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See also: Formulas for the Volumes of Some Common Solids (table)Formulas for the Volumes of Some Common Solids
Solid Volume1
cube l3
right rectangular parallelepiped lwh
prism Bh
right circular cylinder πr2h
pyramid 1-3Bh
..... Click the link for more information.


measure of solid content or capacity, usually expressed in units that are the cubes of linear units, such as cubic inches and cubic centimeters, or in units of dry and liquid measure, such as bushels, gallons, and liters. Volumes of complicated geometric forms are often calculated using integral calculuscalculus,
branch of mathematics that studies continuously changing quantities. The calculus is characterized by the use of infinite processes, involving passage to a limit—the notion of tending toward, or approaching, an ultimate value.
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. See the table entitled Formulas for the Volumes of Some Common SolidsFormulas for the Volumes of Some Common Solids
Solid Volume1
cube l3
right rectangular parallelepiped lwh
prism Bh
right circular cylinder πr2h
pyramid 1-3Bh
..... Click the link for more information.
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The following article is from The Great Soviet Encyclopedia (1979). It might be outdated or ideologically biased.



one of the fundamental quantities associated with geometric solids. In the simplest cases volume is measured by the number of unit cubes that can fit in the solid, that is, the number of cubes with an edge of unit length.

The problem of calculating the volumes of very simple solids stems from practical needs and was a stimulus to the development of geometry. The mathematics of the ancient East—Babylonia and Egypt—had a number of mostly empirical rules for calculating the volume of such frequently encountered solids as prismatic beams, whole and truncated pyramids, and cylinders. The volume formulas included inaccurate ones. The percentage error resulting from the use of inaccurate formulas was slight only within the limits of the linear dimensions commonly encountered in solids.

The Greek mathematicians of the last centuries before the Common Era freed the theory of volume calculation from approximate empirical rules. Euclid’s Elements and the works of Archimedes contain only exact rules for calculating the volumes of polyhedrons and certain round solids, namely, the cylinder, cone, sphere, and parts thereof. In their theory of volumes of polyhedrons, Greek mathematicians had to overcome the considerable difficulties that make this branch of geometry substantially different from the related branch dealing with the areas of polygons. Not until the early 20th century was the reason for this difference found. Using rectilinear cuts it is possible to dissect a polygon into parts that can be rearranged into a square. Dehn showed in 1901 that the analogous transformation of an arbitrary polyhedron into a cube by means of plane cuts is in general impossible. That is why, in establishing the formula for the volume of a tetrahedron, the simplest of all polyhedrons, Euclid had to resort to an infinite process of successive approximations—the method of exhaustion.

An infinite process also underlies the modern treatment of volume measurement. The modern approach considers all possible polyhedrons inscribed in the solid K and all possible polyhedrons circumscribed about K. The calculation of the volume of a polyhedron reduces to the calculation of the volume of the polyhedron’s constituent tetrahedrons. Let {Vi} be the set of volumes of the polyhedrons inscribed in K and {Vd} be the set of volumes of the polyhedrons circumscribed about K. The set {Vi} is bounded from above by the volume of any circumscribed polyhedron, and the set {Vd} is bounded from below by, for example, the number 0. The least upper bound of {Vi} is called the inner volume V̱ of K, and the greatest lower bound of {Vd} is called the outer volume V̱ of K. If $V coincides with V, then the number V = V = V is called the volume of K, and K is said to be Jordan measurable. A necessary and sufficient condition for a solid to be measurable is that for any positive number ∊ there exist a polyhedron circumscribed about the solid and a polyhedron inscribed in the solid such that the difference VdVi of their volumes is less than ∊.

Analytically, volume can be expressed by means of multiple integrals. Let the solid K (Figure 1) be bounded by a cylindrical surface with generators parallel to the z-axis, by the Jordan-measurable region M of the plane xOy, and by the surface

Figure 1

z = f(x, y), which is intersected by any line parallel to a generator of the cylinder at exactly one point. The volume of such a solid can be calculated by means of the double integral

V = ∫∫Mf (x, y) dxdy

The volume of a solid bounded by a closed surface that meets a line parallel to the z-axis at no more than two points can be calculated as the difference of the volumes of two solids of the kind just described. The volume of a solid can also be expressed by the triple integral

Figure 2

where the integration extends over the part of space occupied by the solid. Sometimes it is convenient to calculate the volume of a solid in terms of cross sections. Let a solid (Figure 2) lying between the planes z = a and z = b, b > a, be cut by planes perpendicular to the z-axis. If all cross sections of the solid are measurable and the cross-sectional area S is a continuous function of z, then the volume of the solid can be expressed by the simple integral

Historically, the operation of integration was actually used (in various geometric forms) to calculate the volumes of simple solids—the pyramid, the sphere, and some solids of revolution—long before the development of the integral calculus. Thus the way was prepared for the development of the integral calculus in the 17th and 18th centuries. In particular, Cavalieri’s principle, which is still important as a teaching device, contained formula (1) in embryonic form. Simpson’s rule, which is appropriate when the function S(z) in (1) is a polynomial of at most third degree, is also useful in elementary instruction.


