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in mechanics, ratio of the forceforce,
commonly, a "push" or "pull," more properly defined in physics as a quantity that changes the motion, size, or shape of a body. Force is a vector quantity, having both magnitude and direction.
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 acting on a surface to the area of the surface; it is thus distinct from the total force acting on a surface. A force can be applied to and sustained by a single point on a solid. However, a force can only be sustained by the surface of an enclosed fluid, i.e., a liquid or a gas. Thus it is more convenient to describe the forces acting on and within fluids in terms of pressure. Units of pressure are frequently force units divided by area units, e.g., pounds per square inch, dynes per square centimeter, or newtons (N) per square meter.

Pressure of Fluids

A fluid exerts a pressure on all bodies immersed in it. For a fluid at rest the difference in pressure between two points in it depends only upon the density of the fluid and the difference in depth between the two points. For example, a swimmer diving down in a lake can easily observe an increase in pressure with depth. For each meter (foot) increase in depth, the swimmer is subjected to an increase in pressure of 9,810 N per sq m (62.4 lb per sq ft), because water weighs 9,810 N per cu m (62.4 lb per cu ft). Since a liquid is nearly incompressible, its density does not change significantly with increasing depth. Therefore, the increase in pressure is caused solely by the increase in depth.

The variations in pressure of a gas are more complicated. For example, since air has such a low density compared to a liquid, a change in its pressure is only measurable between points that have a great height difference. The air pressure in a typical room is the same everywhere, but it is noticeably lower at the top of a mountain than at sea level. Because air is a gas, it is compressible. Its density decreases with increasing altitude. Thus changes in air pressure depend upon both the variations in the density of air and changes in the altitude at which it is measured. These two factors combine to reduce the air pressure at an altitude of 5,500 m (18,000 ft) to one half its value at sea level. Atmospheric (air) pressure at sea level will support a column of mercury that is about 76 cm (30 in.) high. The exact height varies with the weather. A unit called a standard atmosphere exerts a pressure equivalent to a column of mercury 76 cm high at sea level when the temperature is 0°C;; it is equal to 101,300 N per sq m (14.7 lb per sq in.).

Influences on and Effects of Pressure

Different gas lawsgas laws,
physical laws describing the behavior of a gas under various conditions of pressure, volume, and temperature. Experimental results indicate that all real gases behave in approximately the same manner, having their volume reduced by about the same proportion of the
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 relate the pressure of a gas to its volume, its temperature, or both. A rise in pressure affects both the melting pointmelting point,
temperature at which a substance changes its state from solid to liquid. Under standard atmospheric pressure different pure crystalline solids will each melt at a different specific temperature; thus melting point is a characteristic of a substance and can be used
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 and the boiling pointboiling point,
temperature at which a substance changes its state from liquid to gas. A stricter definition of boiling point is the temperature at which the liquid and vapor (gas) phases of a substance can exist in equilibrium.
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 of a substance, raising the melting and boiling points of most substances. In the case of water, however, an increase in pressure lowers its melting point so that the pressure of a skate blade on an ice surface causes the ice below it to be converted to the liquid state (see states of matterstates of matter,
forms of matter differing in several properties because of differences in the motions and forces of the molecules (or atoms, ions, or elementary particles) of which they are composed.
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; expansionexpansion,
in physics, increase in volume resulting from an increase in temperature. Contraction is the reverse process. When heat is applied to a body, the rate of vibration and the distances between the molecules composing it are increased and, hence, the space occupied by the
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). Bernoulli's principleBernoulli's principle,
physical principle formulated by Daniel Bernoulli that states that as the speed of a moving fluid (liquid or gas) increases, the pressure within the fluid decreases.
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 relates the effect of the velocity of a fluid on the pressure within the fluid.


