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Energy Method for Stability of Superposed Fluids

Example 5.5 Energy Method for Stability of Superposed Fluids [Pg.288]

Use Equation 5.127 to determine the stability condition for superposed fluids. Solution [Pg.288]

This result agrees with that obtained by the general analysis above (see remark following Equation 5.61). [Pg.288]

In systrans where A is a thin Uqtttd film in gas, the effect of gravity in Equation 5.126 is replaced by that of disjoining presstrre. As Eqttation 5.104 indicates for an equilibrium film having a tmiform value of 1), taken as zmr for converrience. Pa is given by -( )y + )e), which, in tirm, is V(H -i- H ). Recogrrizing that [Pg.288]

Manipulations similar to those above for a single interface yield the same expression for as in Equation 5.119. For a thin liquid film on a solid surface, only the fluid interface is deformed and the faetor of 2 disappears from the term multiplying (dll/dh) in Equation 5.128. [Pg.289]




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