A theory for fluids in cornered capillaries shows that partially wet corner films exist only inside a bounded region of contact-angle and curvature parameter space.
•case I:s c1 ≤s≤1,s c1 = 1− π 4 f(s) aγ =−8 cosθ+ 4 √π(1−s) 1/2 (C25) •case II: 0≤s≤s c2,s c2 = A(θ) (cosθ−sinθ) 2 f(s) aγ =−sign π 4 −θ 8 p A(θ)s1/2 (C26) A(θ) is given in Eq
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Existent condition of partially wet state in capillary tubes
A theory for fluids in cornered capillaries shows that partially wet corner films exist only inside a bounded region of contact-angle and curvature parameter space.