Fundamentals of fl uid 1 gunt

Basic knowledge Fundamentals of hydrostatics

Hydrostatics is the study of fl uids at rest. The experimental units from GUNT cover and properties of fl uids Hydrostatic on walls Capillarity the basic principles of the following topics • • from the fi eld of hydrostatics: hydrostatic with Coriolis In addition to the ground pressure of a fl uid, it is often important in rise or fall due to manometers and pressure sensors pressure, , surface , • and forces to also know the hydrostatic pressure on boundary surfaces, for molecular forces between the and the capillarity/adhesion. • measurement example in order to calculate the forces acting on the side walls wall or between the liquid and air. The height • buoyancy forces (channel, aquarium etc.) or on weirs. of rise in the depends on the surface • vapour pressure curve • hydrostatic pressure and tension and the diameter of the capillary. • change of state of the resultant forces In wetting liquids (e.g. water) the surface level in the capillary rises. In non-wetting liquids (e.g. mercury) the level falls.

250 250 Hydrostatic pressure 200 200 The pressure in fl uids at rest does not depend on the

direction. It is linearly dependent on the amount of fl uid 150 150 over the element being studied, or the diving depth respectively. 100 100 The hydrostatic pressure for incompressible fl uids that F p 50 F 50 h are not subject to is calculated according to Pas- F cal’s law. h

A Pascal’s law The effect of a force F on a motionless liquid generates a pressure p within the liquid, which at any point acts equally in all directions. The pressure always acts perpen- dicular to the boundary surface A of the liquid. p=F/A All force and pressure processes in liquids are based on h level, F resultant force, A effective area, this law. pressure profi le, water level

Hydrostatic paradox Communicating vessels Stability of fl oating bodies The hydrostatic pressure generates a force F on the Communicating vessels are tubes that are open at the In order to be able to assess whether a body area A. If these areas are equal, this force only depends top and interconnected at the bottom. Regardless of the fl oats stably or could capsize, it is necessary to on the level h; the shape of the vessel is irrelevant. shape and size of the tubes, the level of the fl uid in them determine its metacentre M. The location of the is the same. metacentre depends on the centre of gravity Md of the displaced water A and the angle of heel. Applications include water levels, locks and drain traps The body fl oats stably when the metacentre M z in sewers. is located above the centre of gravity S. Then M the restoring moment Md has a ‘righting’ effect. S The distance between the centre of gravity and A the metacentre is known as the metacentric height z.

h

FFF F AAAA M metacentre, S center of gravity, A center of buoyancy, z metacentric height, Md restoring moment that straightens the fl oating body back up, h level, F force, A area, red line level red line water level

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