Electrical and Electronic Engineering
p-ISSN: 2162-9455 e-ISSN: 2162-8459
2013; 3(2): 49-71
doi:10.5923/j.eee.20130302.04
Funso K. ARIYO, Micheal O. Omoigui
Department of Electronic and Electrical Engineering, Obafemi Awolowo University, Ile-Ife, Nigeria
Correspondence to: Funso K. ARIYO, Department of Electronic and Electrical Engineering, Obafemi Awolowo University, Ile-Ife, Nigeria.
| Email: | ![]() |
Copyright © 2012 Scientific & Academic Publishing. All Rights Reserved.
The first part of this paper presents the basic analyses carried out on Nigerian 330 kV electrical network with distributed generation (DG) penetration. The analyses include load flow, short circuit, transient stability, modal/eigenvalues calculation and harmonics. The proposed network is an expanded network of the present network incorporating wind, solar and small-hydro sources. The choice of some locations of distributed generation has been proposed by energy commission of Nigeria (ECN). The conventional sources and distributed generation were modeled using a calculation program called PowerFactory, written by DIgSILENT.
Keywords: Distributed generation, load flow, short-circuit, transient stability, modal analysis, eigenvalues calculation, harmonics analysis, PowerFactory, DIgSILENT
Cite this paper: Funso K. ARIYO, Micheal O. Omoigui, Investigation of Nigerian 330 kV Electrical Network with Distributed Generation Penetration – Part I: Basic Analyses, Electrical and Electronic Engineering, Vol. 3 No. 2, 2013, pp. 49-71. doi: 10.5923/j.eee.20130302.04.
![]() | Figure 1. Proposed Nigerian 330 kV electrical network (37-bus system) |
used is 100 MVA, while the transmission line lengths (in Kilometers, Km) were per-unitized on the base value of 100 Km.![]() | (1) |
is the terminal voltage of the ith generator; and
and
are the generator real and reactive powers.For n-bus system, the node-voltage equation in matrix form is:![]() | (2) |
![]() | (3) |
is the vector of the injected bus currents and
is the vector of bus voltages measured from the reference node.
is known as the bus admittance matrix. The diagonal element of each node is the sum of admittances connected to it. It is known as self-admittance given as:![]() | (4) |
![]() | (5) |
of the nodes, and the active (P) and reactive (Q) power flow on branches. The network nodes are represented by specifying two of these four quantities. PowerFactory uses the Newton-Raphson (power equation, classical) method as its non-linear equation solver. This method is used for large transmission systems, especially when heavily loaded. It was used for A.C. load flow.From Kirchhoff’s Current law (KCL), the current at bus I is given by [7]:![]() | (6) |
![]() | (7) |
![]() | (8) |
![]() | (9) |
![]() | (10) |
and
, the voltage and phase angle for each bus are computed iteratively using:![]() | (11) |
and
are calculated from Jacobian matrix. The results of the analysis are shown and discussed in section 9.![]() | (12) |

The period and damping of this mode are given by:![]() | (13) |
![]() | (14) |
and
are amplitudes of two consecutive swing maxima or minima respectively.The oscillatory periods of local generator oscillations are typically in the range of 0.5 to 5 Hz. Higher frequencies of the natural oscillations, that is, those which are normally not regulated out, are often damped to a greater extent than slower oscillations. The oscillatory period of the oscillations of areas (inter-area oscillations) is normally a factor of 5 to 20 times greater than that of the local generator oscillations [14].The absolute contribution of an individual generator to the oscillation mode which has been excited as a result of a disturbance can be calculated by:The nomenclature is given in Appendix.‘c’ is set to the unit vector, that is, c = [1, ...,1], which corresponds to a theoretical disturbance which would equally excite all generators with all natural resonance frequencies simultaneously. The elements of the eigenvectors
then represents the mode shape of the eigenvalue i and shows the relative activity of a state variable, when a particular mode is excited. They show for example, the speed amplitudes of the generators when an eigenfrequency is excited, whereby those generators with opposite signs in
oscillate in opposite phase. The right eigenvectors
can thus be termed the "observability vectors''. The left eigenvectors
measures the activity of a state variable x in the i-th mode, thus the left eigenvectors can be termed the "relative contribution vectors''. Normalization is performed by assigning the generator with the greatest amplitude contribution the relative contribution factor 1 or -1 respectively. For n-machine power system, n-1 generator oscillation modes will exist and n-1 conjugate complex pairs of eigenvalues
will be found. The mechanical speed
of the n generators will then be described by [14]:![]() | (15) |
and
are combined to a matrix P of participation factor by:![]() | (16) |
are called the participation factors. They give a good indication of the general system dynamic oscillation pattern. They may be used easily to determine the location of eventually needed stabilizing devices in order to influence the system damping efficiently. Furthermore the participation factor is normalized so that the sum for any mode is equal to 1[21, 22].
