Maybe it's time to consider the Y-Δ transformation .
It's really not that difficult, particularly for the values here.
The delta is the triangle on the left. Those are the resistors in Loop a . Point A is equivalent to point A in your overall circuit. Point B is at the node which you labeled with voltage V
1 on some of your diagrams. Point C is at the node which you labeled with voltage V
2 on some of your diagrams.
The idea here is to replace that given set of resistors connected in that way, with a set of resistors in a "Y" configuration, as seen on the right. We need this set of resistors in the Y-configuration to behave exactly as the original set in the Δ-configuration in regards to nodes A, B, and C.
What this boils down to is that the resistances between the three nodes (taken pair-wise) must be the same for both configurations.
Starting with the Δ-configuration, find the resistance between A & B, between B & C, and between A & C .
For example: between A&B: The single resistor, r, is in parallel with the series combination of r and 3r. R
AB = (4r
2)/(5r) = (4/5)r .
R
BC gives the same result: R
BC = (4/5)r .
For R
AC we have 3r in parallel with the series combination of r and r, giving R
AB = (3r⋅2r)/(5r) = (6/5)r .
Now figure out what R
A, R
B, and R
C must be in the Y-configuration on the right. For each pair here, we only have two resistors in series.
We must have:
RA + RB = (4/5)r
RB + RC = (4/5)r
RA + RC = (6/5)r
What do you get for these?