Water in a cylindrical tank has been turning long enough to rotate as a rigid body…

PHYSICS · Multi-part · Fermi University Physics · Mechanics & Dynamical Systems · Fluids & Continuum Physics · Kinematics, conservation laws and ideal flow

Fluids and Continuum Physics, Ch Kinematics of flow: fields, streamlines and the material derivative

Problem

Water in a cylindrical tank has been turning long enough to rotate as a rigid body about the vertical axis x=y=0x = y = 0. In Cartesian coordinates the velocity field is u=(−Ωy,  Ωx,  0),Ω=3.0 s−1,\mathbf{u} = (-\Omega y,\; \Omega x,\; 0), \qquad \Omega = 3.0\ \mathrm{s^{-1}}, with xx, yy in metres. One side of the tank is warmed, and a steady temperature field is maintained in the water, T=T0+Ax,T0=293 K,A=8.0 K m−1,T = T_0 + Ax, \qquad T_0 = 293\ \mathrm{K}, \qquad A = 8.0\ \mathrm{K\,m^{-1}}, which reads the same at every fixed point at all times. Heating and heat conduction together hold this field steady; how they do so does not matter here. Consider the point RR at x=0.20 mx = 0.20\ \mathrm{m}, y=0.10 my = 0.10\ \mathrm{m}. ((a)) Compute ∇⋅u\nabla\cdot\mathbf{u} and state what it says about the volume of a fluid parcel. ((b)) Find DT/DtDT/Dt for the particle at RR. ((c)) Find axa_x and aya_y for that particle, and say in one sentence in which direction a\mathbf{a} points.

Browse the problem library