Study on the Convective Term Discretized by Strong Conservation and Weak Conservation Schemes for Incompressible Fluid Flow and Heat Transfer

Table 2

Flow area and velocity expressions of the one-dimensional problem.

	Flow area	Velocity u
CASE 1	𝐴=−sin(𝜋𝑥/2)+1.5	𝑢= 0.2/(−sin(𝜋𝑥/2)+1.5)
CASE 2	𝐴=4(−sin(𝜋𝑥/2)+1.01)	𝑢= 0.05/(−sin(𝜋𝑥/2)+1.01)