The interlaminar shear stress is essentially the same as the normal shear stress, due to it being the complementary shear to the normal. They're the same.
SW's method is fine, if a little conservative for your thickish, stiff skins. The shear varies linearly from zero at the outer surface of the skin to the interface value. It is then effectively constant across the core, although there is a tiny bit of the usual rectangular-section peaking with a very slightly higher value at the neutral axis (a really stiff core cf. the face sheets will increase this small peaking; with steel face sheets and an elastomer (=low modulus) core, it's not a worry).
A slightly more accurate value for the interface shear value is to divide the shear force by the distance between face sheet centerlines.
For an actual structure you need to do structual analysis to assess the shear/unit width, and then apply the shear stress formula as we've described. For a simply supported flat rectangular plate the peak will be in the center of the plate, and the formula in Roark will be adequate.
An old copy of Allen, "Analysis and Design of Structural Sandwich Panels" or Zenkert, "An Introduction to Sandwich Contruction" will clear things up. (I'm told that Tom Bitzer's "Honeycomb Technology" is also good.)
In fact, our old friends at Diab and Hexcel may well help:
With a flexible elastomer core watch out for the large shear component of the deflection due to the normal loading, and the comcommitent decrease in buckling loads due to any in-plane loading.