Kudriavtsev, L. D. Matematicheskii analiz, vols. 1–2. Moscow, 1970.
Lebesgue, H. Ob izmerenii velichin, 2nd ed. Moscow, 1960. (Translated from French.)
The Great Soviet Encyclopedia, 3rd Edition (1970-1979). © 2010 The Gale Group, Inc. All rights reserved.


The intensity of a sound.
(computer science)
A single unit of external storage, all of which can be read or written by a single access mechanism or input/output device.
(engineering acoustics)
The magnitude of a complex audio-frequency current as measured in volume units on a standard volume indicator.
A measure of the size of a body or definite region in three-dimensional space; it is equal to the least upper bound of the sum of the volumes of nonoverlapping cubes that can be fitted inside the body or region, where the volume of a cube is the cube of the length of one of its sides. Abbreviated vol.
McGraw-Hill Dictionary of Scientific & Technical Terms, 6E, Copyright © 2003 by The McGraw-Hill Companies, Inc.


1. the magnitude of the three-dimensional space enclosed within or occupied by an object, geometric solid, etc.
2. fullness or intensity of tone or sound
3. History a roll or scroll of parchment, papyrus, etc.
Collins Discovery Encyclopedia, 1st edition © HarperCollins Publishers 2005


A physical storage unit. A volume can be a hard disk, SSD, removable disk cartridge, CD-ROM disc, floppy disk or reel of tape. See volume label and logical volume.
Copyright © 1981-2019 by The Computer Language Company Inc. All Rights reserved. THIS DEFINITION IS FOR PERSONAL USE ONLY. All other reproduction is strictly prohibited without permission from the publisher.
References in periodicals archive ?
End-diastolic volume versus pulmonary artery wedge pressure in evaluating cardiac preload in trauma patients.
Such changes were more pronounced in patients of the second group (compensated CPH) and were accompanied by an increase in the myocardial mass of the left ventricle and by a moderate increase in the end-diastolic volume and end-systolic volume.
Variable Acronym aortic pressure (mm Hg) AoP mean arterial pressure (mm Hg) MAoP cardiac output (mL/min) CO "contractible" volume of veins (mL) CVV sympathetic (inotropic) homeostatic Sy contractility modulation ejection fraction of the left ventricle EF end-diastolic volume of left ventricle (mL) EDVLV end-diastolic volume of section S2 of EDVS2 left ventricle end-diastolic pressure in left ventricle EDPLV (mm Hg) end-systolic volume of left ventricle (mL) ESVLV stroke volume of the left ventricle (mL) SVLV left atrial pressure (mm Hg) LAtP left ventricular pressure (mm Hg) LVP left ventricular volume (mL) LVV intrathoracic pressure (mm Hg) ITP
Relationship of wedge pressure to end-diastolic volume in patients undergoing myocardial revascularization.
(e) Analysis of CMRI reveals a normal RV end-diastolic volume (76 ml), reduced RV ejection fraction of 28%, and preserved left ventricular ejection fraction of 60%.
RV end-diastolic volume and end-systolic volume were calculated using Simpson's rule.
Both RV end-diastolic volume and RA volume decreased significantly in the control group during the follow-up period from 76.72 [+ or -] 27.56 to 59.39 [+ or -] 10.21 ml ( P < 0.001) and from 84.27 [+ or -] 32.68 to 43.21 [+ or -] 20.48 ml, respectively ( P < 0.001).
The following parameters were below the level in the control group: left ventricle end-systolic volume (LVESV), left ventricle end-diastolic volume (LVEDV), stroke volume (SV), cardiac output (Q), stroke volume index (SVI), left ventricle end-diastolic volume/left ventricular myocardial mass (LVEDV/LVMM), stroke index (SI), left ventricle diastolic function--maximum later peak velocity (peak A) (LVDF-[V.sub.a]), maximum blood flow velocity--aortic valve ([V.sub.max]-AoV), gradient (difference) of blood pressure--mitral valve ([Pg.sub.max]-MV), gradient (difference) of blood pressure--aortic valve ([Pg.sub.max]--AoV), and gradient (difference) of blood pressure - pulmonary valve ([Pg.sub.max]-PuV).
Systolic heart Diastolic heart failure failure LV remodeling Eccentric Concentric hypertrophy remodeling Concentric hypertrophy LV end-diastolic volume [up arrow] [right arrow] LV end-diastolic pressure [up arrow] [up arrow] LV ejection fraction [down arrow] [right arrow] LV dP/dt [down arrow] [right arrow] LV stiffness [right arrow] [up arrow] E/E' [up arrow] [up arrow] LA dilatation + + BNP or NT-proBNP [up arrow] [up arrow] LV: left ventricular; E/E': early mitral flow velocity/ early diastolic mitral annular velocity ratio; LA: left arterial; BNP: brain natriuretic peptide.
(7) progressive reduction in both left ventricular end-diastolic volume index and stroke volume with entry into microgravity was documented with echocardiography.
The 6-month results included a 25% reduction from baseline in left ventricular end-diastolic volume and a 19% decrease in left ventricular mass.
Similarly, the end-diastolic volume index dropped from 133 to 103 mL/[m.sup.2] in the CRT-on group but remained stable in controls.