Tham khảo tài liệu 'sabatier agrawal machado advances in fractional calculus episode 11', kỹ thuật - công nghệ, cơ khí - chế tạo máy phục vụ nhu cầu học tập, nghiên cứu và làm việc hiệu quả | NEW POSSIBILITIES IN DESCRIPTION OF DISORDERED MEDIA 387 Appendix A Table 1. The calculated fractal dimension for clusters obtained for different systems obtained by the methods described in section 2. For the lattice model with random exclusion permission we use the abbreviation LMRE P Type of model number of neighbors z Ro with values of the stdev a with values of the stdev No with values of the stdev p with values of the stdev D with values of the stdev Size of the cluster diameter number of particles involved Conventional DLA-procedure A A A A A 00 o -C JI a A random rain model. A A 1 9807 A 0 5399 A 1 858 A n 104 R The lattice DLA model z 3 A 0 991 A A A A 5c II 1 w 00 00 LMRE z 3 A A A A A 5c II II 5 o 00 LMRP z 3 A A A A A 5c II II 1 The lattice DLA model z 4 A A A A A N 8042 R 167 LMRE z 4 A A A A A N 8250 R 165 LMRP z 4 A A A A A N 11801 R 167 The lattice DLA model z 6 A A A A A in II II S LMRE z 6 A A A A A N 6118 R 292 LMRP z 6 A A A A A 5c II II 5 388 Nigmatullin and Alekhin Table 2. Parameters of the QF obtained by the procedure described in section 3 Type of model Ro with values of the stdev a with values of the stdev No with values of the stdev p with values of the stdev D with values of the stdev Size of the cluster diameter .
