2014 |
8 |
Conventional Method |
1 |
0.093023 |
0.093023 |
0.17 |
Proposed Method (w = 1) |
0.75 |
0.222222 |
0.732558 |
0.343 |
Proposed Method (w = 485) |
1 |
0.145455 |
0.453488 |
0.254 |
Proposed Method (w = 8.5) |
0.75 |
0.222222 |
0.732558 |
0.343 |
2015 |
63 |
Conventional Method |
1 |
0.134043 |
0.134043 |
0.236 |
Proposed Method (w = 1) |
0.952381 |
0.437956 |
0.829787 |
0.6 |
Proposed Method (w = 485) |
1 |
0.225806 |
0.540426 |
0.368 |
Proposed Method (w = 8.5) |
0.904762 |
0.431818 |
0.82766 |
0.585 |
2016 |
5 |
Conventional Method |
1 |
0.060241 |
0.060241 |
0.114 |
Proposed Method (w = 1) |
1 |
0.138889 |
0.626506 |
0.244 |
Proposed Method (w = 485) |
1 |
0.104167 |
0.481928 |
0.189 |
Proposed Method (w = 8.5) |
1 |
0.138889 |
0.626506 |
0.244 |
2017 |
5 |
Conventional Method |
1 |
0.054348 |
0.054348 |
0.103 |
Proposed Method (w = 1) |
1 |
0.714286 |
0.978261 |
0.833 |
Proposed Method (w = 485) |
1 |
0.076923 |
0.347826 |
0.143 |
Proposed Method (w = 8.5) |
1 |
0.714286 |
0.978261 |
0.833 |
2020 |
1 |
Conventional Method |
1 |
0.02381 |
0.02381 |
0.047 |
Proposed Method (w = 1) |
1 |
0.111111 |
0.809524 |
0.2 |
Proposed Method (w = 485) |
1 |
0.034483 |
0.333333 |
0.067 |
Proposed Method (w = 8.5) |
1 |
0.125 |
0.833333 |
0.222 |
2021 |
2 |
Conventional Method |
1 |
0.057143 |
0.057143 |
0.108 |
Proposed Method (w = 1) |
1 |
0.4 |
0.914286 |
0.571 |
Proposed Method (w = 485) |
1 |
0.090909 |
0.428571 |
0.167 |
Proposed Method (w = 8.5) |
1 |
0.4 |
0.914286 |
0.571 |
2022 |
19 |
Conventional Method |
1 |
0.097436 |
0.097436 |
0.178 |
Proposed Method (w = 1) |
0.368421 |
0.466667 |
0.897436 |
0.412 |
Proposed Method (w = 485) |
0.894737 |
0.114865 |
0.317949 |
0.204 |
Proposed Method (w = 8.5) |
0.631579 |
0.461538 |
0.892308 |
0.533 |
2023 |
2 |
Conventional Method |
1 |
0.030303 |
0.030303 |
0.059 |
Proposed Method (w = 1) |
1 |
0.333333 |
0.939394 |
0.5 |
Proposed Method (w = 485) |
1 |
0.037037 |
0.212121 |
0.071 |
Proposed Method (w = 8.5) |
1 |
0.285714 |
0.924242 |
0.444 |