The Mechanical Principles of Engineering and ArchitectureLongman, Brown, Green, and Longmans, 1855 - 675 стор. |
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Сторінка iii
... Cylinder ; " thirdly , " On the descent of a body upon an inclined plane , when subjected to variations of temperature , which would otherwise rest upon it ; " fourthly , " On the state bor- dering upon motion of a body moveable about a ...
... Cylinder ; " thirdly , " On the descent of a body upon an inclined plane , when subjected to variations of temperature , which would otherwise rest upon it ; " fourthly , " On the state bor- dering upon motion of a body moveable about a ...
Сторінка xxiii
... Cylinder · 607 608 613 629 • 631 Note F. - On the Descent upon an Inclined Plane of a Body sub- ject to Variations of Temperature , and on the Motion of Glaciers Note G. - The best Dimensions of a Buttress · 651 659 660 Note H ...
... Cylinder · 607 608 613 629 • 631 Note F. - On the Descent upon an Inclined Plane of a Body sub- ject to Variations of Temperature , and on the Motion of Glaciers Note G. - The best Dimensions of a Buttress · 651 659 660 Note H ...
Сторінка 86
... cylinder about its axis of symmetry . Let AB be the axis of such a cylinder , whose radius AC is represented by a , and its height by b . Con- ceive the cylinder to be made up of cylindrical rings having the same axis ; let AP = p be ...
... cylinder about its axis of symmetry . Let AB be the axis of such a cylinder , whose radius AC is represented by a , and its height by b . Con- ceive the cylinder to be made up of cylindrical rings having the same axis ; let AP = p be ...
Сторінка 87
... cylinder PR , which is taken from this solid to form the hollow cylinder , would be ba1 . Now let I represent the moment of inertia of the hollow cylinder CP , therefore I + { πbа „ ^ = { } πbα ̧ * , B 2 ` . I = } πb ( a‚1 — a‚1 ) ...
... cylinder PR , which is taken from this solid to form the hollow cylinder , would be ba1 . Now let I represent the moment of inertia of the hollow cylinder CP , therefore I + { πbа „ ^ = { } πbα ̧ * , B 2 ` . I = } πb ( a‚1 — a‚1 ) ...
Сторінка 88
... cylinder of very small height , B R its moment of inertia about AB ( equation 64 ) is represented by yAx . Now the moment of inertia I of the whole cone is equal to the sum of the moments of all such elements , • ;. I = } πΣy1Ax . Let ...
... cylinder of very small height , B R its moment of inertia about AB ( equation 64 ) is represented by yAx . Now the moment of inertia I of the whole cone is equal to the sum of the moments of all such elements , • ;. I = } πΣy1Ax . Let ...
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Загальні терміни та фрази
a₁ angle of resistance angular velocity arch axes axis beam body bordering upon motion capstan centre of gravity circumference compression corresponding crank curve cylinder deflexion descend determined dimensions displaced fluid distance ditto driven wheel driving Edition epicycloidal equal equation equilibrium evident exceedingly small extrados force formula friction given hypocycloidal impact inclination inertia intersect involute lamina length limiting angle line of centres line of resistance machine modulus moment of inertia moving numbers of teeth observing obtain oscillation P₁ P₂ parallel passing perpendicular pitch circle plane point of application point of contact portion position radius repre respect resultant revolution revolve rupture screw space stability Substituting supposed surfaces of contact taken to represent tion tooth U₁ U₂ unguent vertical vis viva viva vols voussoirs W₁ wall weight whence it follows whilst whole
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