Hydrostatics: Forces on Surfaces

When a surface is submerged in a fluid, hydrostatic pressure acts perpendicular to the surface.

Force on Plane Surfaces

For a plane surface of area AA inclined at an angle θ\theta, the total hydrostatic force FF is:

F=γhˉAF = \gamma \bar{h} A

  • hˉ\bar{h} = Vertical depth to the centroid (CC) of the area.
  • FF acts at the Center of Pressure (CPCP), not the centroid.

Location of Center of Pressure (ypy_p): The distance measured along the inclined plane from the surface:

yp=yˉ+IxcyˉAy_p = \bar{y} + \frac{I_{xc}}{\bar{y}A}

  • yˉ\bar{y} = Distance to centroid along the incline (hˉ=yˉsinθ\bar{h} = \bar{y} \sin\theta)
  • IxcI_{xc} = Moment of inertia about the centroidal axis

Force on Curved Surfaces

The force is typically resolved into horizontal (FHF_H) and vertical (FVF_V) components.

Components of Force

Horizontal Component (FHF_H): The force on the vertical projection of the curved surface. FH=γhˉprojAprojF_H = \gamma \bar{h}_{proj} A_{proj}

Vertical Component (FVF_V): The weight of the fluid volume directly above the curved surface (real or imaginary). FV=γVaboveF_V = \gamma V_{above}

Resultant Force: R=FH2+FV2R = \sqrt{F_H^2 + F_V^2}

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