# Fluid statics

(Redirected from Hydrostatic pressure)
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## Overview

Fluid statics (also called hydrostatics) is the science of fluids at rest, and is a sub-field within fluid mechanics. The term usually refers to the mathematical treatment of the subject. It embraces the study of the conditions under which fluids are at rest in stable equilibrium. The use of fluid to do work is called hydraulics, and the science of fluids in motion is fluid dynamics.

## Pressure in fluids at rest

Due to the inability to resist deformation, fluids exert pressure normal to any contacting surface. In addition, when the fluid is at rest that pressure is isotropic, i.e. it acts with equal magnitude in all directions. This characteristic allows fluids to transmit force through the length of pipes or tubes, i.e., a force applied to a fluid in a pipe is transmitted, via the fluid, to the other end of the pipe. If the forces are not balanced, the fluid will move in the direction of the resulting force.

This concept was first formulated, in a slightly extended form, by the French mathematician and philosopher Blaise Pascal in 1647 and would later be known as Pascal's law. This law has many important applications in hydraulics. Galileo Galilei, also was one of the fathers of hydrostatics.

### Hydrostatic pressure

Considering a small cube of liquid at rest below a free surface, the weight of the liquid above must be balanced by a pressure in this small cube. For an infinitely small cube the stress is the same in all directions and liquid weight or equivalent pressure can be expressed as

${\displaystyle \ P=\rho gh+P_{a}}$

where, using SI units,

P is the hydrostatic pressure (in pascals);

ρ is the liquid density (in kilograms per cubic metre);

g is gravitational acceleration (in metres per second squared);

h is the height of liquid above (in metres);

Pa is the atmospheric pressure (in pascals).

### Atmospheric pressure

The ideal gas law predicts that, for a gas of constant temperature, T, its density, ρ, will vary with height, h, as:

${\displaystyle \ \rho \ (h)=\rho \ (0)e^{-Mgh/RT}}$

where:

g = the acceleration due to gravity
T = Absolute Temperature (eg degrees Kelvin)
R = Ideal gas constant
M = Molar mass
ρ = Density
h = height

## Buoyancy

A solid body immersed in a fluid will have an upward buoyant force acting on it equal to the weight of displaced fluid. This is due to the hydrostatic pressure in the fluid.

In the case of a container ship, for instance, its weight force is balanced by a buoyant force from the displaced water, allowing it to float. If more cargo is loaded onto the ship, it would sit lower in the water - displacing more water and thus receive a higher buoyant force to balance the increased weight force.

Discovery of the principle of buoyancy is attributed to Archimedes.

### Stability

A floating object is stable if it tends to restore itself to an equilibrium position after a small displacement. For example, floating objects will generally have vertical stability, as if the object is pushed down slightly, this will create a greater buoyant force, which, unbalanced against the weight force will push the object back up.

Rotational stability is of great importance to floating vessels. Given a small angular displacement, the vessel may return to its original position (stable), move away from its original position (unstable), or remain where it is (neutral).

Rotational stability depends on the relative lines of action of forces on an object. The upward buoyant force on an object acts through the centre of buoyancy, being the centroid of the displaced volume of fluid. The weight force on the object acts through its centre of gravity. An object will be stable if an angular displacement moves the line of action of these forces to set up a 'righting moment'. See also Angle of loll.

## Liquids-fluids with free surfaces

Liquids can have free surfaces at which they interface with gases, or with a vacuum. In general, the lack of the ability to sustain a shear stress entails that free surfaces rapidly adjust towards an equilibrium. However, on small length scales, there is an important balancing force from surface tension.

### Surface tension effects

#### Capillary action

When liquids are constrained in vessels whose dimensions are small, compared to the relevant length scales, surface tension effects become important leading to the formation of a meniscus through capillary action. This capillary action has profound consequences for biological systems as it is part of on of the two driving mechanisms of the flow of water in plant xylem, the transpirational pull.

#### Drops

Without surface tension, drops would not be able to form. The dimensions and stability of drops are determined by surface tension.