Principles of the Mechanics of Machinery and Engineering: Theoretical mechanics.-v. 2. Applied mechanicsLea and Blanchard, 1848 |
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Principles of the Mechanics of Machinery and Engineering: Theoretical mechanics Julius Weisbach Volledige weergave - 1848 |
Principles of the Mechanics of Machinery and Engineering: Theoretical mechanics Julius Weisbach Volledige weergave - 1848 |
Principles of the Mechanics of Machinery and Engineering: Theoretical mechanics Julius Weisbach Volledige weergave - 1848 |
Veelvoorkomende woorden en zinsdelen
ABCD accelerated motion axis of revolution axis XX axle base beam body breadth c₁ centre of gravity centrifugal force co-efficient components consequently cord corresponding cubic curve cylinder density described determined direction distance efflux elasticity equal equation equilibrium Example feet follows formula friction funicular G₁ G₂ h₁ H₂ head of water heights due hence horizontal impact inches inclined plane inertia inversely lastly line of gravity M₁ M₂ mass mean force mechanical effect moment of inertia obtain orifice oscillation P₁ P₂ parabola parallel parallelogram parallelogram of forces parallelopiped pendulum point of application pressure pulley pyramid Q₁ radius resistance resultant right angles S₁ Simpson's rule space specific gravity statical surface tang tension terminal velocity tion transverse section triangle uniformly accelerated V₁ vertical vis viva volume weight G wheel کے
Populaire passages
Pagina 204 - ... surface, and whose height is equal to the depth of the centre of gravity of the surface below the surface of the liquid.
Pagina 155 - Show that the moment of inertia of a body about any axis is equal to the moment of inertia about a parallel axis through the...
Pagina 231 - The heads are measured where the water may be considered still. TABLE II. — The Coefficients for the Efflux through rectangular orifices in a thin vertical plate, the heads of water being measured directly over the orifice.
Pagina 203 - The force which must be expended in order to raise the piston, is equal to the weight of a column of water, whose base is the section of the piston, and whose height is that to which the water is raised.
Pagina 167 - VI = 0,6324 . r ; two-fifths of the mass of the sphere, at a distance equal to the radius of the sphere from the axis of rotation, has the same moment of inertia as the entire sphere. The formula W=%M r...
Pagina 201 - It is evident that after each stroke of the pump the pressure on the piston and the force necessary to raise it will be increased by the weight of a column of water whose base is the horizontal section of the piston, and whose height is equal to the increase which the elevation of the column in CE receives from the water driven through the valve x.
Pagina 147 - Eider's theory, that the strength of pillars to bear incipient flexure is directly as the fourth power of the diameter, and inversely as the square of the length.
Pagina 211 - PC sm $ ; and this is, therefore, the greater, the greater the weight, the greater the distance of the metacentre from the centre of gravity of the ship, and the greater the angle of inclination of this last, § 289.
Pagina 182 - ... that of the centre of oscillation from the centre of gravity, but also...
Pagina 182 - ... the times of oscillation are as the square roots of the lengths of the pendulum.