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It is difficult to perform head-on collision experiments at capillary numbers larger than approximately 0.01 in the four-roll mill that is used in our lab. For larger Ca, the drops collide and are maintained via an active control system in the head-on configuration for a very long period of time, but eventually rotate out of the plane of the flow and separate (Ref. 8). We do not know at this stage whether this behavior at large Ca is due to limitations of the flow control scheme, or is due to inhibited coalescence due to the increasing importance of the re-circulating flow within the drops (Ref. 16), as originally suggested by Loewenberg (Ref. 17)
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It is difficult to perform head-on collision experiments at capillary numbers larger than approximately 0.01 in the four-roll mill that is used in our lab. For larger Ca, the drops collide and are maintained via an active control system in the head-on configuration for a very long period of time, but eventually rotate out of the plane of the flow and separate (Ref. 8). We do not know at this stage whether this behavior at large Ca is due to limitations of the flow control scheme, or is due to inhibited coalescence due to the increasing importance of the re-circulating flow within the drops (Ref. 16), as originally suggested by Loewenberg (Ref. 17).
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The details of the full two drops calculation will be given in a subsequent publication and are presented in Baldessari (Ref. 41)
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