Mechanics Flashcards
is that branch of mechanics which deals with the motion of bodies under the action of forces.
Dynamics
deals with the effects of forces on bodies at rest.
Statics
Dynamics has two distinct parts:
Kinematics
Kinetics
the study of motion without reference to the forces which cause motion
Kinematics
relates the action of forces on bodies to their resulting motions.
Kinetics
made careful observations concerning bodies in free fall, motion on an inclined plane, and motion of the pendulum.
Galileo (1564–1642)
is the geometric region occupied by bodies.
Space
which is generally recognized as one of the greatest of all recorded contributions to knowledge
Principia
was able to make an accurate formulation of the laws of motion and, thus, to place dynamics on a sound basis.
Newton (1642–1727)
an imaginary set of rectangular axes assumed to have no translation or rotation in space.
the primary inertial system or astronomical frame of reference
The basic frame of reference for the laws of Newtonian mechanics
the primary inertial system or astronomical frame of reference
is a measure of the succession of events and is considered an absolute quantity in Newtonian mechanics.
Time
is the quantitative measure of the inertia or resistance to change in motion of a body
Mass
the vector action of one body on another.
Force
is a body of negligible dimensions
Particle
is a body whose changes in shape are negligible compared with the overall dimensions of the body or with the changes in position of the body as a whole.
Rigid body
Law I
A particle remains at rest or continues to move with uniform velocity (in a straight line with a constant speed) if there is no unbalanced force acting on it.
Law II
The acceleration of a particle is proportional to the resultant force acting on it and is in the direction of this force.
Law III
The forces of action and reaction between interacting bodies are equal in magnitude, opposite in direction, and collinear.
Newton’s second law forms the basis for most of the analysis in dynamics.
F=ma