|
|
|
used was 100 MVA, while the transmission line lengths (in Kilometers, Km) were per-unitized on the base value of 100 Km.Detailed reports can be provided in the ‘output of results-complete system report’ icon provided by the software.Secondly, short-circuit calculation was carried out on transmission line connecting F.C.T. and Niger generating stations.
|
|
|
![]() | Figure 2. Total apparent power (MVA) |
![]() | Figure 3. Turbine power (p.u.) |
![]() | Figure 4. Total power factor |
![]() | Figure 5. Total active power (MW) |
![]() | Figure 6. Speed (p.u.) |
![]() | Figure 7. Mechanical torque (p.u.) |
![]() | Figure 8. Benue hydro generating station parameters |
![]() | Figure 9. Eigenvalue plot – QR method |
![]() | Figure 10. Eigenvalue plot - selective method |
![]() | Figure 11. Mode bar plot - controllability |
![]() | Figure 12. Mode bar plot - observability |
![]() | Figure 13. Mode bar plot - participation factor |
![]() | Figure 14. Mode phasor plot - controllability (0,0 origin) |
![]() | Figure 15. Mode phasor plot - observability (0,0 origin) |
![]() | Figure 16. Mode phasor plot - participation factor |
![]() | Figure 17. Balanced network - harmonic distortion, A |
![]() | Figure 18. Balanced network - positive-sequence current, A |
![]() | Figure 19. Balanced network - current diversity factor |
![]() | Figure 20. Balanced network - voltage diversity factor |
![]() | Figure 21. Unbalanced network - harmonic distortion |
![]() | Figure 22. Unbalanced network-positive-sequence current, A |
![]() | Figure 23. Unbalanced network - current diversity factor |
![]() | Figure 24. Unbalanced network - voltage diversity factor |
![]() | Figure 25. Frequency sweep - current diversity factor |
![]() | Figure 26. Frequency sweep - harmonic distortion (current) |
![]() | Figure 27. Frequency sweep - positive-sequence current |
![]() | Figure 28. Frequency sweep - voltage diversity factor |
peak current;
breaking current (RMS value);
peak short-circuit breaking current;
initial symmetrical short-circuit current;
peak breaking apparent power;
decaying d.c. component;
thermal current;
load current;
initial short-circuit current;
factor for the calculation of
;
factor for the heat effect of the d.c. component
factor for the heat effect of the a.c. component;
are nominal conditions.
