How does cutting a spring increase spring constant? I know that on cutting a spring into n equal pieces, spring constant becomes n times.
But I have no idea why this happens. 
Please clarify the reasons 
 A: Equations are nice, but if you're looking for a conceptual answer :

A: In general, the spring constant or stiffness of a coiled spring is given as
$$k=\frac{\pi Gd^4}{64R^3n}$$
Where, $G$ is modulus of rigidity of spring material
$d$ is the diameter of spring wire 
$R$ is the mean radius of coil 
$n$ is the effective number of coils in spring which is directly proportional to the length of coiled spring i.e. $n\propto L$
Above formula simply shows that if the other parameters are kept constant then
$k$ is inversely proportional to $n$ number of coils. Since the number of coils $n$ is directly proportional to length $L$ of coiled spring hence its spring constant $k$ is inversely proportional to its length. Thus
$$k\propto \frac 1n\iff k\propto \frac1L$$
Therefore if a spring is broken into certain no. of pieces, all parameters $G$, $R$ & $d$ remain constant for all the pieces except the number of coils or turns $n$ decreases hence stiffness $k$ increases. 
In general, if a coiled spring of length $L$ & stiffness $k$ is broken into $m$ no. of pieces of lengths $L_1, L_2, L_3, \ldots L_m$ then their respective spring constant or stiffness is given as follows
$$k_1=k\left(\frac{L}{L_1}\right),  \ \ \ k_2=k\left(\frac{L}{L_2}\right),\dots k_i=k\left(\frac{L}{L_i}\right), \ldots , k_m=k\left(\frac{L}{L_m}\right)$$
Relation among spring constants of broken pieces & original spring:
$$\implies L1=\frac{kL}{k_1}, \ L2=\frac{kL}{k_2}, \ldots , Li=\frac{kL}{k_i}\ldots, Lm=\frac{kL}{k_m}$$
If we add all $m$ number of lengths of pieces we get original length $L$ of spring i.e.
$$L_1+L_2+\ldots +L_i+\ldots +L_m=L$$
$$\frac{kL}{k_1}+\frac{kL}{k_2}+\ldots+\frac{kL}{k_i}+\ldots+\frac{kL}{k_m}=L$$
$$KL\left(\frac{1}{k_1}+\frac{1}{k_2}+\ldots+\frac{1}{k_i}+\ldots+\frac{1}{k_m}\right)=L$$
$$\color{blue}{\frac{1}{k_1}+\frac{1}{k_2}+\ldots+\frac{1}{k_i}+\ldots+\frac{1}{k_m}=\frac1k}$$ 
Above relation of spring constants is analogous to parallel connection of $m$ number of electric resistances
A: For a given deformation, the distance change between two adjacent particles (molecules/atoms) is more if you decrease the length of the spring. Thus, if you keep the displacement small enough so as the intermolecular force is linearly proportional to the intermolecular distance, the force required to produce the same deformation in a short spring is more compared to a longer spring. If you cut a spring into $n$ pieces, the distance change between two particles would have to be $n$ times more to keep the total deformation the same, and linearity tells us that the force required will be $n$ times greater.
Note that the above model may fail as in a real metal spring, there are grain boundaries, dislocations, etc. But it is presents a good intutive picture.
A: Let us consider that you join these n pieces of springs in series. Now you know that you have got the original spring whose spring constant is $k$ (say). Now joining springs in series is like joining resistors in parallel (identical formulae) which can easily proven by balancing forces. Hence,
$$\frac{1}{k} = \frac{1}{k'} + \frac{1}{k'} + \frac{1}{k'}+\dots n ~\rm times$$ where $k'$ is the spring constant of individual cut springs.
On solving the above equation you will get that the spring constant becomes $n$ times.
A: This happens because spring constant is not really a constant. If you consider any normal elastic material, when a force F is applied, the strech is given by hooke's law :
$$\frac{{F}/{A}}{{\Delta L}/{L}}=Y$$
where $Y$ is the young's modulus of material, which is upto a limit, constant and depend only on the material.
This means the strech
$$\Delta L = \frac{FL}{AY}$$
or
$$F = \frac{AY}{L}\Delta L$$
we see that the proportionality constant for spring is thus  $\frac{AY}{L}$. Thus, for a spring of $\frac{1}{2}$ the length, spring constant would be double.
A: spring constant is inversely proportional to its length hence when a spring of constant $k$ is cut into $n$ number of pieces, the length becomes $\frac1n$ times  initial length so spring constant becomes $k/(1/n)=nk$. therefore $k$ becomes $n$ times on cutting a spring.
