The network is not reducible to a simple series and parallel combinations of resistors,There is,however a clear symmetry in the problem which we can exploit to obtain the equivalent resistance of the network.
Now the job is to find the sides in which the current is the same,say I.Further,at the corners the incoming current I must split equally into the outgoing branches.In this manner,the current in all the 12 edges of the cube are easily written down in terms of I,using Kirchhoff's first rule and the symmetry in the problem.For example take a closed loop,and apply Kirchhoff's second law [itex]\rightarrow[/itex] -IR-(1/2)IR-IR+ε = 0 ;where R is the resistance of each edge and ε the emf of the battery.
Now find the equivalent resistance R[itex]_{eq}[/itex]
For R=R Ω,R[itex]_{eq}[/itex] = ? and for ε=V Volts,the total current in the network is [itex]\longrightarrow[/itex]