electromagnetic radiation from lightning return strokes to tall structures

The study of the interaction of lightning electromagnetic fields with electrical systems and the design of appropriate protection strategies are generally based on statistical distributions of the lightning current measured at the channel base using either instrumented towers or artificial initiation of lightning using rockets. Recent studies based both on numerical modeling and experimental observations have shown that the presence of the structure struck by (or used to initiate) lightning does affect the current measurement in a way depending upon the geometry of the structure itself, compromising therefore the reliability of the statistics adopted so far for lightning data. The aim of this thesis is to provide new elements (from both theoretical and experimental investigations) to improve the understanding of the electromagnetic consequences of the impact of lightning return strokes to tall structures. Chapter 2 introduces to the phenomenology of cloud-to-ground lightning and the importance of lightning return-stroke modeling. Among the different classes of return-stroke models existing in the literature, the attention is focused in this thesis on the so-called engineering models, which allow describing the current distribution along the channel as a function of the current at the channel base and the return-stroke speed, two quantities for which data can be obtained experimentally. After presenting a review of five engineering return-stroke models describing lightning strikes to ground, the extension of the engineering models to take into account the presence of an elevated strike object is presented and discussed. The original contributions of this thesis, consisting of both theoretical and experimental works, are presented in Chapters 3 through 6. Chapter 3 is devoted to the computation of the electromagnetic field produced by lightning return strokes to elevated strike objects, using the extension of the engineering models to include an elevated strike object presented in the previous chapter. It is shown, for the first time, that the current distribution associated with these extended models exhibits a discontinuity at the return-stroke wavefront which (although not physically conceivable) needs to be taken into account by an additional term in the equations for the electromagnetic field, the so-called "turn-on" term. A general analytical formula describing the "turn-on" term associated with this discontinuity for various engineering models is derived and simulation results illustrating the effect of the "turn-on" term on the radiated electric and magnetic fields are also presented. In the second part of the chapter, dedicated to the investigation of the propagation effects on lightning electromagnetic field traveling along a finitely-conducting ground, the commonly-used assumption of an idealized perfectly-conducting ground is relaxed in order to analyze, for the first time, how the electromagnetic field radiated by a tower-initiated strike is affected while propagating along a soil characterized by a finite conductivity. The results showed that the attenuation of the initial peak of the field radiated by a tower-initiated strike, resulting from the propagation over finitely conducting ground, depends strongly on the risetime of the current, the tower height and the ground conductivity and is, in general, much more important than the attenuation experienced, while propagating along the same finite ground, by the field produced by ground-initiated strikes. Chapter 4 presents a comparison among the predictions obtained using the five extended engineering return-stroke models for lightning strikes to tall structures described in Chapter 2. The spatial-temporal current profiles along the tower-channel axis predicted by the engineering models, as well as the respective predictions for the radiated electric and magnetic fields, calculated at different distances, are compared and discussed. It is shown that the computed electromagnetic fields associated with a strike to a tall tower are generally less model-dependent than those corresponding to a strike to ground, especially as far as the first-peak value is concerned, which is nearly model-insensitive in case of tall-tower strikes. A theoretical analysis is performed in the last part of the chapter with the aim to provide, for the same five engineering models extended to take into account the presence of the tower, expressions relating the return-stroke current and the associated distant radiated electric and magnetic fields. It is demonstrated, in addition, that only one model among the five presented is characterized by simple analytical formulas relating current-peak and far-field peak values, which (being the electromagnetic field peak value nearly independent of the adopted model) become general expressions applicable for any engineering return-stroke model in case of tower-initiated lightning. It was also shown that the peak amplitude of the electromagnetic field radiated by a lightning strike to a tall structure is relatively insensitive to both the values of the top reflection coefficient and the return-stroke speed. This latter result is important, in particular, because, unlike ground-initiated strikes, for which the far-field peak is strongly dependent on the return-stroke speed, far field peaks associated with strikes to tall structures are little sensitive to the return stroke speed. Since in most practical cases the value of the return-stroke speed is unknown, this interesting result suggests a possible calibration procedure for lightning detection systems by means of direct measurement of lightning currents on instrumented towers. Chapter 5 reports on the simultaneous measurements of the return-stroke current and of the electric and magnetic fields at three distances associated with lightning strikes to the Toronto CN Tower (553 m) that have been carried out during the summer of 2005. This is the first time ever that simultaneous records of lightning current and associated electric and magnetic fields at three distances have been obtained. Two propagation paths for the electromagnetic field to the first and to the second field measurement stations (located, respectively, 2.0 km and 16.8 km away from the CN Tower) were along the soil and through the Toronto city, whereas for the third location (50.9 km away) the propagation path was nearly entirely across the fresh water of Lake Ontario. It is shown that the waveforms of the electric and magnetic fields at 16.8 km and 50.9 km exhibit a first zero-crossing about 5 microseconds after the onset of the return-stroke, which is part of a narrow undershoot and which may be attributed to the transient processes along the tower. Effects of propagation (decrease of field amplitude and increase of its risetime) could also be observed in experimental records. It is shown that the fields at 50.9 km are less affected by such attenuation, compared to those at 16.8 km, presumably because the path of propagation was mostly across Lake Ontario. The measured waveforms are compared with the theoretical predictions obtained using five engineering return-stroke models, extended to include the presence of the strike object, finding a reasonable agreement for the magnetic field waveforms at the three considered distances. The overall agreement between the theoretically predicted and the experimentally observed field-peak-to-current-peak ratio is reasonable, although the theoretical expression appears to underestimate the experimentally measured ratio (by about 25 %). This may be due, at least in part, to the enhancement effect of the buildings on which the field measurement antennas were installed. Finally, the directly-measured lightning currents at the tower were correlated and compared with the current-peak estimations provided by the US National Lightning Detection Network (NLDN). It is shown that the NLDN-inferred values overestimate the actual current peaks because the presence of the tall struck object produces an enhanced radiated field at far distances (with respect to strikes to flat ground), which is not included in the algorithm used to infer lightning current peaks from remote field measurements. It is shown in this thesis that correcting the NLDN estimates using the correction factor introduced by the tower results in an excellent estimation of lightning current peaks. This is an important conclusion of this study showing that the estimation of lightning peak currents for tall towers can be greatly improved by considering the tower correction factor. Chapter 6 is devoted to the measurement of electromagnetic fields radiated by lightning. In its first part, the need for guidelines for reporting lightning data obtained experimentally is emphasized. The second part of the chapter presents the design, the construction and preliminary tests of a low-cost, multi-channel lightning field measuring system for the simultaneous measurement of three components of the electromagnetic field radiated by lightning. The proposed system uses one single optical link for the transmission of the three signals, appropriately digitized and multiplexed, lowering considerably the overall cost of the system itself.

