The pressure in a liquid is a function of the depth alone. This is a fundamental fact about liquids.
Pressure function
The fluid pressure in a liquid is a function of depth:
In SI units:
The pressure of a fluid acts upon any surface in the fluid by exerting a force perpendicular to the surface. Force is pressure times area. If the pressure varies across the surface, the total force must be calculated using an integral to add up differing contributions of force on each portion of the surface.
Fluid force on submerged plate
Total fluid force on plate:
Use for top of plate (shallow) and for bottom of plate (deepest).
Have at the surface.
This formula assumes the plate is oriented straight vertically, not slanting.
Note that increases with depth, reverse from the usual -axis.
02 Illustration
Fluid force on a triangular plate
15 - Fluid force on a triangular plate
Find the total force on the submerged vertical plate with the following shape: Equilateral triangle, sides , top vertex at the surface, liquid is oil with density .
The moment of a region to an axis is the total (integral) of mass times distance to that axis:
“Moment to :”
“Moment to :”
Notice the swap in letters! has integral with while has integral with .
Because needs distance to -axis.
Notice that if you remove or factors from the integrands, the integrals give total mass .
These formulas are obtained by slicing the region into rectangular strips that are parallel to the axis in question.
The area per strip is then:
— region under
— region between and
— region ‘under’
— region between and
The idea of moment is related to:
Torque balance and angular inertia
Center of mass
The center of mass (CoM) of a solid body is a single point with two important properties:
“average position” of the body
The average position determines an effective center of dynamics. For example, gravity acting on every bit of mass of a rigid body acts the same as a force on the CoM alone.
“balance point” of the body
The net torque (rotational force) about the CoM, generated by a force distributed over the body’s mass, equivalently a force on the CoM, is zero.
Note:
When the body has uniform density, then the CoM is also called the centroid.
Center of mass from moments
Coordinates of the CoM:
Here and are the moments and is the total mass of the body.
Center of mass from moments - explanation
Notice how these formulas work. The total mass is always . The moment to (for example) is . Dividing these:
where .
In other words, through the formula , we find that is the average value of over the region with area .
A downside of the technique above is that to find we needed to convert the region into functions in . This would be hard to do if the region was given as the area under a curve but cannot be found analytically. An alternative formula that works in this situation.
Midpoint of strips for opposite variables
When the region lies between and , we can find with an -integral:
When the region lies between and , we can find with a -integral:
Use or for regions “under a curve” or .
The idea for these formulas is to treat each vertical strip as a point concentrated at the CoM of the vertical strip itself.
The height to this midpoint is , and the area of the strip is , so the integral becomes .
Midpoint of strips formula - full explanation
If the strip is located at some , with values from up to , then:
The area of the strip is . So the integral formula for can be recast:
If the vertical strips are between and , then the midpoints of the strips are given by the ‘average’ function:
Find the center of mass of the region which combines a rectangle and triangle (as in the figure) by computing separate moments. What are those separate moments? Assume the mass density is .
Solution
By symmetry, the center of mass of the rectangle is located at .