Natural philosophy. Mechanics, Τόμος 1Murby, 1873 |
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Αποτελέσματα 1 - 5 από τα 20.
Σελίδα 3
... remain in the same place ; that is , it will continue at rest . If , how- ever , it be not allowed to remain by itself , but some power , such as a push , be brought to bear upon it , it will not continue in the same position , but will ...
... remain in the same place ; that is , it will continue at rest . If , how- ever , it be not allowed to remain by itself , but some power , such as a push , be brought to bear upon it , it will not continue in the same position , but will ...
Σελίδα 10
... remains unchanged . Hence it appears that the SPACE described by a particle moving with uniform velocity may be represented by the area of a rectangle having for one of its sides a line representing TIME ; and for an adjacent side a ...
... remains unchanged . Hence it appears that the SPACE described by a particle moving with uniform velocity may be represented by the area of a rectangle having for one of its sides a line representing TIME ; and for an adjacent side a ...
Σελίδα 13
... remains to express the space passed over under the action of a uniformly accelerating force in terms of the acceleration and the time . This is easily done , for the acceleration has been previously . Wherefore the space traversed by a ...
... remains to express the space passed over under the action of a uniformly accelerating force in terms of the acceleration and the time . This is easily done , for the acceleration has been previously . Wherefore the space traversed by a ...
Σελίδα 15
... remains to show the character of a line of velocities in the most general case ; that is , when the motion is irregularly accelerated and retarded . In such a case It has been proved that the rectangle is represented by vt , and the ...
... remains to show the character of a line of velocities in the most general case ; that is , when the motion is irregularly accelerated and retarded . In such a case It has been proved that the rectangle is represented by vt , and the ...
Σελίδα 19
... remain at rest ; in the latter ( b ) motion will be imparted to it . A body under the influence of forces which neutralize each other , is said to be in equilibrium . The door in our first supposed case was therefore in equilibrium ...
... remain at rest ; in the latter ( b ) motion will be imparted to it . A body under the influence of forces which neutralize each other , is said to be in equilibrium . The door in our first supposed case was therefore in equilibrium ...
Άλλες εκδόσεις - Προβολή όλων
Natural Philosophy: Part 1, Mechanics (1873) J. Alfred Skertchly Δεν υπάρχει διαθέσιμη προεπισκόπηση - 2008 |
Συχνά εμφανιζόμενοι όροι και φράσεις
acceleration angle of repose attached axis beam body moves called central force centre of gravity centrifugal force circle circumference continuous circular motion curve cylinder descend diameter direction distance earth effect equal equilibrium exerted falling body feet per second fixed point foot-pounds force of gravity forces acting friction fulcrum Hence horizontal impact inches inclined plane isochronous kinetic energy length lever lifted machine mechanical efficiency miles per hr movable block multiplied number of seconds number of units oscillation parabola parallel forces parallelogram particle passive force path perpendicular pitch position pounds pounds weight pressure produce projectile proportional pulley radii radius raise ratio rectilinear motion represent resistance rest resultant revolution revolve rope passing round screw sheave simple pendulums space square stone surface suspended teeth tons triangle upper block velocity vertical vibrate wedge wheel and axle
Δημοφιλή αποσπάσματα
Σελίδα 41 - Newton's Three Laws of Motion," and are as follows: (1) All bodies continue in a state of rest, or of uniform motion in a straight line, unless acted upon by some external force that compels a change.
Σελίδα 15 - To find the area of a trapezoid. RULE. Multiply half the sum of the two parallel sides "by the perpendicular distance between them : the product will be the area.
Σελίδα 87 - This proportion teaches us that, when in equilibrium, the power is to the weight as the height of the plane is to its length.
Σελίδα 41 - First. A body in motion, and not acted upon by any external force, will move with a uniform velocity in a straight line.
Σελίδα 59 - There is an equilibrium upon the wheel and axle when the power is to the weight as the radius of the axle to the radius of the wheel.
Σελίδα 48 - Hence it is evident, that in every species of lever there will be an equilibrium, when the power is to the weight as the distance of the weight from the fulcrum is to the distance of the power from the fulcrum.
Σελίδα 32 - 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.
Σελίδα 134 - The force is proportional to the square of the velocity and inversely proportional to the radius of turn during radial acceleration.
Σελίδα 46 - These machines are ; 1. the lever; 2. the wheel and axle ; 3. the pulley ; 4. the inclined plane ; 5. the wedge ; and 6. the screw.
Σελίδα 28 - 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...