A Treatise on Analytical Statics, with Numerous ExamplesMacmillan and Company, 1853 - 318 sider |
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Side 3
... remain the same . The cause of this undeviating effect is assumed to be an affinity which all bodies have for the earth , and is termed the force of attraction . If the body be prevented from falling by the interposition of a table or ...
... remain the same . The cause of this undeviating effect is assumed to be an affinity which all bodies have for the earth , and is termed the force of attraction . If the body be prevented from falling by the interposition of a table or ...
Side 6
... remain at rest . This force , which is equivalent in its effect to the combined effect of the original forces , is called their resultant , and the original forces are called the components of the resultant . It will be necessary , then ...
... remain at rest . This force , which is equivalent in its effect to the combined effect of the original forces , is called their resultant , and the original forces are called the components of the resultant . It will be necessary , then ...
Side 7
... angles BAC , CAD , DAB each equal to 120 ° ; the particle will remain at rest , for there 18 no reason why it should move in one direction rather than another . Each of the forces is therefore equal and FORCES IN THE SAME LINE . 7.
... angles BAC , CAD , DAB each equal to 120 ° ; the particle will remain at rest , for there 18 no reason why it should move in one direction rather than another . Each of the forces is therefore equal and FORCES IN THE SAME LINE . 7.
Side 18
... remain on a given smooth curve . By a smooth curve we understand a curve that can only exert force on the particle in a direction normal to the curve at the point of contact . Let X , Y , Z denote the forces acting on the particle in ...
... remain on a given smooth curve . By a smooth curve we understand a curve that can only exert force on the particle in a direction normal to the curve at the point of contact . Let X , Y , Z denote the forces acting on the particle in ...
Side 19
... remain on a given smooth surface . A smooth surface is one which can exert no force on the particle except in a direction normal to the surface . Let X , Y , Z denote the forces acting on the particle in directions parallel to three ...
... remain on a given smooth surface . A smooth surface is one which can exert no force on the particle except in a direction normal to the surface . Let X , Y , Z denote the forces acting on the particle in directions parallel to three ...
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A Treatise on Analytical Statics: With Numerous Examples Isaac Todhunter Uten tilgangsbegrensning - 1866 |
A Treatise on Analytical Statics: With Numerous Examples Isaac Todhunter Uten tilgangsbegrensning - 1866 |
A Treatise on Analytical Statics, with Numerous Examples Isaac Todhunter Uten tilgangsbegrensning - 1853 |
Vanlige uttrykk og setninger
angle attracted particle axes axis beam Cambridge centre of gravity circle coefficient of friction conditions of equilibrium cone constant coordinates cose cosß cosy couple Crown 8vo curve cylinder denote density displacement distance ds ds dx dy dz elastic string element ellipsoid equal equation equi find the centre fixed point forces acting frustum Hence horizontal plane inclined plane latus rectum law of attraction length lever mass origin P₁ P₂ parabola parallel forces passing point of application position of equilibrium pressure PROP pullies radius resolved rest resultant attraction rigid body round shell shew sine single force single resultant smooth solid sphere spheroid straight line suppose surface system of forces tangent tension triangle uniform vanish vertex virtual velocity weight ΣΖ ΣΡ ΣΥ ΣΧ
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Side 12 - Prize Essay for 1877. 8vo. 8.r. 6V. SMITH— Works by the Rev. BARNARD SMITH, MA, Rector of Glaston, Rutland, late Fellow and Senior Bursar of St. Peter's College, Cambridge. ARITHMETIC AND ALGEBRA, in their Principles and Application ; with numerous systematically arranged Examples taken from the Cambridge Examination Papers, with especial reference to the Ordinary Examination for the BA Degree.
Side 9 - Geometry. With a numerous collection of Easy Examples progressively arranged, especially designed for the use of Schools and Beginners. By G. HALE PUCKLE, MA, St. John's College, Cambridge, Mathematical Master in the Royal Institution School, Liverpool.
Side 7 - TODHUNTER.— A Treatise on the Differential Calculus ; and the Elements of the Integral Calculus. With numerous Examples. By I. TODHUNTER, MA, Fellow and Tutor of St. John's College, Cambridge. Second Edition. Crown 8vo. cloth, 10».
Side 13 - Problems proposed in the Senate House Examination, January 1854. By the Moderators (W. WALTON, MA Trinity College, and CF MACKENZIE, MA Fellow of Caius College). In 8vo. cloth, 10*.
Side 6 - The Evidences of Christianity as Exhibited in the Writings of its Apologists down to Augustine. An Essay which obtained the Hulsean Prize for the Year 1852. By WJ BOLTON, of Gonville and Caius College, Cambridge. 8vo. cloth, 6s.
Side 4 - Archer).— Works by the Rev. WILLIAM ARCHER BUTLER, MA, late Professor of Moral Philosophy in the University of Dublin : SERMONS, DOCTRINAL AND PRACTICAL. Edited, with a Memoir of the Author's Life, by THOMAS WOODWARD, Dean of Down.
Side 13 - FROST.— The First Three Sections of Newton's Principia. With Notes and Problems in illustration of the subject. By PERCIVAL FROST, MA late Fellow of St.
Side 4 - Present a richer combination of the qualities for Sermons of the first class than any we have met with in any living writer.