Elements of Mechanics: For the Use of Colleges, Academies, and High SchoolsA.S. Barnes & Burr, 1859 - 338 pages |
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Page 22
... suppose m to be equal to 1 , we shall have , f = v . That is , the measure of an impulse is the velocity which it can impart to a unit of mass . An incessant force is made of a succession of impulses . It has been agreed to take , as ...
... suppose m to be equal to 1 , we shall have , f = v . That is , the measure of an impulse is the velocity which it can impart to a unit of mass . An incessant force is made of a succession of impulses . It has been agreed to take , as ...
Page 23
... suppose m to be equal to 1 , we shall have , ƒ = v . That is , the measure of an incessant force is the velocity which it can generate in a unit of mass in a unit of time . If the force is of such a nature as to act equally upon every ...
... suppose m to be equal to 1 , we shall have , ƒ = v . That is , the measure of an incessant force is the velocity which it can generate in a unit of mass in a unit of time . If the force is of such a nature as to act equally upon every ...
Page 27
... suppose the material point O , to be acted upon simul- taneously by the two forces P and Q , it will , by virtue of the first , be found at the end of one second somewhere on the line PR ; and by virtue of the second somewhere on the ...
... suppose the material point O , to be acted upon simul- taneously by the two forces P and Q , it will , by virtue of the first , be found at the end of one second somewhere on the line PR ; and by virtue of the second somewhere on the ...
Page 45
... suppose the points of application to be transferred to O , their resultant may be deter- M Fig . 19 . mined by the parallelogram of forces . The direction of the resultant will pass through O. ( Art . 28. ) Whether the forces be ...
... suppose the points of application to be transferred to O , their resultant may be deter- M Fig . 19 . mined by the parallelogram of forces . The direction of the resultant will pass through O. ( Art . 28. ) Whether the forces be ...
Page 52
... Suppose each force resolved into three components , re- spectively parallel to the co - ordinate axes , the points of application being unchanged : The components parallel to the axis of X are , Pcosa , P'cosa , P''cosx , & c . , Rcosa ...
... Suppose each force resolved into three components , re- spectively parallel to the co - ordinate axes , the points of application being unchanged : The components parallel to the axis of X are , Pcosa , P'cosa , P''cosx , & c . , Rcosa ...
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Common terms and phrases
A. S. BARNES algebraic sum angular velocity atmosphere axes axle body called centre of gravity centrifugal force cistern components cord cubic cubic foot curve cylinder denote the angle distance elementary entire equal Equation equilibrium exerted feet fluid force applied force of gravity forces acting friction fulcrum Hence horizontal hydrometer inches inclined plane inertia instrument lever arm liquid machine mass mercury moment of inertia moments motion orifice parallel forces parallelogram parallelogram of forces particles passing Pcosa pendulum perpendicular pipe piston point of application polygon position power and resistance pressure principle principle of moments pulley pump quantity radius radius of gyration represent reservoir respect resultant right angles rope rotation Schools screw SOLUTION space specific gravity square steam Substituting suppose temperature tension tion triangle tube unit upper surface vertex vertical vessel vibration volume weight wheel whence
Popular passages
Page 182 - ... plus the product of the area and the square of the distance between the axes.
Page 223 - This electromotive force may be resolved into two components, one parallel and the other perpendicular to I, as shown, for example, in Fig.
Page 114 - The power is to the weight, as the radius of the pulley is to the chord of the arc enveloped by the rope.
Page 39 - Lami's Theorem. If three forces acting on a particle keep it in equilibrium, each is proportional to the sine of the angle between the other two.
Page 7 - BOURDON'S ALGEBRA 1 50 KEY TO DAVIES' BOURDON'S ALGEBRA 1 50 DAVIES' LEGENDRE'S GKOMETRY 1 50 DAVIES' ELEMENTS OF SURVEYING 1 50 DAVIES' ANALYTICAL GEOMETRY 1 25 DAVIES' DIFFERENTIAL AND INTEGRAL CALCULUS 1 25 DAVIES' DESCRIPTIVE GEOMETRY 2 00 DAVIES...
Page 42 - Hence, the moment of the resultant of two forces is equal to the algebraic sum of the moments of the forces taken separately. 53. Forces Acting at Different Points. Parallel Forces.— We have thus far considered forces acting upon a single particle, or upon one point of a body. If, how- Fia 33...
Page 180 - ... must be measured on a line at right angles to the direction of the force. Moment of Inertia. The moment of inertia of a body, with respect to an axis, is the sum of the products obtained by multiplying the mass of each elementary particle by the square of its distance from the axis; hence, the moment of inertia of the same body varies according to the position of the axis.
Page 5 - ... feet. Thus it appears, that it requires a force to lift the piston exactly equal to the weight of a column of water, whose base is equal to the section of the piston, and whose height...
Page 8 - JOHN A.* PORTER, AM. MD, Professor of Agricultural and Organic Chemistry in Yale College. Price $1.00. These works have been prepared expressly for Public and Union Schools, Academies, and Seminaries, where an extensive course of study on this subject and expensive apparatus was not desired, or could not be afforded. A fair, practical knowledge of Chemistry is exceedingly desirable, and almost a necessity, at tho present day, but it has been...