To find the normal reaction on point A, we need to understand the equilibrium condition of the rod supported by two knife edges.
R_A + R_B = W
R_A \cdot d = W \cdot (d - a)
R_A = \frac{W(d - a)}{d}
This reasoning correctly identifies the moments and balances the forces, illustrating how the normal reaction is distributed based on the center of mass location.
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 