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See also:MANOMETER (Gr. µavos, thin or loose; µerpov, a measure) , an See also:instrument for measuring the pressures exerted by gases or vapours . An alternative name is pressure See also:gauge, but this See also:term may conveniently be restricted to manometers used in connexion with See also:steam-boilers, &c . The principle of hydro-See also:statics suggest the most See also:common forms . Suppose we have a U See also:tube (fig . 1), containing a liquid: if the pressures on the surfaces of the liquid be equal, then the surfaces will be at the same height . If, on the other See also:hand, the pressure in one See also:limb be greater than the pressure in the other, the surfaces will be at 2 Manoeuvres incidentally afford an excellent opportunity of testing new patterns of equipment, transport or other materiel under conditions approximating to those of active service . different heights. the difference being directly proportional to the difference of pressures. and inversely as the specific gravity of the liquid used . Two forms are in use: (I) the " open-tube," in which the pressure in one limb is equal to the atmospheric pressure, and (2) the' closed-tube," in which the experimental pressure is balanced against the liquid See also:column and the See also:air compressed into the upper See also:part of a closed limb of the tube . In the " open tube " See also:form (fig . I) the pressure on the See also:surface a is equal to the pressure on the surface at b (one atmos1,here) plus the hydrostatic pressure exerted by the liquid column of height a b . The liquid commonly used is See also:mercury . If a See also:scale be placed behind the limbs of the tube, so that the difference a b can be directly determined, then the pressure in a is at once expressible as P + a b in millimetres or inches of mercury, where P is the atmospheric pressure, known from an See also:ordinary barometric observation . In the " closed tube " form (fig . 2) the calculation is not so See also:simple, for the variation of pressure on the mercury surface in the closed limb has to be taken into See also:account . Suppose the length of the air column in the closed limb be h when the mercury is at the same height in both tubes . Applying the experimental pressure to the open end, if this be greater than atmospheric pressure the mercury column will rise and the air column diminish in the closed limb . I.et the length of the air column be h', then its pressure is h/h' atmospheres . The difference in height of the mercury columns in the two limbs is 2 (h-h'), and the pressure in the open limb is obviously equal to that of a column of mercury of length 2(h-h'), plus h/h' atmospheres . These See also:instruments are equally serviceable for deter-See also:mining pre. sores less than one See also:atmosphere . In laboratory practice, e.g. when it is required to determine the degree of exhaust of a See also:water See also:pump, a common form consists of a See also:vertical See also:glass tube having its See also:lower end immersed in a See also:basin of mercury, and its upper end connected by means of an intermediate See also:vessel to the exhaust . The mercury rises it the tube, and the difference between the barometric height and the length of the mercury column gives the pressure attained . |
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