Applied Mechanics, Volume 1John Wiley, 1913 |
Table des matières
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Autres éditions - Tout afficher
Applied Mechanics, Volume 1 Charles Edward Fuller,William Atkinson Johnston Affichage du livre entier - 1913 |
Applied Mechanics, Volume 1 Charles Edward Fuller,William Atkinson Johnston Affichage du livre entier - 1915 |
Applied Mechanics, Volume 1 Charles Edward Fuller,William Atkinson Johnston Affichage du livre entier - 1915 |
Expressions et termes fréquents
acceleration algebraic sum angle angular velocity applied assuming attraction axis of rotation center of gravity center of percussion compression conditions of equilibrium constant cos² couple cylinder determine deviating force diameter displacement elementary equal to zero equation evident F₂ force F formula friction Hence horizontal impact instant kinetic energy line of action M₁ M₂ mass moment of inertia moments of inertia motion of translation obtain parallel forces parallel to OX path perpendicular distance plane point of application position potential energy Problem product of inertia pulley r₁ radius resolved respect resultant force revolutions per minute rigid body secs sin² solid Solution speed sphere stress Substituting system of forces tangential component tension tion triangle unit unknown forces v₁ vector sum vertical weight wheel ΣΜ ΣΥ ΣΧ
Fréquemment cités
Page 3 - I. — Every body continues in its state of rest or of uniform motion in a straight line, except in so far as it is compelled by force to change that state.
Page 11 - If three forces acting at a point are in equilibrium they can be represented in magnitude and direction by the three sides of a triangle taken in order.
Page 3 - To every action there is always an equal and contrary reaction; or, the mutual actions of any two bodies are always equal and oppositely directed in the same straight line.
Page 20 - moment of a force" with respect to a point is the product of the force and the perpendicular distance from the given point to the line of action of the force.
Page 134 - Expressed in words, this equation states that the polar moment of inertia for an area, with respect to an axis perpendicular to its plane, is equal to the sum of the moments of inertia about any two mutually perpendicular axes in its plane that intersect on the polar axis.
Page 125 - ... solid thus generated is equal to the product of the revolving area and the path described by the center of gravity of the plane area during the revolution.
Page 18 - If three forces, acting at a point, be represented in magnitude and direction by the sides of a triangle taken in order, they will be in equilibrium.
Page 165 - Steiner. is true for bath a plane laminar body and a thin three-dimensional body, and states that the moment of inertia of a body about any axis is equal to its moment of inertia about a parallel axis through its...
Page 107 - Their points of application remain the same. 2°. Their relative magnitudes are unchanged. 3°. They remain parallel to each other. Hence, in finding the centre of a set of parallel forces, we may suppose the forces turned through...
Page 29 - The perpendicular distance between the lines of action of the two forces is called the arm, and the product of one of the forces and the arm is called the moment of the couple. A...