Classical laminate theory doesn't directly address through-thickness stresses/strains, and that includes interlaminar shears. The NASA document appears to address CLT only, and is no immediate use for through-thickness stresses.
{Note on RP1351:
RP1351 also has a couple of errors. One is unimportant and is in the bit where the author solves the ABD matrix using determinants, which nobody now uses since fully inverting a 6x6 is trivial these days. However, the other appears relatively serious. RP 1351 P. 9 says that
[Qbar] = [T'][Q][R][T] ([T'] is the inverse of [T])
whereas I think it should be
[Qbar] = [T'][Q][R][T][R']
or, alternatively,
[Qbar] = [T'][Q][T'T] ([T'T] is the transpose of [T'])
This has to do with keeping consistency between tensor and engineering shear strains, and it's possible that the author (Nettles) has compensated elsewhere, but as far as I'm aware coding something up using the RP1351 equations will give the wrong answers.
}
The through-thickness stresses and strains due to *in-plane and hygrothermal* loads peak at the laminate edges and drop off fairly sharply with distance in from the edge, typically trending to almost zero at about 1.0*thickness in for shear and less than that for direct 3-direction stress. (See Datoo's book for a reasonable description and analysis of edge-effects.) NB: codes such as NASTRAN that work with layered elements typically cannot calculate these stresses. It's necessary to model the layers explicitly to recover them.
The through-thickness shears due to *applied shear loads* are distributed through the thickness a bit differently from in a non-layered plate or beam.
NASTRAN and other codes with interlaminar shear recovery in layered elements will calculate interlaminar shear stresses due to applied mechanical shear loads correctly, and FE of a unit plate is often the simplest way to go. I don't currently have a spreadsheet-style solution available, though I hope to recover an old McDonnell Douglas one next week.
Essentally you take the plate-axis (X-direction, not 1-direction) endload in each ply due to the bending from the moment caused by the shear load and add up the endloads between the plate/beam extreme fibre and the point of interest through the thickness. This is exactly what the the classical S.A.y_bar/I aka V.Q/(I.b) formulas used for isotropic materials do. To put it another way, you have to do a ply-by-ply analysis of a plate with a unit bending load on it to find the plate-axis direction endloads in each ply then add them up. So, classical laminate theory and NASA RP1351 are appropriate as a means to find these endloads (if TP1351 isn't as wrong as I think it may be).
I'll update with the appropriate formulae when I can.