generator speed vector
ith eigenvalue
ith right eigenvector
magnitude of excitation of the ith mode (at t=0);n number of conjugate complex eigenvalues PARAMETERS USED FOR POWERFACTORY ANALYSIS(ⅰ) Wind generator data (output = 50 MW):Static generator (wind) ratings = 3MVA; active power = 2MW; power factor = 0.95; terminal voltage = 0.69kV; number of generators = 25; (ⅱ) Solar generator data (output = 50 MW):Static generator (solar) ratings = 0.6MVA; active power = 0.5MW; power factor = 0.95; terminal voltage = 0.4kV; number of generators = 100; (ⅲ) Synchronous generator controllers data:• PSS:
• AVR:
• Turbine and governor: 
| [1] | Sambo A. S., Garba B., I. H. Zarma and M. M. Gaji, “Electricity Generation and the Present Challenges in the Nigerian Power Sector”, Unpublished Paper, Energy Commission of Nigeria, Abuja-Nigeria, 2010. |
| [2] | www.google.com/publicdata. |
| [3] | ThisDay Newspaper, 3rd October, 2011. |
| [4] | www.energy.gov.ng. |
| [5] | Magazine article; African Business, No. 323, August-September 2006. |
| [6] | Ileoje, O.C., “Potentials for Renewable Energy Application in Nigeria, Energy Commission of Nigeria”, pp 5-16, 1997. |
| [7] | Fagbenle R.L., T.G. Karayiannis, “On the wind energy resource of Nigeria”, International Journal of Energy Research. Number 18, pp 493-508, 1994. |
| [8] | Okoro, O.I. and Madueme, T.C.: “Solar energy investments in a developing economy”,Renewable Energy 29, 2004, pp. 1599-1610. |
| [9] | Garba,B and Bashir, A. M (2002). Managing Energy Resources in Nigeria: Studies on Energy Consumption Pattern in Selected Areas in Sokoto State. Nigerian Journal of Renewable Energy, Vol. 10 Nos. 1&2, pp. 97-107. |
| [10] | M. S. Adaramola and O. M. Oyewola, ‘Wind Speed Distribution and Characteristics in Nigeria’, ARPN Journal of Engineering and Applied Sciences, VOL. 6, NO. 2, FEBRUARY 2011. |
| [11] | Gonzalez-Longatt F.M., ‘Impact of Distributed generation over Power Losses on Distributed System’, 9th International Conference, Electrical Power Quality and Utilization, Barcelona, 9-11 October, 2007. |
| [12] | M. Begović, A. Pregelj, A. Rohatgi, ‘Impact of Renewable Distributed Generation on Power Systems’, Proceedings of the 34th Hawaii International Conference on System Sciences, 2001. |
| [13] | Mohamed El Chehaly ‘Power System Stability Analysis with a High Penetration of Distributed Generation’, Unpublished M.Sc. Thesis, McGill University, Montréal, Québec, Canada, February 2010. |
| [14] | DIgSILENT PowerFactory Version 14.1 Tutorial, DIgSILENT GmbH Heinrich-Hertz-StraBe 9, 72810 Gomaringen, Germany, May, 2011. |
| [15] | Saadat H., “Power System Analysis”, McGraw- Hill International Editions, 1999. |
| [16] | http://webstore.iec.ch/preview/info_iec60909-0%7 Bed1.0%7Den_d.pdf |
| [17] | Serrican A.C., Ozdemir A., Kaypmaz A., ‘Short Circuit Analyzes Of Power System of PETKIM Petrochemical Aliaga Complex’, The Online Journal on Electronics and Electrical Engineering (OJEEE), Vol. (2) – No. (4), pp 336-340, Reference Number: W10-0037. |
| [18] | Patel J.S. and Sinha M.N.‘Power System Transient Stability Analysis using ETAP Software’, National Conference on Recent Trends in Engineering & Technology, 13-14 May 2011. |
| [19] | Iyambo P.K., Tzonova R., ‘Transient Stability Analysis of the IEEE 14-Bus Electrical Power System’, IEEE Conf. 2007. |
| [20] | Dashti R. and Ranjbar B, ‘Transient Analysis of Induction Generator Jointed to Network at Balanced and Unbalanced Short Circuit Faults’, ARPN Journal of Engineering and Applied Sciences, Vol. 3, No. 3, June 2008. |
| [21] | Kundur P. ‘Power System Stability and Contrl’, The EPRI Power System Engineering Series, McGraw-Hill, 1994. |
| [22] | Kumar G.N., Kalavathi M.S. and Reddy B.R. Eigen Value Techniques for Small Signal Stability Analysis in Power System Stability’, Journal of Theoretical and Applied Information Technology, 2005 – 2009. |
| [23] | IEEE Recommended Practices and Requirements for Harmonic Control in Electrical Power Systems, IEEE Std. 519-1992, 1993. |
| [24] | Manmek T., Grantham C. and Phung T. ‘A Real Time Power Harmonics Measuring Technique under Noisy Conditions’, Australasian Universities Power Engineering Conference, Brisbane, Australia, 26th-29th September 2004 |