Laws of motion
In physics, motion is described through two sets of apparently contradictory laws of mechanics. Motions of all largescale and familiar objects in the universe (such as projectiles, planets, cells, and humans) are described by classical mechanics. Whereas the motion of very small atomic and subatomic objects is described by quantum mechanics.
First law:

In an inertial reference frame, an object either remains at rest or continues to move at a constant velocity, unless acted upon by a net force.

Second law:

In an inertial reference frame, the vector sum of the forces F on an object is equal to the mass m of that object multiplied by the acceleration a of the object: F = ma.

Third law:

When one body exerts a force on a second body, the second body simultaneously exerts a force equal in magnitude and opposite in direction on the first body.

Classical mechanics
Classical mechanics is used for describing the motion of macroscopic objects, from projectiles to parts of machinery, as well as astronomical objects, such as spacecraft, planets, stars, and galaxies. It produces very accurate results within these domains, and is one of the oldest and largest in science, engineering, and technology.
Classical mechanics is fundamentally based on Newton's laws of motion. These laws describe the relationship between the forces acting on a body and the motion of that body. They were first compiled by Sir Isaac Newton in his work Philosophiæ Naturalis Principia Mathematica, first published on July 5, 1687. Newton's three laws are:
 A body either is at rest or moves with constant velocity, until and unless an outer force is applied to it.
 An object will travel in one direction only until an outer force changes its direction.
 Whenever one body exerts a force F onto a second body, (in some cases, which is standing still) the second body exerts the force −F on the first body. F and −F are equal in magnitude and opposite in sense. So, the body which exerts F will go backwards.^{[3]}
Newton's three laws of motion were the first to accurately provide a mathematical model for understanding orbiting bodies in outer space. This explanation unified the motion of celestial bodies and motion of objects on earth.
Classical mechanics was further enhanced by Albert Einstein's special relativity and general relativity. Special relativity is concerned with the motion of objects with a high velocity, approaching the speed of light; general relativity is employed to handle gravitational motion at a deeper level.
Uniform Motion:
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When an object moves with a constant speed at a particular direction at regular intervals of time it's known as the uniform motion. For example: a bike moving in a straight line with a constant speed.
EQUATIONS OF UNIFORM MOTION:
If v = final velocity, u = initial velocity, a = acceleration, t = time, s = displacement, then :
 $\mathbf {v} =\mathbf {u} +\mathbf {a} \mathbf {t}$
 $\mathbf {v} ^{2}=\mathbf {u} ^{2}+2\mathbf {a} \mathbf {s}$
 $\mathbf {s} =\mathbf {u} \mathbf {t} +{\frac {\mathbf {a} \mathbf {t} ^{2}}{2}}$
Quantum mechanics
Quantum mechanics is a set of principles describing physical reality at the atomic level of matter (molecules and atoms) and the subatomic particles (electrons, protons, neutrons, and even smaller elementary particles such as quarks). These descriptions include the simultaneous wavelike and particlelike behavior of both matter and radiation energy as described in the wave–particle duality.^{[citation needed]}
In classical mechanics, accurate measurements and predictions of the state of objects can be calculated, such as location and velocity. In the quantum mechanics, due to the Heisenberg uncertainty principle, the complete state of a subatomic particle, such as its location and velocity, cannot be simultaneously determined.^{[citation needed]}
In addition to describing the motion of atomic level phenomena, quantum mechanics is useful in understanding some largescale phenomenon such as superfluidity, superconductivity, and biological systems, including the function of smell receptors and the structures of proteins.^{[citation needed]}