#Newton's laws


Newton's laws of motion are three physical laws that, together, laid the foundation for classical mechanics. They describe the relationship between a body and the forces acting upon it, and its motion in response to those forces. More precisely, the first law defines the force qualitatively, the second law offers a quantitative measure of the force, and the third asserts that a single isolated force doesn't exist. These three laws have been expressed in several ways, over nearly three centuries,[a] and can be summarised as follows:



##First law

In an inertial frame of reference, an object either remains at rest or continues to move at a constant velocity, unless acted upon by a force.[2][3]

$$ \sum \mathbf{F} = 0\; \Leftrightarrow\; \frac{\mathrm{d} \mathbf{v} }{\mathrm{d}t} = 0.$$


##Second law

In an inertial frame of reference, 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: $F = ma$. (It is assumed here that the mass $m$ is constant – see below.)


$$  \mathbf{F} = \frac{\mathrm{d}\mathbf{p}}{\mathrm{d}t} = \frac{\mathrm{d}(m\mathbf v)}{\mathrm{d}t}.   $$

$$
\mathbf{F} = m\,\frac{\mathrm{d}\mathbf{v}}{\mathrm{d}t} = m\mathbf{a},
$$

##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.


$$
\mathbf{F}_A = \mathbf{F}_B
$$

##SVG in markdown

!(svg:[{circle: {cx: 100,cy: 80,r:40,stroke:black,stroke-width:4, fill: red}}, {circle: {cx: 250,cy: 80,r:20,stroke:black,stroke-width:4, fill: orange}}, {line: {x1: 100,y1:80,x2:250,y2:80,stroke:blue,stroke-width:4}}, {text: {x: 100,y:70, style:font-family:sans-serif;, val:A}}, {text: {x: 250,y:80, style:font-family:sans-serif;, val:B}}])

Newton's laws are applied to objects which are idealised as single point masses,[9] in the sense that the size and shape of the object's body are neglected to focus on its motion more easily. This can be done when the object is small compared to the distances involved in its analysis, or the deformation and rotation of the body are of no importance. In this way, even a planet can be idealised as a particle for analysis of its orbital motion around a star.

In their original form, Newton's laws of motion are not adequate to characterise the motion of rigid bodies and deformable bodies. Leonhard Euler in 1750 introduced a generalisation of Newton's laws of motion for rigid bodies called Euler's laws of motion, later applied as well for deformable bodies assumed as a continuum. If a body is represented as an assemblage of discrete particles, each governed by Newton's laws of motion, then Euler's laws can be derived from Newton's laws. Euler's laws can, however, be taken as axioms describing the laws of motion for extended bodies, independently of any particle structure.[10]

Newton's laws hold only with respect to a certain set of frames of reference called Newtonian or inertial reference frames. Some authors interpret the first law as defining what an inertial reference frame is; from this point of view, the second law holds only when the observation is made from an inertial reference frame, and therefore the first law cannot be proved as a special case of the second. Other authors do treat the first law as a corollary of the second.[11][12] The explicit concept of an inertial frame of reference was not developed until long after Newton's death.

In the given interpretation mass, acceleration, momentum, and (most importantly) force are assumed to be externally defined quantities. This is the most common, but not the only interpretation of the way one can consider the laws to be a definition of these quantities.

Newtonian mechanics has been superseded by special relativity, but it is still useful as an approximation when the speeds involved are much slower than the speed of light.[13]

###Seminal physics publications 

***
|**Author**|**Dates**|**Contribution**|
| :--------------------------------| --------------------------------: | :-------------------------------- :| 
| Aristotle               |384 – 322 BCE	|Physicae Auscultationes	|
| Archimedes              |287 – 212 BCE 		|On Floating Bodies	|
| Ptolemy             |90 – 168	|Almagest, Geographia, Apotelesmatika		|
| Aryabhatta         |476 – 550       |Āryabhaṭīya            |
| Alhazen               |965 – 1040		|Book of Optics		|
|Copernicus	|1473 – 1543	|On the Revolutions of the Celestial Spheres	|
|Galilei		|1564 – 1642		|Dialogue Concerning the Two Chief World Systems	|
|Descartes	|1596 – 1650		|Meditations on First Philosophy	|
|Newton	|1643 – 1727		|Philosophiæ Naturalis Principia Mathematica	|
|Faraday	|1791 – 1867		|Experimental Researches in Electricity	|
|Maxwell	|1831 – 1879		|A Treatise on Electricity and Magnetism	|
***


###Birds of India

***
|**Small Blue Kingfisher**|**Peafowl**|
|:----------------------------:|:-------------:|
|![Pond Kingfisher](https://upload.wikimedia.org/wikipedia/commons/thumb/c/cc/Common_Kingfisher_Alcedo_atthis.jpg/220px-Common_Kingfisher_Alcedo_atthis.jpg "Small Blue Kingfisher")|![Peafowl](https://upload.wikimedia.org/wikipedia/commons/thumb/c/c3/Peacock_by_Nihal_jabin.jpg/330px-Peacock_by_Nihal_jabin.jpg =220x220 "Peacock from behind")|
***

###References

[1] [Aristotle's works on Physics](http://classics.mit.edu/Aristotle/physics.html)

[2] Archimedes, !doi[10.1038/057409a0]

[3] [Works of Aryabhatta](http://articles.adsabs.harvard.edu/cgi-bin/nph-iarticle_query?1977BASI....5...10A&defaultprint=YES&filetype=.pdf)

[4] Newton, !doi[10.1098/rstl.1695.0077]

[4] Maxwell, !doi[10.1080/00033799800200151]

[5] Faraday, !doi[10.1098/rstl.1865.0008]