Open Access

Table 1

Simulations carried out with both PAMDEAS and PHANTOM.

Name Species Bouncing & compaction Disruption a0 (µm) υfrag (m s−1)
GF-Si-comp-Vf10 Si No No Comp 10
GF-Si-comp-Vf20 Si No No Comp 20
GF-Si-comp-Vf40 Si No No Comp 40
GF-Si-a02-Vf10 Si No No 0.2 10
GF-Si-a02-Vf20 Si No No 0.2 20
GF-Si-a02-Vf40 Si No No 0.2 40
GBFc-Si-a02-Vf10 Si Yes No 0.2 10
GBFc-Si-a02-Vf20 Si Yes No 0.2 20
GBFc-Si-a02-Vf40 Si Yes No 0.2 40
GBFcS-Si-a02-Vf205 (*) Si Yes No 0.2 20
GF-H2O-comp-Vf15 H2O No No Comp 15
GF-H2O-a02-Vf15 H2O No No 0.2 15
GBFc-H2O-a02-Vf15 H2O Yes No 0.2 15
GBFcD-Si-a02-Vf10 Si Yes Yes 0.2 10
GBFcD-Si-a02-Vf20 Si Yes Yes 0.2 20
GBFcD-H20-a02-Vf15 H2O Yes Yes 0.2 15

Notes. The ‘G’ stands for growth, ‘F’ for fragmentation, ‘B’ for bounce, ‘c’ for compaction, and ‘D’ for rotational disruption. The term ‘comp’ in the column for the monomer size a0 denotes compact grains, with porosity evolution not taken into account. ‘D’ simulations were run only with PHANTOM. (*)This simulation includes a snow line, indicated by ‘S’, with an inner threshold of 20 m s−1 and an outer threshold of 5 m s−1 to model the CO snow line (T = 20 K, approximately ~100 au).

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