xvideo xx 665

xvideo xx 761

xvideo xx 661 b

xvideo xx 665

xvideo xx 665

xvideo xx 106f

xvideo xx 661 a

xvideo xx 334f

xvideo xx 8661

Authors | Formulations |
---|---|

Price, 1984 [8] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(T − _{i}T)(1 − _{j}ε) + a_{4}TΔ_{j}ε |

Prata and Platt, 1991 [14] | ${T}_{s}={a}_{0}+{a}_{1}\frac{{T}_{i}}{\mathit{\epsilon}}+{a}_{2}\frac{{T}_{j}}{\mathit{\epsilon}}+{a}_{3}\frac{1-\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Vidal, 1991 [15] | ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}-{T}_{j})+{a}_{3}\frac{1-\mathit{\epsilon}}{\mathit{\epsilon}}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Ulivieri et al., 1992 [16] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(1 − ε) + a_{4}Δε |

Sobrino et al., 1993 [17] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(T − _{i}T)_{j}^{2} + a_{4}(1 − ε) + a_{5}Δε |

Sobrino et al., 1994 [18] | ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}-{T}_{j})+{a}_{3}\mathit{\epsilon}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Coll et al., 1997 [19] | T = _{s}T_{i}+ a_{0} + a_{1}(T − _{i}T) + _{j}a_{2}(T − _{i}T)_{j}^{2} + a_{3}(1 − ε) + a_{4}Δε |

Seller | Coupons | Base Price | Total Price | |

$14.99 +$1.98 shipping | $16.97 |
Shop | ||

$25.19 +$2.99 shipping | $28.18 |
Shop | ||

$14.99 Free Shipping | $14.99 |
Shop | ||

Use International Shipping Rates |

RMSE (K) | Authors | |||||||||

VZA(°) | GSW | Price84 | Prata91 | Vidal91 | Ulivieri92 | Sobrino93 | Sobrino94 | Coll97 | BL95 | |

0 | 0.37 | 0.73 | 1.15 | 0.38 | 0.38 | 0.37 | 0.38 | 0.38 | 0.22 | |

33.56 | 0.41 | 0.74 | 1.26 | 0.43 | 0.42 | 0.42 | 0.42 | 0.43 | 0.25 | |

44.42 | 0.46 | 0.74 | 1.35 | 0.48 | 0.47 | 0.47 | 0.47 | 0.47 | 0.28 | |

51.32 | 0.52 | 0.75 | 1.43 | 0.53 | 0.53 | 0.51 | 0.53 | 0.52 | 0.32 | |

56.25 | 0.57 | 0.77 | 1.49 | 0.58 | 0.58 | 0.57 | 0.58 | 0.57 | 0.36 | |

60 | 0.63 | 0.80 | 1.54 | 0.64 | 0.64 | 0.62 | 0.64 | 0.62 | 0.41 |

Authors | Formulations |
---|---|

Price, 1984 [8] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(T − _{i}T)(1 − _{j}ε) + a_{4}TΔ_{j}ε |

Prata and Platt, 1991 [14] | ${T}_{s}={a}_{0}+{a}_{1}\frac{{T}_{i}}{\mathit{\epsilon}}+{a}_{2}\frac{{T}_{j}}{\mathit{\epsilon}}+{a}_{3}\frac{1-\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Vidal, 1991 [15] | ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}-{T}_{j})+{a}_{3}\frac{1-\mathit{\epsilon}}{\mathit{\epsilon}}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Ulivieri et al., 1992 [16] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(1 − ε) + a_{4}Δε |

Sobrino et al., 1993 [17] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(T − _{i}T)_{j}^{2} + a_{4}(1 − ε) + a_{5}Δε |

Sobrino et al., 1994 [18] | ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}-{T}_{j})+{a}_{3}\mathit{\epsilon}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Coll et al., 1997 [19] | T = _{s}T_{i}+ a_{0} + a_{1}(T − _{i}T) + _{j}a_{2}(T − _{i}T)_{j}^{2} + a_{3}(1 − ε) + a_{4}Δε |

Authors | Formulations |
---|---|

Price, 1984 [8] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(T − _{i}T)(1 − _{j}ε) + a_{4}TΔ_{j}ε |

Prata and Platt, 1991 [14] | ${T}_{s}={a}_{0}+{a}_{1}\frac{{T}_{i}}{\mathit{\epsilon}}+{a}_{2}\frac{{T}_{j}}{\mathit{\epsilon}}+{a}_{3}\frac{1-\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Vidal, 1991 [15] | ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}-{T}_{j})+{a}_{3}\frac{1-\mathit{\epsilon}}{\mathit{\epsilon}}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Ulivieri et al., 1992 [16] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(1 − ε) + a_{4}Δε |

Sobrino et al., 1993 [17] | T = _{s}a_{0} + a_{1}T + _{i}a_{2}(T − _{i}T) + _{j}a_{3}(T − _{i}T)_{j}^{2} + a_{4}(1 − ε) + a_{5}Δε |

Sobrino et al., 1994 [18] | ${T}_{s}={a}_{0}+{a}_{1}{T}_{i}+{a}_{2}({T}_{i}-{T}_{j})+{a}_{3}\mathit{\epsilon}+{a}_{4}\frac{\mathrm{\Delta}\mathit{\epsilon}}{\mathit{\epsilon}}$ |

Coll et al., 1997 [19] | T = _{s}T_{i}+ a_{0} + a_{1}(T − _{i}T) + _{j}a_{2}(T − _{i}T)_{j}^{2} + a_{3}(1 − ε) + a_{4}Δε |