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Table 3.

Parameters of the rotating models.

Model Dh Dv Overshoot dov K (erg) νadd (cm2 s−1) ν0, α Turbulence
solidRA DA 0.0325 1.1 × 1031
R1 Mathis et al. (2018) Zahn (1992) 7.5 × 1030
R1B.S Mathis et al. (2018) Zahn (1992) DB 0.340 7.5 × 1030
R1B.E Mathis et al. (2018) Zahn (1992) DB 0.100 7.5 × 1030
R1A Mathis et al. (2018) Zahn (1992) DA 0.0325 7.5 × 1030
R1K Mathis et al. (2018) Zahn (1992) DK 0.055 7.5 × 1030
νR1A Mathis et al. (2018) Zahn (1992) DA 0.0325 7.5 × 1030 3.5 × 104
ν.spadaR1A Mathis et al. (2018) Zahn (1992) DA 0.0325 1.2 × 1030 2.5 × 105
ν.spada(t)R1A Mathis et al. (2018) Zahn (1992) DA 0.0325 7.5 × 1030 2.5 × 104, 0.5
ν2.spada(t)R1A Mathis et al. (2018) Zahn (1992) DA 0.0325 7.5 × 1030 100, 12
Mathis et al. (2018) Zahn (1992) DA 0.0325 7.5 × 1030 3.5 × 104 DT6.425
Mathis et al. (2018) Zahn (1992) DA 0.0325 7.5 × 1030 3.5 × 104 DT6.42
Mathis et al. (2018) Zahn (1992) DA 0.0325 7.5 × 1030 3.5 × 104 DPM5000
Mathis et al. (2018) Zahn (1992) DA 0.0325 7.5 × 1030 3.5 × 104 DTach
R2A Zahn (1992) Talon & Zahn (1997) DA 0.0325 7.5 × 1030
Zahn (1992) Talon & Zahn (1997) DA 0.0325 3.0 × 1030
Zahn (1992) Talon & Zahn (1997) DA 0.0325 4.5 × 1030 2.5 × 104
R3A Mathis et al. (2004) Zahn (1992) DA 0.0325 7.5 × 1030
νR3A Mathis et al. (2004) Zahn (1992) DA 0.0325 7.5 × 1030 3.5 × 104

Notes. Models (Col. 1) related to the prescriptions for horizontal and vertical turbulent viscosities (Cols. 2 and 3 respectively), the formalism for the overshoot (Col. 4), the value adopted for the free parameter dov that controls the depth of the overshooting (Col. 5), the wind torque K (Col. 6), the value of the additional constant viscosity νadd (Col. 7), the parameters describing its evolution (ν0 and α) according to Eq 20 (Col. 8), and the adopted turbulence coefficient (Col. 9). References. DB: Baraffe et al. (2017), DA: Augustson & Mathis (2019), DK: Korre et al. (2019), DT.425: Richard et al. (2005), DT.42: Richard et al. (2005), DPM5000: Richard et al. (2005), DTach: Brun et al. (1999)

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