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22
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85035273642
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(Formula presented) was obtained by numerical derivation of (Formula presented), where (Formula presented) is the driving frequency and k the critical wave number for parametric excitation. This value of (Formula presented) was within 10% of that given by the shallow fluid approximation 19,(Formula presented)
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(Formula presented) was obtained by numerical derivation of (Formula presented), where (Formula presented) is the driving frequency and k the critical wave number for parametric excitation. This value of (Formula presented) was within 10% of that given by the shallow fluid approximation 19,(Formula presented).
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26
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85035271717
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13 (Formula presented) in the highly dissipative regime was fit by: (Formula presented). For (Formula presented) (Formula presented) (Formula presented)
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In 13 (Formula presented) in the highly dissipative regime was fit by: (Formula presented). For (Formula presented) (Formula presented) (Formula presented).
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27
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85035277107
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For our experimental conditions, (Formula presented). The gravity wave approximation here is justified, since surface tension 13 in this parameter range plays a negligible role
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For our experimental conditions, (Formula presented). The gravity wave approximation here is justified, since surface tension 13 in this parameter range plays a negligible role.
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28
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85035296943
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Phys. Fluids (to be published)
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Y. Murakami, Phys. Fluids (to be published).
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Murakami, Y.1
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