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An Experimental Study of Ion Motion
Optimization for Constraint Economic Load
Dispatch Problem
• Presented By: Mohit Kumar
• Department of Electrical and Instrumentation engineering,
Sant Longowal Institute of Engineering and Technology
• Longowal, Sangrur, India
Table of Content
1. Introduction
3. Motivation for the Proposed Work
4. Modeling of the problem
5. Ion Motion Optimization
6. Result Analysis
7. Conclusion
8. References
1. Introduction
Economic Load dispatch in power systems is an
important, real world optimization problem that
has minimization of generation cost as its
objective.
Solving the Economic Load dispatch Problem has
been attempted from the early 1970's [1].
These early attempts employed classical, gradient
based techniques such as lambda-iteration
method, gradient method and dynamic
programming [2].
Cont’d
However, gradient based methods require that
the function to be optimized be differentiable,
continuous and convex to successfully locate the
global optimum.
The Economic Load Dispatch problem has to
satisfy a number of constraints including the
presence of prohibited operating zones, valve
point loading effect, and ramp rate constraints,
which make the problem a non-convex and
discontinuous one.
Cont’d
Cont’d
Cont’d
These complicating factors also led to a huge
interest in gradient free, evolutionary
computation or metaheuristic methods of
optimization being employed to solve the
Economic Load Dispatch problem.
Some meta-heuristic methods employed to solve
EcLD problems are Evolutionary programming
(EP) [2], Shuffled differential evolution (SDE) [3],
effective Lightning Flash Algorithm (LFA) [4] and
enhanced particle swarm optimization
(Enhanced-PSO) [5].
2.Motivation for the Proposed Work
Problem Solving Tools applied to solve selected power system
problems
Classical/Traditional Techniques Metaheuristic/Soft-computing
Techniques
Lambda-iteration method
 Gradient method
Dynamic programming
Branch and bound method
 Linear Programming
Improved Lambda-iteration
method, etc.
 Genetic Algorithm and its
variants
Particle swarm optimization
and its variants
Differential evolution and its
variants
Harmony search algorithm
and its variants, etc.
Cont’d
But none of above can claim to be the best
problem solving tool because each technique
