At this stage, all U and D edges, with the possible exception of FU/FD, which may need to be exchanged. Physically rotate the cube sideways to view the remaining four E edges as M edges.
Now that both the the R and L faces (ie the original U and D faces) have been (largely) settled, we shift to a new paradigm. Regard these two faces as two metal plates with the M slice in between. Only this M slice have edges to be solved. They can always be solved with either of the following algorithms using suitable conjugates of Mn.
The remaining cubes on this page have yellow on the R face, as a result of the physical rotation.
Note that Fa is called Z in the standard notation. Refer to this page for the movement names.
Noting that M moves one M edge to another,
EM3 is topologically the same as EM1F. At that time, our sole concern was FU. Actually it moves three edges without affecting other things.
Use two different ways to look at EM3:
Formally, we can also say that U2 is a mono-move on the F face. The commutator EM3 is thus analogous to CM3 and EM3R.
Similar to EM3, we have
Again, use two ways to look at EM4:
Use EM3 and EM4 to settle the position of the M edges. In some cases, you would end up with one single pair of swapped edges, which indicates it is time for some unfinished business.
Remember that back in Part II, there is one situation where we left FU and FD swapped and unhandled. We are treating them now.
After the physical rotation at the beginning of Part III, the four E edges have become M edges. FU and FD now lie on the front of the R and L faces (the two pieces marked with black Xs). Use Mn to move the swapped M edges to the back (the two pieces marked with white Xs, on the B face).
After physical rotation X, a conjugate of EM4 will swap the two pairs of edges.
Continue to Completing the Cube
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