TY - JOUR
T1 - Predictions of the effect of clumping on the wind properties of O-type stars
AU - Muijres, L.E.
AU - de Koter, A.
AU - Vink, J.S.
AU - Krticka, J.
AU - Kubát, J.
AU - Langer, N.
PY - 2011
Y1 - 2011
N2 - Aims. Both empirical evidence and theoretical findings indicate that the stellar winds of massive early-type stars are inhomogeneous,
i.e., porous and clumpy. For relatively dense winds, empirically derived mass-loss rates might be reconciled with predictions if these
empirical rates are corrected for clumping. The predictions, however, do not account for structure in the wind. To allow for a consistent
comparison, we investigate and quantify the effect of clumpiness and porosity of the outflow on the predicted wind energy and the
maximal effect on the mass-loss rate of O-type stars.
Methods. Combining non-LTE model atmospheres and aMonte Carlo method to compute the transfer of momentum from the photons
to the gas, the effect of clumping and porosity on the energy transferred from the radiation field to the wind is computed in outflows
in which the clumping and porosity stratification is parameterized by heuristic prescriptions.
Results. The impact of structure in the outflow on the wind energy is complex and is a function of stellar temperature, the density of
gas in the clumps, and the physical scale of the clumps. If the medium is already clumped in the photosphere, the emergent radiation
field will be softer, slightly increasing the wind energy of relatively cool O stars (30 000 K) but slightly decreasing it for relatively hot
O stars (40 000K). More important is that as a result of recombination of the gas in a clumped wind the line force increases. However,
because of porosity the line force decreases, simply because photons may travel in-between the clumps, avoiding interactions with
the gas. If the changes in the wind energy only affect the mass-loss rate and not the terminal velocity of the flow, we find that the
combined effect of clumpiness and porosity is a small reduction in the mass-loss rate if the clumps are smaller than 1/100th the local
density scale height Hρ. In this case, empirical mass-loss determinations based on Hα fitting and theory match for stars with dense
winds ( ˙M >∼ 10−7 M yr−1) if the overdensity of gas in the clumps, relative to the case of a smooth wind, is modest. For clumps larger
than 1/10th Hρ, the predicted mass-loss rates exhibit almost the same dependence on clumpiness as do empirical rates. We show that
this implies that empirical and predicted mass-loss rates can no longer be matched. Very high overdensities of gas in clumps of such
large size may cause the predicted ˙M to decrease by a factor of from 10 to 100. This type of structure is likely not to be the cause of
the “weak-wind problem” in early-type stars, unless a mechanism can be identified that causes extreme structure to develop in winds
for which ˙M
AB - Aims. Both empirical evidence and theoretical findings indicate that the stellar winds of massive early-type stars are inhomogeneous,
i.e., porous and clumpy. For relatively dense winds, empirically derived mass-loss rates might be reconciled with predictions if these
empirical rates are corrected for clumping. The predictions, however, do not account for structure in the wind. To allow for a consistent
comparison, we investigate and quantify the effect of clumpiness and porosity of the outflow on the predicted wind energy and the
maximal effect on the mass-loss rate of O-type stars.
Methods. Combining non-LTE model atmospheres and aMonte Carlo method to compute the transfer of momentum from the photons
to the gas, the effect of clumping and porosity on the energy transferred from the radiation field to the wind is computed in outflows
in which the clumping and porosity stratification is parameterized by heuristic prescriptions.
Results. The impact of structure in the outflow on the wind energy is complex and is a function of stellar temperature, the density of
gas in the clumps, and the physical scale of the clumps. If the medium is already clumped in the photosphere, the emergent radiation
field will be softer, slightly increasing the wind energy of relatively cool O stars (30 000 K) but slightly decreasing it for relatively hot
O stars (40 000K). More important is that as a result of recombination of the gas in a clumped wind the line force increases. However,
because of porosity the line force decreases, simply because photons may travel in-between the clumps, avoiding interactions with
the gas. If the changes in the wind energy only affect the mass-loss rate and not the terminal velocity of the flow, we find that the
combined effect of clumpiness and porosity is a small reduction in the mass-loss rate if the clumps are smaller than 1/100th the local
density scale height Hρ. In this case, empirical mass-loss determinations based on Hα fitting and theory match for stars with dense
winds ( ˙M >∼ 10−7 M yr−1) if the overdensity of gas in the clumps, relative to the case of a smooth wind, is modest. For clumps larger
than 1/10th Hρ, the predicted mass-loss rates exhibit almost the same dependence on clumpiness as do empirical rates. We show that
this implies that empirical and predicted mass-loss rates can no longer be matched. Very high overdensities of gas in clumps of such
large size may cause the predicted ˙M to decrease by a factor of from 10 to 100. This type of structure is likely not to be the cause of
the “weak-wind problem” in early-type stars, unless a mechanism can be identified that causes extreme structure to develop in winds
for which ˙M
U2 - 10.1051/0004-6361/201014290
DO - 10.1051/0004-6361/201014290
M3 - Article
SN - 0004-6361
VL - 526
SP - A32/1-A32/11
JO - Astronomy and Astrophysics
JF - Astronomy and Astrophysics
ER -