has its own limitations, advantages and
disadvantages.
For example:
 Traditional methods are only applicable for
the problems which have continuous
differentiable objective function.
Cont’d
 The tuning of genetic algorithm parameters in
complex search spaces is difficult.
 Premature convergence of genetic algorithm
reduces its performance and search capability.
 An evolutionary computation technique,
known as particle swarm optimization, has
become a candidate for many optimization
applications due to its high performance and
flexibility but is not self adaptive.
4.Modeling of the problem
• 𝐹𝑖 𝑥𝑖 = 𝑎𝑖 𝑥𝑖
2
+ 𝑏𝑖 𝑥𝑖 + 𝑐𝑖 + 𝑒𝑖 × sin 𝑓𝑖(𝑥𝑖
𝑚𝑖𝑛
− 𝑥𝑖)
• 𝐹 𝑇 = 𝑖=1
𝑁𝑣
𝐹𝑖(𝑥𝑖)
• 𝑖=1
𝑁𝑣
𝑥𝑖 − 𝑃𝐿 − 𝑃 𝐷 = 0
• 𝑥𝑖
𝑚𝑖𝑛
≤ 𝑥𝑖 ≤ 𝑥𝑖
𝑚𝑎𝑥
𝑖 = 1,2, … , 𝑁𝑣
• 𝑃𝐿 = 𝐵00 + 𝑖=1
𝑁 𝑉
𝐵0𝑖 𝑥𝑖 + 𝑖=1
𝑁 𝑉
𝑗=1
𝑁 𝑉
𝑥𝑖 𝐵𝑖𝑗 𝑥𝑗
• 𝐹𝑇 =
𝐹𝑇 ; 𝑥𝑖 ∈ 𝐹𝑅
𝐹𝑇 + 𝑟 𝑖=1
𝑁
𝑥𝑖 − 𝑥 𝐿 − 𝑥 𝐷
2
; 𝑜𝑡ℎ𝑒𝑟𝑤𝑖𝑠𝑒
ION MOTION OPTIMIZATION
Cation
Anion
Best Cation
Best Anion
Cont’d
• 𝑥𝑗𝑖 = 𝑥𝑖
𝑚𝑖𝑛
+ 𝑟𝑎𝑛𝑑 𝑗, 𝑖 𝑥𝑖
𝑚𝑎𝑥
− 𝑥𝑖
𝑚𝑖𝑛
• 𝐴𝑗𝑖 = 𝑥𝑗𝑖 ; 𝑖 = 1,2, … , 𝑁𝑣; 𝑗 = 1,2, … , 0.5𝑁𝑝
• 𝐶𝑗𝑖 = 𝑥𝑗𝑖 ; 𝑖 = 1,2, … , 𝑁𝑣; 𝑗 = 0.5𝑁𝑝 + 1, 0.5𝑁𝑝 + 2, … , 𝑁𝑝
• 𝐴𝑗𝑖
𝐹
=
1
1+𝑒𝑥𝑝
(−
0.1
𝐴 𝑗𝑖
𝐷)
• 𝐴𝑗𝑖
𝐷
= 𝐴𝑗𝑖 − 𝐶𝑖
𝑏𝑒𝑠𝑡
• 𝐶𝑗𝑖
𝐹
=
1
1+𝑒𝑥𝑝
−
0.1
𝐶 𝑗𝑖
𝐷
• 𝐶𝑗𝑖
𝐷
= 𝐶𝑗𝑖 − 𝐴𝑖
𝑏𝑒𝑠𝑡
Cation
Anion
Best Cation
Best Anion
Cont’d
• 𝐶𝑗𝑖
𝑛𝑒𝑤
= 𝐶𝑗𝑖 + 𝐶𝑗𝑖
𝐹
𝐴𝑖
𝑏𝑒𝑠𝑡
− 𝐶𝑗𝑖
• 𝐴𝑗𝑖
𝑛𝑒𝑤
= 𝐴𝑗𝑖 + 𝐴𝑗𝑖
𝐹
𝐶𝑖
𝑏𝑒𝑠𝑡
− 𝐴𝑗𝑖
Cation
Anion
Best Cation
Best Anion
Cont’d
• 𝐶𝑗𝑖
𝑛𝑒𝑤
=
𝐶𝑗𝑖 + 𝜑1 𝐴𝑖
𝑏𝑒𝑠𝑡
− 1 ; z𝑗𝑖 > 0.5
𝐶𝑗𝑖 + 𝜑1 𝐴𝑖
𝑏𝑒𝑠𝑡
; z𝑗𝑖 < 0.5 𝑎𝑛𝑑 z𝑗𝑖 > 0.05
𝑥𝑖
𝑚𝑖𝑛
+ z𝑗𝑖 (𝑥𝑖
𝑚𝑎𝑥
−𝑥𝑖
𝑚𝑖𝑛
) ; z𝑗𝑖 < 0.05
• 𝐴𝑗𝑖
𝑛𝑒𝑤
=
𝐴𝑗𝑖 + 𝜑2 𝐶𝑖
𝑏𝑒𝑠𝑡
− 1 ; z𝑗𝑖 > 0.5
𝐴𝑗𝑖 + 𝜑2 𝐶𝑖
𝑏𝑒𝑠𝑡
; z𝑗𝑖 < 0.5 𝑎𝑛𝑑 z𝑗𝑖 > 0.05
𝑥𝑖
𝑚𝑖𝑛
+ z𝑗𝑖 (𝑥𝑖
𝑚𝑎𝑥
−𝑥𝑖
𝑚𝑖𝑛
) ; z𝑗𝑖 < 0.05
Result Analysis
Generator Number Power output (MW)
𝒙 𝟏
∗
(𝐌𝐖) 629.0191
𝒙 𝟐
∗
(𝐌𝐖) 299.4592
𝒙 𝟑
∗
(𝐌𝐖) 297.7103
𝒙 𝟒
∗
(𝐌𝐖) 60.0
𝒙 𝟓
∗
(𝐌𝐖) 60.0
𝒙 𝟔
∗
(𝐌𝐖) 60.0
𝒙 𝟕
∗
(𝐌𝐖) 60.0
𝒙 𝟖
∗
(𝐌𝐖) 60.00001
𝒙 𝟗
∗
(𝐌𝐖) 109.9108
𝒙 𝟏𝟎
∗
(𝐌𝐖) 40.0
𝒙 𝟏𝟏
∗
(𝐌𝐖) 40.00003
𝒙 𝟏𝟐
∗
(𝐌𝐖) 55.0
𝒙 𝟏𝟑
∗
(𝐌𝐖) 55.0
Loss (𝑷 𝑳) (𝐌𝐖) 26.09937
Minimum cost (𝑭 𝑻) ₹ /𝒉 18205.670
Average cost ₹/𝒉 18371.92733
Maximum cost ₹/ 18485.020
Standard deviation (SD) 76.844125
Cont’d
1.832358E+04
1.842358E+04
1.852358E+04
1.862358E+04
1.872358E+04
1.882358E+04
1.892358E+04
0 100 200 300 400 500 600 700
Fuelcost(₹/hr)
Iteration
13 Generator problem with loss
(@ PD=1800MW)
Conclusion
 In this paper IMO algorithm is
presented and applied on real world
economic load dispatch.
