What is(are) the effect(s) of disorder on electrical conductivity? As a non-specialist, I asked the question "What are disorders in condensed matter parlance?" about the meaning of disorder in condensed matter physics. I also wrote a non-specialist answer after some research. Here is yet another question that has been bugging me.
Crystalline metals with perfect periodicity perfectly conduct electric current (Correct me if I'm wrong). What happens when one gradually introduces more and more disorder into a periodic structure? Does the conductivity necessarily decrease?
 A: Short answer is the resistivity increases until it transitions to insulator.
A band description makes things more clear.  Before the transition, the electronic states are pertubatively connected to to disorderless band conductor.  After the transition to an insulator the electronic states all become localized and in momentum space this shows up as a band gap around the fermi energy and effectively looks like a band insulator.  This is anderson localization: https://en.wikipedia.org/wiki/Anderson_localization
Long answer: Its complicated and not fully understood.  In 1D there is no transition.  The smallest amount of disorder will localize the system.  But at a certain interaction strength the system will delocalize and start conducting again.
Out side of 1D, the non interacting case can be described with different effect models, where usually another or multiple effective fields are introduced which interact with the electron field to cause localization.  Here the normal mean field description of a phase transition works and can give you universal scaling relations at the transition. For some discussion you can see this review for the super symmetric method: http://arxiv-export-lb.library.cornell.edu/abs/1002.2632
But things are more complicated and there might not be a simple transition.  The griffiths effect describes the possibility of rare regions to localize or delocalize the system in the traditionally conducting or insulating limits.  This then creates a middle zone between the transition from conductor to insulator where rare regions play a more important role and may smooth the transition to a cross over.  
Finally there has been observations that disorder can actually delocalize a mott insulator(where a gap opens around the fermi surface due to interactions).  Here disorder increases conductivity: https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.112.206402 
A: Long range order is less important to metallic behaviour than often believed. When alkali metals melt there is only a small jump in resistivity. When silicon melts, it turns from a semiconductor into a liquid metal, as does germanium. Amorphous Si and Ge are, however, semiconductors. These examples show that long range disorder or order are not deciding whether a material conducts or not. Long range disorder does increase resistivity. 
A more useful picture of conduction is obtained by using local orbitals, as in the Hubbard model. This model in its basic form has two parameters, on-site electron-electron repulsion $U$ and nearest neighbour hopping $t$. It shows that the ratio $t/J$ is decisive. If the repulsion is strong localised orbitals and insulating behaviour results. In the opposite case, delocalised electron orbitals and conduction result. 
