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Table 2

Fit coefficients of the rising and falling slopes of η-Aquariids and Orionids average profiles presented in Figs. 4 and 5.

η-Aquariids

System Bp Bm Bp2 Bm2 ZHRm ZHRm2 (°) (°)
29 MHz 0.111 ± 0.005 0.073 ± 0.003 0.122 ± 0.008 0.094 ± 0.007 76 66 44.5 46.8
38 MHz 0.126 ± 0.012 0.074 ± 0.006 0.164 ± 0.010 0.108 ± 0.006 51 49 44.7 45.3
VMN 0.129 ± 0.010 0.083 ± 0.006 0.180 ± 0.012 0.105 ± 0.006 70 60 44.3 47.3
VMDB 0.104 ± 0.014 0.065 ± 0.007 0.121 ± 0.011 0.106 ± 0.014 70 64 44.4 46.4

[1] 0.135 ± 0.003 0.078 ± 0.003

Orionids

System Bp Bm Bp2 Bm2 ZHRm ZHRm2 (°) (°)

29 MHz 0.078 ± 0.009 0.069 ± 0.007 0.106 ± 0.008 0.103 ± 0.009 33 31 207.3 209.7
38 MHz 0.215 ± 0.047 0.118 ± 0.024 0.349 ± 0.043 0.233 ± 0.032 35 32 208.2 210.3
VMN 0.073 ± 0.008 0.054 ± 0.006 0.128 ± 0.011 0.095 ± 0.009 35 32 207.7 210.0
VMDB 0.073 ± 0.022 0.080 ± 0.023 0.120 ± 0.027 0.168 ± 0.044 40 33 207.7 210.5

[2] 0.122 0.098
[3] 0.140 0.140

Notes. Each estimate is followed by the fit formal uncertainty. The parameters Bp2 and Bm2 are adaptations of Eq. (2)’s Bp and Bm coefficients for profiles containing a dip or a plateau. The modeled maximum ZHR (ZHRm, ZHRm2) and the solar longitude endpoints of the plateau () are provided for information. [1]: η-Aquariids coefficients provided by Campbell-Brown & Brown (2015). [2,3]: Orionids coefficients determined by Jenniskens (1994) from Northern [2]and Southern [3] Hemisphere observations.

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