by Li, illustrated in Figure 33, is characterized by liquids in containers whose interiors are in the form of surfaces of revolution. 0^ , and are respective surface tensions at the liquid-vapor, liquid-solid, and solid-vapor interfaces, in dyne/cm; in the plane of Figure 33, the "horizontal boundary" is the point intersection of the surface (liquid-vapor interface) with the toroidal annulus shown, u = u(x) is the vapor-annulus interface, v = v(x) is the liquid-annulus interface, and z = z(x) is the liquid-vapor interface, where u - u(x) and v = v(x) are known and z = z(x) is sought. The total potential energy K of the system consists of the sum of surface energies and the effective (net) central-force-field or contact-force potential energy, where FIGURE 33 Liquid in container of revolution in low gravity field
RkJQdWJsaXNoZXIy MTU5NjU0Mg==