[1]  Vladimir A. Rakov,et al.  On different approaches to calculating lightning electric fields , 2001 .

[2]  Kenji Matsuura,et al.  Luminous propagation of lightning attachment to CN tower , 1995 .

[3]  James L. Drewniak,et al.  IEEE International Symposium on Electromagnetic Compatibility , 1994 .

[4]  Farhad Rachidi,et al.  Estimation of Lightning-Caused Stresses in A MV Distribution Line Using A Three-Wire Approach , 2006 .

[5]  D. M. Le Vine,et al.  Comment on the transmission‐line model for computing radiation from lightning , 1992 .

[6]  Farhad Rachidi,et al.  Extension of two return stroke models to consider the influence of elevated strike objects on the lightning return stroke current and the radiated electromagnetic field: comparison with experimental results , 1996 .

[7]  Martin A. Uman,et al.  A remote sensor for the three components of transient electric fields , 1988 .

[8]  F. Rachidi,et al.  Influence of the height of an elevated strike object on the enhancement of lightning radiated fields , 2003, 2003 IEEE Bologna Power Tech Conference Proceedings,.

[9]  Vernon Cooray,et al.  Propagation effects on the lightning-generated electromagnetic fields for homogeneous and mixed sea-land paths , 1994 .

[10]  Wasyl Janischewskyj,et al.  Electromagnetic field radiation model for lightning strokes to tall structures , 1996 .

[11]  F. Rachidia,et al.  Return stroke current profiles and electromagnetic fields associated with lightning strikes to tall towers : Comparison of engineering models , 2007 .

[12]  Martin A. Uman,et al.  Methods for calculating the electromagnetic fields from a known source distribution: application to lightning , 1989 .

[13]  Farhad Rachidi,et al.  Simultaneous Measurements of Electromagnetic Fields at two Distances and of Current Associated with Lightning Return Strokes to the CN Tower , 2002 .

[14]  Y. Baba,et al.  On the interpretation of ground reflections observed in small-scale experiments Simulating lightning strikes to towers , 2005, IEEE Transactions on Electromagnetic Compatibility.

