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18 model. Equation (13) appears to be a reasonable approximation for the terminal bubble velocity also in nonclassical cases, where γ may contain additional physics.
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58
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note
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We note that since simulations are of limited resolution and thus may resolve only a small number (∼ 100) of modes, the assumptions leading to the approximation for the saturation amplitude in Eq. (11) are, at most, only roughly satisfied. Also in cases of discrete or isolated modes, Eq. (8) is more suitable than Eq. (11). We therefore use Eq. (8) as the saturation criterion in the present model.
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