 The algorithm performance is very good
and it may be the good optimization
technique for many other engineering
optimization problems.
 A future study may be directed towards
inclusion of chaotic maps in IMO
algorithm.
References
1. Dhillon JS, Kothari DP. Power system optimization. Prentice Hall of India
Private Limited. 2010.
2. Sinha N, Chakrabarti R and Chattopadhyay PK, “Evolutionary
programming techniques for economic load dispatch”, IEEE Transactions
on evolutionary computation, vol. 7(1), pp.83-94, 2013
3. A. S. Reddy and K. Vaisakh, “Shuffled differential evolution for large scale
economic dispatch,” Electr. Power Syst. Res., vol. 96, pp. 237–245, 2013.
4. M. Kheshti, X. Kang, Z. Bie, Z. Jiao, and X. Wang, “An effective Lightning
Flash Algorithm solution to large scale non-convex economic dispatch
with valve-point and multiple fuel options on generation units,” Energy,
vol. 129, pp. 1–15, 2017.
5. Q. Qin, S. Cheng, X. Chu, X. Lei, and Y. Shi, “Solving non-convex / non-
smooth economic load dispatch problems via an enhanced particle swarm
optimization,” Appl. Soft Comput. J., vol. 59, pp. 229–242, 2017.
6. B. Javidy, A. Hatamlou, and S. Mirjalili, “Ions motion algorithm for solving
optimization problems,” Appl. Soft Comput. J., vol. 32, pp. 72–79, 2015
An Experimental Study of Ion Motion Optimization for Constraint Economic Load Dispatch Problem

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An Experimental Study of Ion Motion Optimization for Constraint Economic Load Dispatch Problem

  • 1. An Experimental Study of Ion Motion Optimization for Constraint Economic Load Dispatch Problem • Presented By: Mohit Kumar • Department of Electrical and Instrumentation engineering, Sant Longowal Institute of Engineering and Technology • Longowal, Sangrur, India
  • 2. Table of Content 1. Introduction 3. Motivation for the Proposed Work 4. Modeling of the problem 5. Ion Motion Optimization 6. Result Analysis 7. Conclusion 8. References
  • 3. 1. Introduction Economic Load dispatch in power systems is an important, real world optimization problem that has minimization of generation cost as its objective. Solving the Economic Load dispatch Problem has been attempted from the early 1970's [1]. These early attempts employed classical, gradient based techniques such as lambda-iteration method, gradient method and dynamic programming [2].
  • 4. Cont’d However, gradient based methods require that the function to be optimized be differentiable, continuous and convex to successfully locate the global optimum. The Economic Load Dispatch problem has to satisfy a number of constraints including the presence of prohibited operating zones, valve point loading effect, and ramp rate constraints, which make the problem a non-convex and discontinuous one.
  • 7. Cont’d These complicating factors also led to a huge interest in gradient free, evolutionary computation or metaheuristic methods of optimization being employed to solve the Economic Load Dispatch problem. Some meta-heuristic methods employed to solve EcLD problems are Evolutionary programming (EP) [2], Shuffled differential evolution (SDE) [3], effective Lightning Flash Algorithm (LFA) [4] and enhanced particle swarm optimization (Enhanced-PSO) [5].
  • 8. 2.Motivation for the Proposed Work Problem Solving Tools applied to solve selected power system problems Classical/Traditional Techniques Metaheuristic/Soft-computing Techniques Lambda-iteration method  Gradient method Dynamic programming Branch and bound method  Linear Programming Improved Lambda-iteration method, etc.  Genetic Algorithm and its variants Particle swarm optimization and its variants Differential evolution and its variants Harmony search algorithm and its variants, etc.
