Intelligent Renewable Energy Systems. Группа авторов

Чтение книги онлайн.

Читать онлайн книгу Intelligent Renewable Energy Systems - Группа авторов страница 13

Intelligent Renewable Energy Systems - Группа авторов

Скачать книгу

Improvement of the students’ performance based on this concept may be represented by (Equation 1. 4) [66]

      where min and max are the two variables that indicate the minimum and the maximum marks of the subject, respectively, and rand generates a random number between 0 and 1.

      The process of getting interested in a subject for different students is not deterministic. It depends on the students’ psychology. So, it may be said that the selection of different categories of students is a random process.

      1.2.2 Performance of SPBO for Solving Benchmark Functions

      The performance of the algorithms selected is evaluated on the basis of the optimal result obtained and on the basis of convergence mobility. For the purposes of analysis, the algorithms are found to converge when the gap between the optimal function result and the result obtained crosses below 1×10-5. The results obtained below 1×10-5 are considered as equal to zero. The parameters of PSO, TLBO, CS and SOS are considered according to the dimension of the benchmark function. But SPBO does not have any parameter and the size of the population needs not vary according to the dimension of the benchmark functions. With the increase of dimension of the functions, the size of the population of the proposed SPBO needs not to be increased. That’s why the population size of SPBO for all the considered benchmark functions is considered to be constant. It is considered as 20 for the proposed SPBO. In order to have a fair comparison of the performance of all the algorithms, the analysis is done based on the number of fitness function evaluations (NFFE) taken to converge.

Problem Type of the function Name of the functions F(x*) Initial range Bounds Dimension (D)
F1 Unimodal Shifted Sphere Function -450 [-100,100]D [-100,100] D 30
F2 Unimodal Shifted Schwefel’s Problem 1.2 -450 [-100,100] D [-100,100] D 30
F3 Unimodal Shifted Rotated High Conditioned Elliptic Function -450 [-100,100] D [-100,100] D 30
F4 Unimodal Shifted Schwefel’s Problem 1.2 with Noise in Fitness -450 [-100,100] D [-100,100] D 30
F5 Unimodal Schwefel’s Problems 2.6 with Global Optimum on Bounds -310 [-100,100] D [-100, 100] D 30
F6 Basic multimodal Shifted Rosenbrock’s Function 390 [-100, 100] D [-100, 100] D 30
F7 Basic multimodal Shifted Rotated Griewank’s Function without Bounds -180 [0, 600] D [0, 600] D 30
F8 Basic multimodal Shifted Rotated Ackley’s Function with Global Optimum on Bounds -140 [-32, 32] D [-32, 32] D 30
F9 Basic multimodal Shifted Rastrigin’s Function -330 [-5, 5] D [-5, 5] D 30
F10 Basic multimodal Shifted Rotated Rastrigin’s Function -330 [-5, 5] D [-5, 5] D 30

      1.2.3

Скачать книгу