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Dynamics
The purpose of classical mechanics is to provide a connection between the acceleration of a body and the forces acting in it. Keep in mind that classical mechanics deals with objects that are large compared with the dimensions of atoms (~10-10m) and move at speeds that the much less than the speed of light (3*108m/s).
The new approach to motion was later formalized by Newton in a form that come to be known as Newton’s first law of motion:
As object at rest will remain at rest and an object in motion will continue a motion with a constant velocity unless it experiences a net external force (or result force). We can say that when the resultant force on a body is zero, its acceleration is zero. That is when ΣF = 0, then a = 0. Newton’s first law is sometimes called the law of inertia and it applies to objects in an inertial frame of reference. Inertia is the property of matter that relates to the tendency of an object to remain at rest or in uniform motion. Mass is a term used to measure inertia. The greater the mass of a body, the less it will accelerate (change its nnn of motion) under the action of an applied force. Newton’s second law The acceleration of an objects is inversely proportional to its mass.
The Newton’s second law: The acceleration of an object is directly proportional to the resultant force acting on it and inversely proportional to its mass
Note that if the resultant force is zero, then a = 0, which corresponds to the equilibrium situation where v is equal to a constant. Thus we can relate mass and force through the following mathematical statement of Newton’s second law: Σ F = ma (1) You should note that equation (1) is a vector expression and hence is equivalent to the following three component equations: Σ Fx = max Σ Fy = may Σ Fz = maz To state the law in its most general form, we first define the momentum, p, of a particle as the product of the mass, m and the velocity, u
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