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hydrostatics

   Also found in: Dictionary/thesaurus, Medical, Wikipedia, Hutchinson 0.03 sec.
hydrostatics: see mechanics mechanics, branch of physics concerned with motion and the forces that tend to cause it; it includes study of the mechanical properties of matter , such as density , elasticity , and viscosity .
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hydrostatics

Branch of physics that deals with the characteristics of fluids at rest, particularly with the pressure in a fluid or exerted by a fluid (gas or liquid) on an immersed body. In applications, the principles of hydrostatics are used for problems relating to pressure in deep water (pressure increases with depth) and high in the atmosphere (pressure lessens with altitude).


hydrostatics
the branch of science concerned with the mechanical properties and behaviour of fluids that are not in motion

hydrostatics [‚hī·drə′stad·iks]
(fluid mechanics)
The study of liquids at rest and the forces exerted on them or by them.

Hydrostatics

The study of liquids at rest. In the absence of motion, there are no shear stresses; the internal state of stress at any point is determined by pressure alone. Hence, the pressure at a point is the same in all directions. Pressure acts normally to all boundary surfaces. For equilibrium under gravity, regardless of the shape of the containing vessel, the pressure is uniform over any horizontal cross section. Pressure varies with height or depth. Two different reference levels are used in measuring pressure. For many engineering purposes, gage pressure is used with pressure measured relative to atmospheric pressure as zero. For most scientific purposes, pressure is referred to true zero. Normal atmospheric pressure at sea level caused by the weight of the air above is approximately 101 kilopascals or 14.7 pounds per square inch absolute.

The buoyant force is the force exerted vertically upward by a fluid on a body wholly or partly immersed in it. Its magnitude is equal to the weight of the fluid displaced by the body. This value is also the vertical component of the fluid pressure force acting upward against the bottom of the body minus the fluid pressure force component (if any) acting vertically downward against the top of the body. If this buoyant force equals the weight of the body, the body will remain at the given level. If it exceeds the weight of the body, the latter will rise, and vice versa. The buoyant force as a single magnitude acts vertically upward through the center of buoyancy which is the center of gravity of the displaced fluid. See Archimedes' principle

Pressure applied to a confined liquid is transmitted with equal intensity throughout the liquid and by it to all surfaces of the confining vessel or piping. Hence, a small force applied to a small area of a confined liquid can create a large force against a large area. If the small and large areas are pistons, the device may be a hydraulic press or jack. Because the transmitting liquid is practically incompressible and its volume virtually constant, the linear movement of the large piston will be to that of the small piston in inverse proportion to their areas. The principle of multiplying a force by means of liquid pressure applies also to hydraulic brakes, power steering, control systems, and the like; the actuating force may be a pump instead of a small piston.



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6) Aquatic physical therapy incorporates individual assessment, evidence-based practice, and clinical reasoning skills to devise treatment plans based on the principles of hydrostatics and hydrodynamics and the physiologic effects of immersion.
52) Over the course of the 1840s, he lectured on current events, scientific and political topics, ancient and modern governments, "The Progression of Man" from his savage state to the present, and "The Life, Times, and Doings of Socrates"; he also published A Journey Up the Mississippi as well as popular science articles on hydrostatics and Archimedes and poetry.
For example, he notes their common interest in exploring the relation between a mover and moved in both natural and violent motions and the application of a mechanical principle to the analysis of motion, although Galileo used Archimedes' hydrostatics rather than pseudo-Aristotelian circular motion.
 
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