A steady two-dimensional water flow near a stagnation point is described

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

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

Problem

A steady two-dimensional water flow near a stagnation point is described, in the continuum picture, by the velocity field u=(Sx,  −Sy,  0),S=2.0 s−1,\mathbf{u} = (Sx,\; -Sy,\; 0), \qquad S = 2.0\ \mathrm{s^{-1}}, with xx, yy in metres and uu, vv in metres per second. The water carries the temperature field T=T0+Ax,T0=288 K,A=5.0 K m−1,T = T_0 + Ax, \qquad T_0 = 288\ \mathrm{K}, \qquad A = 5.0\ \mathrm{K\,m^{-1}}, which does not change with time at any fixed point, held so by heating and heat conduction that we need not describe. Consider the point PP at x=0.40 mx = 0.40\ \mathrm{m}, y=0.30 my = 0.30\ \mathrm{m}. ((a)) Evaluate ∇⋅u\nabla\cdot\mathbf{u} and say whether the flow is incompressible. ((b)) Find DT/DtDT/Dt for the fluid particle that is at PP. ((c)) Find the two components axa_x, aya_y of the acceleration of that particle, and the magnitude of the acceleration.

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