- #1
member 428835
Hi PF!
I am considering a partial cylinder filled with fluid. By partial I mean consider something like a half-pipe. If a small disturbance is present, the fluid radius on the open side of the cylinder is ##r=R(1+\epsilon f(\theta,z,t))##. The Young-Laplace equation for capillary pressure is ##p/\gamma = 2H = \kappa_1+\kappa_2##, the two principal radii of curvatures. The author then states that this pressure is ##p = -\gamma[f/R^2-f_{\theta \theta}/R^2-f_{zz}]##, where subscripts denote differentiation.
Can someone help me see why this is the case? We are working in cylindrical coordinates. Thanks so much!
I am considering a partial cylinder filled with fluid. By partial I mean consider something like a half-pipe. If a small disturbance is present, the fluid radius on the open side of the cylinder is ##r=R(1+\epsilon f(\theta,z,t))##. The Young-Laplace equation for capillary pressure is ##p/\gamma = 2H = \kappa_1+\kappa_2##, the two principal radii of curvatures. The author then states that this pressure is ##p = -\gamma[f/R^2-f_{\theta \theta}/R^2-f_{zz}]##, where subscripts denote differentiation.
Can someone help me see why this is the case? We are working in cylindrical coordinates. Thanks so much!