (3) 0.4 0.2 0 0 10 20 30 40 Number of phases 50 60 Fig. 1 |Vll| / |Vln| vs. number of phases III. SECURITY RATING Compaction decreases the positive sequence reactance which increases the security rating of a transmission line. The security limit of a short, lossless transmission line is ( , 7000 Security rating Thermal rating Rating (MW) 5000 4000 3000 where the distances are √ less for 6 phase vs. the distances in double circuit 3φ (2) where |V1 | and |V2 | are the voltage magnitudes at the line terminals and δmax is the maximum tolerable voltage phase angle difference. The security limit is often calculated using 30° as δmax. In (2), only the active power flow due to the positive sequence voltages and currents is calculated. Unbalanced operation is not considered. In (2), a short, lumped, lossless model is used. It is possible to include circuit resistance to capture losses, and it is also possible to use a long line („hyperbolic‟) model that is accurate at one frequency (e.g., 60 Hz). Generally, long lines are limited by security constraints, whereas short lines are limited by thermal constraints, as seen in Fig. 2 (offered as a typical characteristic for a 3φ 500 kV Drake circuit). Therefore, HPO compaction can be beneficial for long lines. 6000 [ ] where S is the line self-reactance, and the Mi are mutual reactances related to di shown in Fig. 3. 500 kV Drake two bundle at 18 in. phase spacing 40 ft. Fig. 3 Configurations and X+ for a double circuit 3φ and 6φ line. The notation S refers to the self inductive reactance of a given phase, and M1 is the mutual reactance with an adjacent phase, and M2 and M3 are the mutual reactances with more distant phases. The subject of circulant Toeplitz matrices is described in [12], and of special interest is the case of a symmetrical circulant Toeplitz (SCT) matrix. When any number of conductors are arranged in a circular symmetric formation (as in Fig. 3), the line impedance matrix is in SCT form, as seen in (3). A circulant matrix has a unique property that all circulant matrices of size nxn share the same n eigenvectors, m = 0, 1, … , n-1, [12], ( [ ] ( √ These n eigenvectors can be arranged in columns to form a modal matrix T to diagonalize Xph, ( The eigenvalues of Xph are calculated using [12], 2000 ∑ 1000 0 0 50 100 Line length (miles) 150 Fig. 2 Line length vs. security and thermal rating of a lossless line: exemplary parameters shown for a 3φ Drake 500 kV line IV. SYMMETRICAL CIRCULANT TOEPLITZ MATRICES High phase order was initially considered at the inception of AC power generation and transmission. Three phase designs have a distinct advantage in that with the addition of a single phase conductor over single phase counterparts, triple power transmission is possi- ( where Xph,1,k is the kth entry of row one of the Xph matrix, m is the mth eigenvalue, and n is the number of phases. Note that λm is the discrete Fourier transform of the sequence {Xph,1,0, Xph,1,1, …, Xph,1,n-1}. V. SIX PHASE VS. DOUBLE CIRCUIT THREE PHASE The 6φ phase to neutral voltages are given by the vector [1 b5 b4 b3 b2 b]t where b is 1/60o. Note that b is one of the six complex roots of unity. It is possible to decouple the 6φ system into six single phase circuits much like is done for 3φ systems and symmetrical com- 3 ponents [14]. The reactance „sequence components‟ can be found using (5), % increase in security rating 14 (7) [ ] [ ] where „diag‟ refers to making the argument vector into a 6x6 diagonal matrix. The terminology of the six sequence names, ns, pt, ..., was proposed in reference [14]. The phase spacing and reactances of any candidate line are [15], ( ( ( ( ) ) ( ) ) ( 13 12 11 10 9 8 7 0 10 20 30 40 phase spacing distance, d2 3ph, (ft) 50 Fig. 5 The percent increase in security rating for comapct 6φ over double circuit 3φ is plotted versus phase spacing (distance d2) of the original double circuit 3φ. with GMR and dab (in feet). Assume that phase to phase spacing is linearly related to the phase to phase voltage. If the 6φ voltage phase to phase is 1/√ times the comparison 3φ phase to phase voltage magnitude, the spacing can be √ times closer in the 6φ line. This will be termed compact six phase construction. To determine the increase in security rating for compact 6φ as compared to a double circuit 3φ design, the conductor configuration is shown in Fig. 3. For the configuration in Fig. 3, each distance will be related to the double circuit 3φ distance, d2. Use the following notation, Double circuit three phase √ √ VI. TWELVE PHASE VS. QUADRUPLE THREE PHASE For further testing of compact HPO, a comparison will be made between quadruple 3φ and 12φ. The phase to phase voltage for 12φ is a factor of 0.29886 less than the 3φ case. For this reason, the phases in 12φ can be compacted by the same factor. The configurations for the resultant 12 conductors can be seen in Fig. 6. Using the configuration in Fig. 6, the line reactance