Force on a plane surface
Water pressure grows with depth: . On a flat gate, all the small pushes are square to the gate and add up to one force. It acts below the centroid, because the deeper part is pushed harder.
Total force
= vertical depth of the centroid, kN/m³.
Where it acts (centre of pressure)
and are measured along the slope from the water surface: .
Distance below the centroid
The deeper the gate, the smaller e.
Area, centroid, Ig and Ig/A of common gates
| Shape (height L measured along the slope) | Area A | Centroid from the bottom edge | Ig (about the centroid) | Ig/A |
|---|---|---|---|---|
| Rectangle b × L | ||||
| Triangle, base b at the bottom | ||||
| Triangle, base b at the top | ||||
| Circle, diameter D | ||||
| Semicircle, radius r | from the flat side | |||
| Trapezoid, b₁ bottom, b₂ top |
Hinged gates and lifted gates
Hinged gate: force P at the free edge
The water always tries to push the gate open (away from the water). P holds it closed, or opens it if the gate stays shut by itself.
Hinge reaction
Vertical gate lifted in guides
The water presses the gate on its guides, so friction μF resists the motion.
Force on a curved surface
Split the force into a horizontal part and a vertical part. They are easy to find separately.
Horizontal part
The force on the vertical projection of the curve. It acts at the centre of pressure of that projection.
Vertical part
The weight of the liquid directly above the curve, up to the surface. If the liquid is below the curve, use the imaginary liquid above it; FV then points up. It acts through the centroid of that volume.
Resultant
On a circular surface every push points to the centre, so the resultant passes through the centre. A Tainter gate hinged there feels no turning effect from the water.
Gate lab
Choose a gate, set the water depth above the bottom of the gate, and watch the pressure diagram and the forces. Drag the 3D view to look around.
Solution
Worked examples
A vertical gate 2 m wide and 3 m high has its bottom 5 m below the water surface. Find the total force and where it acts.
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A circular gate 1.2 m in diameter lies on a wall sloping at 60° from the horizontal. Its lowest point is 3 m below the water surface. Find the force and the centre of pressure.
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A vertical gate 1.5 m wide and 2 m high is hinged at its top edge. The water is 3 m deep above the bottom of the gate. Neglecting the gate weight, find the force P at the bottom edge needed to keep it closed.
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The hinge is 1 m below the surface, so the arm of F is 1.1667 m.
P = 34.34 kNA vertical gate 3 m wide and 2 m high weighs 20 kN. The water is 4 m deep above its bottom on one side and 1.5 m on the other. The friction coefficient on the guides is 0.2. What force is needed to raise the gate?
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A quarter-circle gate of radius 2 m and length 3 m bulges toward the water. The water surface is level with the top of the gate. Find the horizontal and vertical forces and the resultant.
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The water directly above the curve fills the square 2 m × 2 m minus the quarter circle:
F_H = 58.86 kN, F_V = 25.26 kN, F = 64.05 kN, through the centre of the circleA Tainter gate has a radius of 6 m and is hinged 4 m above the sill. It holds water 6 m deep. Find the forces per metre of length and show that the water makes no moment about the hinge.
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Below the hinge level the curved face looks down, so the water under it pushes up. Above the hinge level it looks up, so the water on it pushes down. Adding the slices along the arc gives a net upward force:
Every push points to the centre of the circle, so the resultant passes through the hinge:
F_H = 176.58 kN/m, F_V = 68.87 kN/m up, F = 189.54 kN/m through the hingeA cylinder 2 m in diameter holds back water 2 m deep on one side and 1 m deep on the other. Find the net forces per metre of length.
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Quiz: test yourself
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