Macroscopically, at a constant volume, the pressure  
\[p\]
  exerted by a gas is proportional to its temperature  
\[T\]
  in Kelvins. We can write this as  
\[p=kT\]
  where  
\[k\]
  or  
\[\frac{p}{T}=k\]
  where  
\[k\]
  is a constant.
Microscopically, this can be explained in the following way.