A body immersed in a fluid experiences a larger upward pressure on its lower surface than a downward pressure on its upper surface because of the difference in height or depth between the two surfaces; this difference in pressure results in a buoyant force that pushes the body upward (see Archimedes' principleArchimedes' principle,
principle that states that a body immersed in a fluid is buoyed up by a force equal to the weight of the displaced fluid. The principle applies to both floating and submerged bodies and to all fluids, i.e., liquids and gases.
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). If the weight of the body is less than the buoyant force, the body will rise; if the weight is greater, the body will sink. The buoyant effect of this pressure may be noted in the rise of balloons or other objects filled with gases, such as hydrogen or helium, that are less dense than air.

Hydraulic Force

According to Pascal's lawPascal's law
[for Blaise Pascal], states that pressure applied to a confined fluid at any point is transmitted undiminished throughout the fluid in all directions and acts upon every part of the confining vessel at right angles to its interior surfaces and equally upon equal
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 the pressure exerted on an enclosed fluid is transmitted undiminished throughout the fluid and acts equally in all directions. On the basis of this law, various hydraulic devices are used to multiply a force. For example, a force of 10 N exerted on a piston whose area is 1 sq m and which is inserted into an enclosed chamber filled with water or another fluid transmits a pressure of 10 N per sq m throughout the fluid. If a second piston, at another part of the chamber, has an area of 10 sq m, then this pressure results in a force of 10 N being exerted on each square meter of its area, or 100 N total force.

Tools for Measuring Pressure

The instrument for measuring atmospheric pressure, the barometerbarometer
, instrument for measuring atmospheric pressure. It was invented in 1643 by the Italian scientist Evangelista Torricelli, who used a column of water in a tube 34 ft (10.4 m) long.
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, is calibrated to read zero when there is a complete vacuum; the pressure indicated by the instrument is therefore called absolute pressure. The term "pressure gauge" is commonly applied to the other instruments used for measuring pressure. They are manufactured in a great variety of sizes and types and are employed for recording pressures exerted by substances other than air—water, oil, various gases—registering pressures as low as 13.8×103 N per sq m (2 lb per sq in.) or as high as 13.8×107 N per sq m (10 tons per sq in.) and over (as in hydraulic presses). Some pressure gauges are made to carry out special operations, such as the one used on a portable air compressor. In this case, the gauge acts automatically to stop further operation when the pressure has reached a certain point and to start it up again when compression has fallen off to a certain limit.

In general, a gauge consists of a metal tube or diaphragm that becomes distorted when pressure is applied and, by an arrangement of multiplying levers and gears, causes an indicator to register the pressure upon a graduated dial. The Bourdon gauge used to measure steam pressure and vacuum consists essentially of a hollow metal tube closed at one end and bent into a curve, generally elliptic in section. The open end is connected to the boiler. As the pressure inside the tube (from the boiler) increases, the tube tends to straighten out. The closed end is attached to an indicating needle, which registers the extent to which the tube straightens out. For pressure too small to be accurately measured by the Bourdon gauge, the manometer is used. The simplest type of manometer consists of a U tube partially filled with a liquid (i.e., mercury), leaving one end open to the atmosphere and the other end to the source of pressure. If the pressure being measured is greater or less than atmospheric pressure, the liquid in the tube moves accordingly. Pressures up to several million lb per sq in. have been produced in experiments to determine the effect of high pressure on various substances.

The Columbia Electronic Encyclopedia™ Copyright © 2013, Columbia University Press. Licensed from Columbia University Press. All rights reserved.


The ratio of force to area. Atmospheric pressure at the surface of Earth is in the vicinity of 15 lbf/in.2 (1.0 × 105 Pa). Pressures in enclosed containers less than this value are spoken of as vacuum pressures; for example, the vacuum pressure inside a cathode-ray tube is 10-8 mmHg, meaning that the pressure is equal to the pressure that would be produced by a column of mercury, with no force acting above it, that is 10-8 mm high. This is absolute pressure measured above zero pressure as a reference level. Inside a steam boiler, the pressure may be 800 lbf/in.2 (5.5 × 106 Pa) or higher. Such pressure, measured above atmospheric pressure as a reference level, is gage pressure, designated psig. See Pressure measurement

McGraw-Hill Concise Encyclopedia of Physics. © 2002 by The McGraw-Hill Companies, Inc.


