I have a 30 VA Radio Shack transformer that's very handy for making measurements of the effects of variations in core configuration because they didn't varnish the laminations. I can unstack it and restack it however I wish.
I restacked it with all the E laminations together and all the I laminations together. I put the stacks on a flat surface and with a soft mallet, I lined up all the edges and then put a nylon screw through a hole in the laminations to keep everything together.
With all the E's together and placed in the bobbin, I could then take the stack of I's and put them across the ends of the E's so that there was one combined butt joint.
I then clamped the E's and I's together with a few pounds of
pressure and measured the power loss with the same setup I described in post #14, applying 120 VAC to the primary with the secondary open circuited..
The DC resistance of the primary is 33.2 ohms.
The first image shows the measurement with the two stacks clamped together. The exciting current is .0787 amps, which gives a copper loss of .0787*.0787*33.2 = .2056 watts. The core loss was 1.65 - .2056 = 1.44 watts.
The second image shows the measurement with the two stacks separated by a .002" piece of nomex, then clamped. The exciting current is .180 amps, which gives a copper loss of 1.076 watts. The core loss was 2.54 - 1.076 = 1.464 watts.
Adding gap to the core substantially increased the exciting current, but hardly changed the core loss at all. This is what I would expect, since the reluctance which the gap adds to the
flux path is in air, and air is not a lossy core material.
When the laminations are stacked in interleaved fashion, increasing the gap between an E lam and its mating I lam causes flux which would normally cross the gap to move to the side, and pass through a neighboring lam, increasing the flux density locally there. That would increase loss in the iron locally.
I'll make a pair of measurements on an interleaved stack and post the results.