  • 9. Cont’d But none of above can claim to be the best problem solving tool because each technique has its own limitations, advantages and disadvantages. For example:  Traditional methods are only applicable for the problems which have continuous differentiable objective function.
  • 10. Cont’d  The tuning of genetic algorithm parameters in complex search spaces is difficult.  Premature convergence of genetic algorithm reduces its performance and search capability.  An evolutionary computation technique, known as particle swarm optimization, has become a candidate for many optimization applications due to its high performance and flexibility but is not self adaptive.
  • 11. 4.Modeling of the problem • 𝐹𝑖 𝑥𝑖 = 𝑎𝑖 𝑥𝑖 2 + 𝑏𝑖 𝑥𝑖 + 𝑐𝑖 + 𝑒𝑖 × sin 𝑓𝑖(𝑥𝑖 𝑚𝑖𝑛 − 𝑥𝑖) • 𝐹 𝑇 = 𝑖=1 𝑁𝑣 𝐹𝑖(𝑥𝑖) • 𝑖=1 𝑁𝑣 𝑥𝑖 − 𝑃𝐿 − 𝑃 𝐷 = 0 • 𝑥𝑖 𝑚𝑖𝑛 ≤ 𝑥𝑖 ≤ 𝑥𝑖 𝑚𝑎𝑥 𝑖 = 1,2, … , 𝑁𝑣 • 𝑃𝐿 = 𝐵00 + 𝑖=1 𝑁 𝑉 𝐵0𝑖 𝑥𝑖 + 𝑖=1 𝑁 𝑉 𝑗=1 𝑁 𝑉 𝑥𝑖 𝐵𝑖𝑗 𝑥𝑗 • 𝐹𝑇 = 𝐹𝑇 ; 𝑥𝑖 ∈ 𝐹𝑅 𝐹𝑇 + 𝑟 𝑖=1 𝑁 𝑥𝑖 − 𝑥 𝐿 − 𝑥 𝐷 2 ; 𝑜𝑡ℎ𝑒𝑟𝑤𝑖𝑠𝑒
  • 13. Cont’d • 𝑥𝑗𝑖 = 𝑥𝑖 𝑚𝑖𝑛 + 𝑟𝑎𝑛𝑑 𝑗, 𝑖 𝑥𝑖 𝑚𝑎𝑥 − 𝑥𝑖 𝑚𝑖𝑛 • 𝐴𝑗𝑖 = 𝑥𝑗𝑖 ; 𝑖 = 1,2, … , 𝑁𝑣; 𝑗 = 1,2, … , 0.5𝑁𝑝 • 𝐶𝑗𝑖 = 𝑥𝑗𝑖 ; 𝑖 = 1,2, … , 𝑁𝑣; 𝑗 = 0.5𝑁𝑝 + 1, 0.5𝑁𝑝 + 2, … , 𝑁𝑝 • 𝐴𝑗𝑖 𝐹 = 1 1+𝑒𝑥𝑝 (− 0.1 𝐴 𝑗𝑖 𝐷) • 𝐴𝑗𝑖 𝐷 = 𝐴𝑗𝑖 − 𝐶𝑖 𝑏𝑒𝑠𝑡 • 𝐶𝑗𝑖 𝐹 = 1 1+𝑒𝑥𝑝 − 0.1 𝐶 𝑗𝑖 𝐷 • 𝐶𝑗𝑖 𝐷 = 𝐶𝑗𝑖 − 𝐴𝑖 𝑏𝑒𝑠𝑡 Cation Anion Best Cation Best Anion
  • 14. Cont’d • 𝐶𝑗𝑖 𝑛𝑒𝑤 = 𝐶𝑗𝑖 + 𝐶𝑗𝑖 𝐹 𝐴𝑖 𝑏𝑒𝑠𝑡 − 𝐶𝑗𝑖 • 𝐴𝑗𝑖 𝑛𝑒𝑤 = 𝐴𝑗𝑖 + 𝐴𝑗𝑖 𝐹 𝐶𝑖 𝑏𝑒𝑠𝑡 − 𝐴𝑗𝑖 Cation Anion Best Cation Best Anion
  • 15. Cont’d • 𝐶𝑗𝑖 𝑛𝑒𝑤 = 𝐶𝑗𝑖 + 𝜑1 𝐴𝑖 𝑏𝑒𝑠𝑡 − 1 ; z𝑗𝑖 > 0.5 𝐶𝑗𝑖 + 𝜑1 𝐴𝑖 𝑏𝑒𝑠𝑡 ; z𝑗𝑖 < 0.5 𝑎𝑛𝑑 z𝑗𝑖 > 0.05 𝑥𝑖 𝑚𝑖𝑛 + z𝑗𝑖 (𝑥𝑖 𝑚𝑎𝑥 −𝑥𝑖 𝑚𝑖𝑛 ) ; z𝑗𝑖 < 0.05 • 𝐴𝑗𝑖 𝑛𝑒𝑤 = 𝐴𝑗𝑖 + 𝜑2 𝐶𝑖 𝑏𝑒𝑠𝑡 − 1 ; z𝑗𝑖 > 0.5 𝐴𝑗𝑖 + 𝜑2 𝐶𝑖 𝑏𝑒𝑠𝑡 ; z𝑗𝑖 < 0.5 𝑎𝑛𝑑 z𝑗𝑖 > 0.05 𝑥𝑖 𝑚𝑖𝑛 + z𝑗𝑖 (𝑥𝑖 𝑚𝑎𝑥 −𝑥𝑖 𝑚𝑖𝑛 ) ; z𝑗𝑖 < 0.05