The force per unit surface area at any point in a gas or liquid. The pressure of a gas is proportional to temperature and density: at constant temperature, as the density is increased the pressure increases accordingly. This law of classical physics does not apply to degenerate matter.
Collins Dictionary of Astronomy © Market House Books Ltd, 2006
The following article is from The Great Soviet Encyclopedia (1979). It might be outdated or ideologically biased.



a physical quantity characterizing the intensity of normal forces (perpendicular to the surface) with which one body acts on another’s surface (for example, the foundations of a building acting on the ground, a liquid acting on the walls of a vessel, and gas in the cylinder of a motor acting on the piston). If the forces are distributed uniformly over the surface, then the pressure ρ on any part of the surface i s p = F/S, where 5 is the area of the part and F is the sum of the forces applied perpendicular to it. If the distribution of forces is nonuniform, this equality gives the mean pressure on the given small area, whereas at the limit, with S tending toward zero, it gives the pressure at a given point. If the distribution of forces is uniform, the pressure at all points of the surface is the same; if the distribution is nonuniform, the pressure varies from point to point.

For a continuous medium, the concept of pressure at each point in the medium is similarly introduced; it plays an important part in the mechanics of liquids and gases. At any point in a quiescent liquid the pressure in all directions is the same;

Table 1. Conversion of units of pressure
 Nlm2barkgflcm2atmmm Hgmm H20
1 N/m2(Pascal).................110-51.01972 x 10-5;0.98692 x 10-5750.06 x 10-50.101972
1 bar = 106dynes/cm2.................10511.019720.98692750.061.01972 x 104
1 kgf/cm2 = 1 at.................0.980665 x 1050.98066510.96784735.56104
1 atm.................1.01325 x 1051.013251.033217601.0332 x 104
1 mm Hg (torr).................133.3221.33322 x 10-31.35951 x 10-31.31579 x10--3113.5951
1 mm H20.................9.806659.80665 x 10-5;10-49.67841 x 10-57.3556 x 10-41

this is true also of moving liquids or gases, if they may be considered ideal (frictionless). In a viscous liquid the value of the mean pressure for three mutually perpendicular directions is taken to be the pressure at a given point.

Pressure plays an important part in physical, chemical, mechanical, and biological phenomena.


In a gaseous medium pressure is associated with the transfer of momentum during collisions of thermally moving gas molecules with each other or with the surface of bodies adjacent to the gas. The pressure in gases, which may be called thermal, is proportional to the temperature (the kinetic energy of the particles). In condensed mediums (liquids and solids), unlike gases, in which the mean distances between randomly moving particles are much greater than the size of the particles themselves, interatomic distances are comparable to atomic dimensions and are determined by the equilibrium of interatomic (intermolecular) forces of repulsion and attraction. When atoms approach one another repulsion forces increase, bringing about so-called cold pressure. In condensed mediums the pressure also has a “thermal” component, which is associated with the thermal vibrations of the atoms (nuclei). Given a steady or diminishing volume of a condensed medium, the thermal pressure rises as the temperature increases. At temperatures of about 104 ° K or more, thermal excitation of electrons makes an appreciable contribution to the thermal pressure.

Pressure is measured with manometers, barometers, and vacuometers, as well as with various pressure sensors.

Units of pressure have the dimensions of force divided by area. In the International System of Units, the unit of pressure is the newton per sq m (N/m2); in the Mks system, it is the kilogram-force per sq cm (kgf/cm2). Subsidiary units of pressure also exist—for example, the physical atmosphere (atm), the technical atmosphere (at), the bar, and mm of water and mercury columns (torr), by means of which the pressure measured is compared with the pressure of a column of liquid (water or mercury). (See Table 1.)