matrix is the SCT matrix X12ph, (10) Compact six phase √ Using (7)-(9), the positive sequence reactances are ( ( √ [ ) ] √ √ ) + Using GMR = 0.0375 ft. corresponding to Drake, the X vs. phase spacing is found and depicted in Fig. 4. The percent increase in security rating for 6φ over double circuit 3φ is depicted in Fig. 5. Where the distances will be a factor of 0.29886 less for 12 phase vs. the distances in quadruple circuit 3 phase. X+ (Ohm/mile of line length) 1 0.9 Fig. 6 Configurations and X+ for quadruple circuit 3φ and 12φ respectively 0.8 0.7 double circuit 3-phase Compact 6-phase 0.6 0.5 0.4 0 10 20 30 40 phase spacing distance, d2 3ph, (ft) 50 Fig. 4 Comparison of X+ for double circuit 3φ, and compact 6φ vs. phase spacing of the original double circuit 3φ (for GMR of 0.0375 ft. Drake conductor). Analogous to the 6φ case, the sequence components for a 12φ system, pictorially shown in [16], is found and expressed in terms of one of the twelve complex roots of unity, namely c = 1/30o. The twelve eigenvectors form the modal matrix T12ph, 4 . √ [ √ √ √ √ √ √ 1.2 1.1 1 Quadruple circuit 3-phase Compact 12-phase 0.9 0.8 10 20 30 40 phase spacing distance, d1 3ph, (ft) 50 Fig. 8 Comparison of X+ for quadruple circuit 3φ, and compact 12φ vs. original quadruple circuit 3φ, phase spacing (for GMR of 0.0375 ft. Drake conductor). 17 % increase in security rating √ 1.3 0.7 0 ] Similar to the 6φ case, using (5)-(6), for 12φ the twelve sequence reactances are, [ X+ (Ohm/mile of line length) 1.4 ] √ [ ] Note that T12ph is independent of the values of the Mi and S and this modal matrix is given by the eigenvectors (4) arranged in columns. For the configuration in Fig. 6, use the following notation to relate all the distances to distance d1 of the quadruple circuit 3φ case. As before, Quadruple circuit three phase Twelve phase Using (8), (9), the 12φ X+ equation, and the distances above, [ ( [ ( )] )] As an illustration for GMR = 0.0375 ft, Figs. 8 and 9 depict X+ and the increase in security rating in the 12φ case. VII. HPO PHASE COMPACTION BENEFITS AND DISADVANTAGES Loading of adjacent transmission assets There is a potential benefit of reducing loading on critical transmission circuits by phase compaction through the use of lower reactance parallel paths. The same advantage is a disadvantage in that some adjacent circuit assets may experience undesired loading (especially adjacent transformers which may require upgrading). 16 15 14 13 12 11 10 0 10 20 30 40 phase spacing distance, d1 3ph, (ft) 50 Fig. 9 The percent increase in security rating for compact 12φ over quadruple circuit 3φ is plotted versus phase spacing (distance d1) of the original quadruple circuit 3φ. Decreased electric and magnetic field strength The electric and magnetic fields of an overhead line may be decreased using phase compaction [5, 10]. Tower height is related to the electric and magnetic field strengths at ground level. There may be implications of permissible lower tower height and further reduction of ROW using phase compaction. Corona levels Compaction of conductors makes electric field strength between conductors higher, and there is simultaneous increase in corona, corona losses, and audible noise. Note that for high phase order, however, there may be an advantageous reduction of corona due to reduced phase to phase voltage in some designs. Decreased ROW Phase compaction results in obvious reduced ROW. The disadvantages of reduced phase spacing include more difficult or preclusion of live line maintenance and circuit maintenance in general. The decreased phase spacing may be unacceptable to some operating companies and in some jurisdictions – regardless of the benefits. Decreased lightning exposure The smaller cross-section of the transmission circuit in the landscape view results in less lightning exposure. Increased shunt capacitance Phase compaction results in higher shunt capacitance. The shunt capacitance is proportional to the in- 5 verse of the logarithm of the spacing and geometric mean distances of the phase conductors and their images, and therefore compaction results in higher shunt capacitance. The higher capacitance results in lower surge impedance, and therefore higher surge impedance loading (SIL) of the line [10]. Although the higher SIL may not result in actual operating point change (note that SIL is simply an index or yardstick of the loadability of the line, and not a measure of the actual operating point), there may be advantages in long line applications. The increased shunt capacitance will raise the operating voltage magnitude. In some cases this is an advantage and in some cases this is a disadvantage. The increased shunt capacitance causes higher inrush current when the line is energized. Probability of flashover Reports in [10] indicate switching surge flashovers in an experimental 500 kV compact design were more prevalent than in conventional