[15]  Vladimir A. Rakov,et al.  Treatment of retardation effects in calculating the radiated electromagnetic fields from the lightning discharge , 1998 .

[16]  V. Rakov,et al.  Distribution of charge along the lightning channel : Relation to remote electric and magnetic fields and to return-stroke models , 1997 .

[17]  Farhad Rachidi,et al.  Current and electromagnetic field associated with lightning-return strokes to tall towers , 2001 .

[18]  M. Uman Lightning return stroke electric and magnetic fields , 1985 .

[19]  M. Uman,et al.  Lightning return stroke current models with specified channel‐base current: A review and comparison , 1990 .

[20]  Wei Guanghui,et al.  Effects of propagation on the return stroke radiation fields , 2002, 2002 3rd International Symposium on Electromagnetic Compatibility.

[21]  Vladimir A. Rakov,et al.  Analytical Representation of Lightning Current Waveforms using Genetic Algorithms , 2004 .

[22]  Wasyl Janischewskyj,et al.  Expanding the modified transmission line model to account for reflections within the continuously growing lightning return stroke channel , 2000, 2000 Power Engineering Society Summer Meeting (Cat. No.00CH37134).

[23]  E. Krider,et al.  Broadband antenna systems for lightning magnetic fields , 1975 .

[24]  F. Rachidi,et al.  Far-field-current relationship based on the TL model for lightning return strokes to elevated strike objects , 2005, IEEE Transactions on Electromagnetic Compatibility.

[25]  Kenneth L. Cummins,et al.  The U.S. National Lightning Detection NetworkTM and Applications of Cloud-to-Ground Lightning Data by Electric Power Utilities , 1998 .

[26]  Yoshihiro Baba,et al.  Lightning electromagnetic environment in the presence of a tall grounded strike object , 2005 .

[27]  Farhad Rachidi,et al.  The Effect of the Measurement Time Constant of Analog Integrators on the Resulting Modeling and Simulation of Lightning , 2004 .

[28]  J. R. Grant,et al.  Characterization of Lightning Return Stroke Electric and Magnetic Fields From Simultaneous Two- Station Measurements (Paper 9C0949) , 1979 .

[29]  Vladimir A. Rakov,et al.  On the Constraints Imposed by the Close Electric Field Signature on the Equivalent Corona Current in Lightning Return Stroke Models , 2004 .

[30]  Martin A. Uman,et al.  Transient electric and magnetic fields associated with establishing a finite electrostatic dipole, revisited , 1991 .

[31]  M. Ianoz,et al.  On lightning return stroke models for LEMP calculations , 1988 .

[32]  James R. Wait,et al.  Propagation effects for electromagnetic pulse transmission , 1986, Proceedings of the IEEE.

[33]  Vernon Cooray,et al.  Effects of propagation on the rise times and the initial peaks of radiation fields from return strokes , 1983 .

[34]  M. Uman,et al.  Magnetic field of lightning return stroke , 1969 .

[35]  Farhad Rachidi,et al.  Tall structure lightning return stroke velocity measurements for 553 m AGL CN telecommunication tower , 2005 .

[36]  D. A. Ward,et al.  Using Rogowski coils for transient current measurements , 1993 .

[37]  Vladimir A. Rakov,et al.  On the computation of electric fields from a lightning discharge in time domain , 2001, 2001 IEEE EMC International Symposium. Symposium Record. International Symposium on Electromagnetic Compatibility (Cat. No.01CH37161).

[38]  J. L. Bermudeza,et al.  Determination of lightning currents from far electromagnetic fields : Effect of a strike object , 2007 .

[39]  Vladimir A. Rakov,et al.  Effect of vertically extended strike object on the distribution of current along the lightning channel , 2002 .

[40]  S. Moreland The Lightning Discharge , 1890, Nature.

[41]  Farhad Rachidi,et al.  On the calculation of Electromagnetic Fields Radiated by Lightning to Tall Structures , 2004 .

[42]  James R. Wait Transient Fields of a Vertical Dipole Over a Homogeneous Curved Ground , 1956 .

[43]  Farhad Rachidi,et al.  Determination of reflection coefficients at the top and bottom of elevated strike objects struck by lightning , 2003 .

[44]  Farhad Rachidi,et al.  Influence of the finite ground conductivity on the transient response to lightning of a tower and its grounding , 2005 .

[45]  Farhad Rachidi,et al.  Electromagnetic environment in the immediate vicinity of a tower struck by lightning , 2004 .

