A Collection of Problems in Illustration of the Principles of Theoretical MechanicsDeighton, Bell, 1876 - 667 páginas |
Dentro del libro
Resultados 1-5 de 53
Página vii
... moving Particle on immoveable Plane Curves 313 • III . Motion of a Particle on Rough Plane Curves 324 IV . Inverse Problems on the Motion of a Particle along im- moveable Plane Curves 325 V. VI . Inverse Problems on the Pressure of a ...
... moving Particle on immoveable Plane Curves 313 • III . Motion of a Particle on Rough Plane Curves 324 IV . Inverse Problems on the Motion of a Particle along im- moveable Plane Curves 325 V. VI . Inverse Problems on the Pressure of a ...
Página 25
... moving parallel to itself along an axis perpendicular to its plane through its centre ; one side of the rectangle varies as the distance from a fixed point in the axis , while half the other is the sine of a circular arc , of which this ...
... moving parallel to itself along an axis perpendicular to its plane through its centre ; one side of the rectangle varies as the distance from a fixed point in the axis , while half the other is the sine of a circular arc , of which this ...
Página 104
... moving freely about the angular points A , B , C , D , ... ; to determine the form of the polygon that it may be in equi- librium , the lengths of the sides being given . p , q , r , s , Let denote the mutual actions of the sides of the ...
... moving freely about the angular points A , B , C , D , ... ; to determine the form of the polygon that it may be in equi- librium , the lengths of the sides being given . p , q , r , s , Let denote the mutual actions of the sides of the ...
Página 116
... moving force of the element Pp , will be mXds , m Yds , mZds . Hence for the equilibrium of Pp we must have , equating to zero the sum of the resolved forces which act upon it parallel to each of the three axes , and dividing the 116 ...
... moving force of the element Pp , will be mXds , m Yds , mZds . Hence for the equilibrium of Pp we must have , equating to zero the sum of the resolved forces which act upon it parallel to each of the three axes , and dividing the 116 ...
Página 157
... In order to determine S , conceive each point of the rod to receive the same vertical displacement B , the point B thus sliding along CD and the rod moving parallel to itself . L Then , putting BOE = p , the virtual VIRTUAL VELOCITIES .
... In order to determine S , conceive each point of the rod to receive the same vertical displacement B , the point B thus sliding along CD and the rod moving parallel to itself . L Then , putting BOE = p , the virtual VIRTUAL VELOCITIES .
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Términos y frases comunes
absolute force acted angular velocity attraction axes axis beam body catenary centre of force centre of gravity circle co-ordinates coefficient of friction cos² curve cycloid cylinder denote density descends determine distance dt dt dt² dx dy dx² elastic ellipse equal equation Euler find the centre fixed point hence horizontal plane inclined plane inertia integrating James Bernoulli John Bernoulli lamina mass middle point moment of inertia motion natural length oscillation parabola perpendicular position of equilibrium pressure radius of gyration radius vector resolving forces rest right angles SECT sin² smooth sphere square straight line string supposing surface taking moments tangent tension triangle tube uniform rod varying inversely vertex vertical plane Vis Viva weight
Pasajes populares
Página 203 - A centre of force attracting inversely as the square of the distance is at the centre of a spherical cavity within an infinite mass of liquid, the pressure on which at an infinite distance is...