  • 16. Result Analysis Generator Number Power output (MW) 𝒙 𝟏 ∗ (𝐌𝐖) 629.0191 𝒙 𝟐 ∗ (𝐌𝐖) 299.4592 𝒙 𝟑 ∗ (𝐌𝐖) 297.7103 𝒙 𝟒 ∗ (𝐌𝐖) 60.0 𝒙 𝟓 ∗ (𝐌𝐖) 60.0 𝒙 𝟔 ∗ (𝐌𝐖) 60.0 𝒙 𝟕 ∗ (𝐌𝐖) 60.0 𝒙 𝟖 ∗ (𝐌𝐖) 60.00001 𝒙 𝟗 ∗ (𝐌𝐖) 109.9108 𝒙 𝟏𝟎 ∗ (𝐌𝐖) 40.0 𝒙 𝟏𝟏 ∗ (𝐌𝐖) 40.00003 𝒙 𝟏𝟐 ∗ (𝐌𝐖) 55.0 𝒙 𝟏𝟑 ∗ (𝐌𝐖) 55.0 Loss (𝑷 𝑳) (𝐌𝐖) 26.09937 Minimum cost (𝑭 𝑻) ₹ /𝒉 18205.670 Average cost ₹/𝒉 18371.92733 Maximum cost ₹/ 18485.020 Standard deviation (SD) 76.844125
  • 17. Cont’d 1.832358E+04 1.842358E+04 1.852358E+04 1.862358E+04 1.872358E+04 1.882358E+04 1.892358E+04 0 100 200 300 400 500 600 700 Fuelcost(₹/hr) Iteration 13 Generator problem with loss (@ PD=1800MW)
  • 18. Conclusion  In this paper IMO algorithm is presented and applied on real world economic load dispatch.  The algorithm performance is very good and it may be the good optimization technique for many other engineering optimization problems.  A future study may be directed towards inclusion of chaotic maps in IMO algorithm.
  • 19. References 1. Dhillon JS, Kothari DP. Power system optimization. Prentice Hall of India Private Limited. 2010. 2. Sinha N, Chakrabarti R and Chattopadhyay PK, “Evolutionary programming techniques for economic load dispatch”, IEEE Transactions on evolutionary computation, vol. 7(1), pp.83-94, 2013 3. A. S. Reddy and K. Vaisakh, “Shuffled differential evolution for large scale economic dispatch,” Electr. Power Syst. Res., vol. 96, pp. 237–245, 2013. 4. M. Kheshti, X. Kang, Z. Bie, Z. Jiao, and X. Wang, “An effective Lightning Flash Algorithm solution to large scale non-convex economic dispatch with valve-point and multiple fuel options on generation units,” Energy, vol. 129, pp. 1–15, 2017. 5. Q. Qin, S. Cheng, X. Chu, X. Lei, and Y. Shi, “Solving non-convex / non- smooth economic load dispatch problems via an enhanced particle swarm optimization,” Appl. Soft Comput. J., vol. 59, pp. 229–242, 2017. 6. B. Javidy, A. Hatamlou, and S. Mirjalili, “Ions motion algorithm for solving optimization problems,” Appl. Soft Comput. J., vol. 32, pp. 72–79, 2015