designs. Voltage and current unbalance Reference [10] reports better charging current balance among the phases for a compact 3φ experimental 500 kV line vs. a traditionally spaced line. This potentially allows lines of hundreds of kilometers to be untransposed. Use of interphase spacers Phase compaction results in an obvious increase for the potential interaction between adjacent phases. The use of interphase (insulating) spacers may be used to avoid this difficulty. The design of span length may also assist in controlling phase spacing. Protection considerations Protection of HPO lines is more complex. Many methods have been proposed, e.g., [2, 3]. One of the main difficulties is the increased number of possible faults, along with the increased range of possible fault current. Operation with loss of a phase For very high phase order circuits, it may be possible to trip only one phase of the HPO circuit, thus allowing all the remaining phases to be sound. With a judicious choice of terminal transformer connections, the impact of operating with one phase out of service may be tolerable. VIII. CONCLUSIONS High phase order with compaction is a potential alternative for overhead transmission. HPO transmission lines have lower phase to phase voltage magnitude. The lower phase to phase voltage allows for compaction of the phases. This compaction increases the mutual coupling in the circuits and decreases the positive sequence reactance, thus increasing the security rating of a transmission line. This paper assesses the increase in security rating for a 6φ line versus a double circuit 3φ line, and a 12φ line versus a quadruple circuit 3φ line. Using a symmetrical conductor configuration results in a symmetrical circulant Toeplitz line reactance matrix. The sequence reactances for 6φ and 12φ lines in terms of self and mutual reactances are calculated. Insight into high phase order calculations using circulant matrices is presented. IX. REFERENCES [1] T. Landers, R. Richeda, E. Krizanskas, J. Stewart, R. Brown. “High phase order economics: constructing a new transmission line,” IEEE Transactions on Power Delivery, Volume 13, Issue 4, 1998. [2] N. Bhatt, S. Venkata, W. Guyker, W. Booth, “Six-phase (multiphase) power transmission systems: Fault analysis,” IEEE Transactions on Power Apparatus and Systems, Volume 96, Issue 3, 1977. [3] E. Badawy, M. El-Sherbiny, A. Ibrahim, M. Farghaly, “A method of analyzing unsymmetrical faults on six-phase power systems,” IEEE Transactions on Power Delivery, Volume 6, Issue 3, 1991. [4] M. Sidik, H. Ahmad, Z. Malek, Z. Buntat, N. Bashir, M. Zarin, Z. Nawawi, M. Jambak, “Induced voltage on objects under six-phase transmission line,” Proc. IEEE Region 10 Conference, Bali, Indonesia, 2011. [5] M. Brown, R. Rebbapragada, T. Dorazio, J. Stewart, “Utility system demonstration of six phase power transmission,” Proc. IEEE Power Engineering Society, Transmission and Distribution Conference, Dallas, TX, 1991. [6] H. C. Barnes, L. O. Barthold, "High phase order power transmission", CIGRE SC 32, Electra, No. 24, 1973. [7] T. Dorazio, “High phase order transmission,” Proc. Southern Tier Technical Conference, Binghamton, NY, 1990. [8] C. Fan, L Liu, Y Tian, “A fault-location method for 12-phase transmission lines based on twelve-sequence-component method,” IEEE Transactions on Power Delivery, Volume 26, Issue 1, 2011. [9] IEEE Standards Association, National Electrical Safety Code, New York, NY, 2012. [10] X. Gong, H. Wang, Z. Zhang, J. Wang, J. Wang, Y. Yuan, “Tests on the first 500 kV compact transmission line in China,” Proc. PowerCon International Conference, Perth, WA, 2000. [11] A. Clerici, G. Valtorta, L. Paris, “AC and/or DC substantial power upgrading of existing OHTL corridors,” Proc. International Conference on AC and DC Power Transmission, London, 1991. [12] R. Gray, Toeplitz and Circulant Matrices: A Review, Foundations and trends in communications and information theory, Now Publishers Inc., Hanover MA, 2006. [13] N. Tesla, My Inventions, the Autobiography of Nikola Tesla, SoHo Books, New York, 2012 [14] A. Augugliaro, L. Dusonchet, A. Spataro, “Mixed three-phase and six-phase power system analysis using symmetrical components method,” Butterworth & Co. (Elsevier Publishers), Amsterdam,1987. [15] William H. Kersting, Distribution System Modeling and Analysis, Taylor & Francis Group, Florida, 2012. [16] E. Klingshirn, “High phase order induction motors,” IEEE Transactions on Power Apparatus and Systems, Volume PAS-102, Issue 1, 1983. X. BIOGRAPHIES Brian Joseph Pierre (StM ‟09) is from Laramie, WY. Mr. Pierre holds the BSEE from Boise State University, Boise, ID (2011). He is presently a doctoral student at Arizona State University, Tempe, AZ. Gerald Thomas Heydt (StM ‟62, M „64, SM ‟80, F ‟91) is from Las Vegas, NV. He holds the Ph.D. in Electrical Engineering from Purdue University. He is a Regents‟ Professor at Arizona State University.