The vertical distance of the center of pressure below the c.g. of the inclined plane area (submerged in liquid) is

A

$$\frac{ I_{c.g.} \sin^{2} \theta}{A \overline{X}}$$

B

$$\frac{ I_{c.g.} \cos^{2} \theta}{A \overline{X}}$$

C

$$\frac{ I_{c.g.} \sin^{2} \theta}{ \overline{X}}$$

D

$$\frac{ I_{c.g.} \cos^{2} \theta}{ \overline{X}}$$