Team | 1 | 2 | 3 | 4 | 5 | RECORDS | |
---|---|---|---|---|---|---|---|

New Orleans | (2) | 25 | 19 | 17 | 25 | 12 | 7-7, 1-1 SLC |

A&M-Corpus Christi | (3) | 21 | 25 | 25 | 23 | 15 | 5-8, 2-0 SLC |

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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 |

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