In the USA and Great Britain pressure is expressed in pounds-force per square inch (lbf/in.2), poundals per square foot (pdl/ft2), inches of water (in. H20), feet of water (ft H20), and inches of mercury (in. Hg); 1 lbf/in.2 = 6,894.76 N/m2; 1 pdl/ft2 = 1.48816 N/m2; 1 in. H20 = 249.089 N/m2; 1 ft H20 =2,989.07 N/m2; 1 in. Hg = 3,386.39 N/m2.


The Great Soviet Encyclopedia, 3rd Edition (1970-1979). © 2010 The Gale Group, Inc. All rights reserved.


A type of stress which is exerted uniformly in all directions; its measure is the force exerted per unit area.
McGraw-Hill Dictionary of Scientific & Technical Terms, 6E, Copyright © 2003 by The McGraw-Hill Companies, Inc.


The force per unit area exerted by a homogeneous liquid or gas on the walls of its container.
McGraw-Hill Dictionary of Architecture and Construction. Copyright © 2003 by McGraw-Hill Companies, Inc.


1. the normal force applied to a unit area of a surface, usually measured in pascals (newtons per square metre), millibars, torr, or atmospheres.
Collins Discovery Encyclopedia, 1st edition © HarperCollins Publishers 2005
References in periodicals archive ?
This will likely make us defensive in our practice and in so doing, we will be forced to improve our cuff pressure management.
ETT Cuff Pressure. The primary outcome of the study was to determine the proportion of cuff pressures in the optimal range from either group.
Automatic MAP was then determined from the cuff pressure associated with the peak of the fitted polynomial curve, and automatic SBP and DBP from the cuff pressures associated with the thresholds of 0.5 and 0.7, respectively, crossing the fitted polynomial curve, as shown in Figure 2.
It is noted that the oscillometric peak setting is not time dependent, and it is cuff pressure dependent.
High cuff pressures while using a classical LMA decrease mucosal perfusion; thus increasing the incidence of post-operative airway morbidity [2].
In a recent study regarding cuff pressure management, 53% of nurses checked the cuff pressure only every 8 hours and frequently only by using finger pressure to check the balloon (Lizy, Swinnen, Labeau, & Blot, 2011).
First, the maximum exercise heart rate (H[R.sub.max]) was compared across cuff pressures. Using the Kolmogorov-Smirnoff test for normality, all p-values were greater than 0.05, indicating the normality assumption for repeated measures ANOVA was met.
indicated that there was no difference in occurrence of pharyngeal complications for patients using LMA under high or low intracuff pressure.[sup][16],[17] The relationship between the cuff pressure and the pharyngeal morbidities has not been yet clearly elucidated by now.
Therefore, we hypothesized that the LMA cuff pressure limiting 25 cm[H.sub.2]O could reduce the postoperative pharyngolaryngeal adverse events, compared with 60 cm[H.sub.2]O by the manufacturer, using LMA Supreme.
Postoperative complications after ETT and LMA are common; however, some studies have shown that the incidence of complications like sore throat following ETT usage is much higher than LMA.12 There are numerous case reports on the complications of LMA like sore throat, hoarseness, bleeding and nerve injury.13-15 The most important possible mechanism is high cuff pressure with N 0 usage during maintenance of anesthesia.16,17
Important intubation considerations for the anesthesiologist taking care of a singer include size of the tube, good view of the vocal folds (which should be relaxed) during tube placement, minimum attempts at intubation (preferably at first attempt), keeping the cuff pressure to minimum, preventing movement of the tube during surgery and during emergence from anesthesia, and prevention of aspiration in the perioperative period.
First, correlation coefficients were used to compare the estimated and measured cuff pressure. Although we can argue that measured cuff pressure represents a gold standard, its accuracy will still depend on the accuracy of the device and the technique to use the device including the error rate and calibration of the device and equilibrium time needed to optimise the accuracy of the device.