[46]  Carl Baum,et al.  The Measurement of Lightning Environmental Parameters Related to Interaction with Electronic Systems , 1982, IEEE Transactions on Electromagnetic Compatibility.

[47]  Farhad Rachidi,et al.  Electromagnetic field radiated by lightning to tall towers: treatment of the discontinuity at the return stroke wave front , 2004 .

[48]  Farhad Rachidi,et al.  On return stroke currents and remote electromagnetic fields associated with lightning strikes to tall structures. 1. Computational models , 2007 .

[49]  E. Petrache,et al.  Lightning strikes to elevated structures: influence grounding conditions on currents and electromagnetic fields , 2005, 2005 International Symposium on Electromagnetic Compatibility, 2005. EMC 2005..

[50]  Gerhard Diendorfer,et al.  On The Effect of The Finite Ground Conductivity on Electromagnetic Field Radiated by Lightning to Tall Towers , 2006 .

[51]  M. Ianoz,et al.  Modified Transmission Line model for LEMP calculations. Effect of the return stroke velocity decreasing and elevated strike object on close fields , 1992 .

[52]  N. Plooster,et al.  Shock Waves From Line Sources , 1968 .

[53]  Farhad Rachidi,et al.  On the Master, Uman, Lin, Standler and the Modified Transmission Line Lightning return stroke current models , 1990 .

[54]  Farhad Rachidi,et al.  On the need for unified criteria describing the quality of lightning data and the design of a lightning field measurement system , 2005 .

[55]  José-Luis Bermudez Arboleda,et al.  Lightning currents and electromagnetic fields associated with return strokes to elevated strike objects , 2003 .

[56]  Farhad Rachidi,et al.  On the influence of elevated strike objects on directly measured and indirectly estimated lightning currents , 1998 .

[57]  C. Nucci,et al.  On return stroke currents and remote electromagnetic fields associated with lightning strikes to tall structures: 2. Experiment and model validation , 2007 .

[58]  N. Herodotou,et al.  Distribution of lightning peak stroke currents in Ontario using an LLP system , 1993 .

[59]  Martin A. Uman,et al.  Return stroke transmission line model for stroke speed near and equal that of light , 2001 .

[60]  Vladimir A. Rakov,et al.  Review and evaluation of lightning return stroke models including some aspects of their application , 1998 .

[61]  Farhad Rachidi,et al.  Measuring System Specially Designed for Lightning Electromagnetic Fields , 2006 .

[62]  S.H.H. Sadeghi,et al.  The effects of tall buildings on the measurement of electromagnetic fields due to lightning return strokes , 2001, 2001 IEEE EMC International Symposium. Symposium Record. International Symposium on Electromagnetic Compatibility (Cat. No.01CH37161).

[63]  Farhad Rachidi,et al.  Currents and radiated electromagnetic fields in lightning strikes to tall structures , 2003 .

[64]  Farhad Rachidi,et al.  Engineering lightning return stroke models including an elevated strike object: far field-current relationship , 2004 .

[65]  Farhad Rachidi,et al.  Propagation effects on the electromagnetic field radiated by lightning to tall towers , 2005 .

[66]  M. Uman,et al.  The electromagnetic radiation from a finite antenna , 1975 .

[67]  Farhad Rachidi,et al.  On the enhancement of electric and magnetic fields from lightning due to close-by metallic structures , 2004 .

[68]  W. K. Brasher,et al.  Journal of the Institution of Electrical Engineers , 1941, Nature.

[69]  Gerhard Diendorfer,et al.  Lightning characteristics based on data from the Austrian lightning locating system , 1998 .

[70]  K. Norton The Propagation of Radio Waves over the Surface of the Earth and in the Upper Atmosphere , 1936, Proceedings of the Institute of Radio Engineers.

[71]  Farhad Rachidi,et al.  Simultaneous Measurements of Return Stroke Current, Electric and Magnetic Fields at Three Distance Ranges Associated with Lightning Strikes to The CN Tower , 2006 .

[72]  Farhad Rachidi,et al.  Determination of lightning currents from far electromagnetic fields , 1993 .

[73]  Martin A. Uman,et al.  On the radiation field turn‐on term associated with traveling current discontinuities in lightning , 1990 .

[74]  Vladimir A. Rakov,et al.  Return stroke current profiles and electromagnetic fields associated with lightning strikes to tall towers: Comparison of engineering models , 2007 .

[75]  Gerhard Diendorfer,et al.  Evaluation of lightning location data employing measurements of direct strikes to a radio tower , 2002 .