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

Table 3

Velocity expressions of the two-dimensional problem.

	Velocity u	Velocity v
CASE 3	𝑢=0.1sin2𝜋𝑥+𝑦	𝑣=−0.1sin2𝜋𝑥+𝑦
CASE 4	𝑢=sin2𝜋𝑥+𝑦	𝑣=−sin2𝜋𝑥+𝑦