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Table 5.

Horizontal averaged convective properties of the models.

Name u rms tot $ u_{\mathrm{rms}}^{\mathrm{tot}} $ [km/s] τconv [day] HP [cm] Λt Λconv ΛHI ΛHeII ΛOV
v036_4_150x20 1.90 3.21 1.24 × 1010 3.35 2.13 0.39 0.86 0.39
v036_4_150x30 1.65 3.42 1.24 × 1010 3.33 1.97 0.34 0.72 0.87
v036_6_150x20 1.25 4.50 1.26 × 1010 3.44 1.92 0.33 0.70 1.02
v036_6_150x30 1.51 3.74 1.26 × 1010 3.44 1.93 0.33 0.70 1.02
v036_6_150x40 1.57 3.55 1.26 × 1010 3.42 1.90 0.31 0.70 1.20
v036_6_150x50 1.53 3.67 1.26 × 1010 3.44 1.92 0.33 0.70 1.20
v036_6_200x20 1.52 3.42 1.29 × 1010 3.23 1.74 0.25 0.70 1.06
v036_8_150x20 1.10 5.02 1.26 × 1010 3.43 1.89 0.30 0.70 1.20
v036_8_150x30 1.30 4.31 1.29 × 1010 3.55 1.88 0.28 0.69 1.17
v036_8_150x40 1.33 4.21 1.29 × 1010 3.55 1.88 0.28 0.69 1.35
v036_9_150x30 1.19 4.70 1.29 × 1010 3.54 1.87 0.31 0.69 1.35
v036_10_150x20 1.31 4.43 1.29 × 1010 3.58 1.94 0.42 0.69 1.35
v036_10_150x30 1.57 3.58 1.35 × 1010 3.78 1.81 0.35 0.66 1.13
v036_12_122x60 1.03 5.53 1.30 × 1010 3.55 1.89 0.25 0.79 1.18
v036_12_150x20 1.09 5.26 1.32 × 1010 3.66 1.88 0.27 0.67 1.50
v036_12_150x30 1.05 5.38 1.32 × 1010 3.66 1.86 0.37 0.67 1.69
v036_12_150x40 1.12 5.00 1.35 × 1010 3.76 1.79 0.27 0.66 1.47
v036_15_150x50⋆ 1.05 5.20 1.41 × 1010 3.93 1.68 0.26 0.63 1.58
v036_18_150x60⋆ 1.25 4.41 1.51 × 1010 4.24 1.57 0.24 0.59 1.16
v036_45_122x40 0.54 10.31 1.39 × 1010 3.85 1.75 0.23 0.74 1.45
v036_45_122x60 0.81 6.47 1.36 × 1010 3.75 1.67 0.24 0.63 1.26
v036_45_150x20 0.43 12.44 1.35 × 1010 3.69 1.72 0.24 0.66 1.47
v046_6_152x20 2.54 2.49 1.45 × 1010 3.50 1.88 0.53 0.78 0.99
v046_6_152x30 1.88 3.20 1.45 × 1010 3.57 1.79 0.35 0.65 1.29
v046_12_152x40 1.38 4.34 1.58 × 1010 3.97 1.64 0.33 0.60 1.35

Notes. The panels are separated according to the angular size and physical parameters of the models. The columns are (from left to right) the mean convective velocity ( u rms tot $ u_{\mathrm{rms}}^{\mathrm{tot}} $), convective turnover timescale (τconv), pressure scale height at the bottom of the convective zone (Hp), turbulent length scale (Λt), full length of the entire convective region (Λconv), length scale of the hydrogen ionization zone (ΛHI), length of the second helium ionization zone (ΛHeII), size of the overshooting region (ΛOV).

(⋆)

This model did not reach τrelax simulation time, due to the large numerical cost; therefore, it is not reliable. It is only included here to show the trends. Statistical evaluation is performed over an interval of 12–18 days.

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