Wow. Thanks for the responses. I wasn't sure if this post would generate any interest. Clearly I was wrong! I'll be looking at the Hardy Cross Column analogy and the Gere text to see if I can yield anything from them. I remember coming across a "simple beam analysis" spreadsheet as a young EIT, and thought it was crazy and the most advanced thing ever. Once I started digging into the code, I realized that it was just Newmark's method with some Roark formulas. Breaking that barrier has really allowed me to dig into numerical methods to approximate and solve otherwise complex situations. Fast forward to yesterday's query, and I think I have another barrier to break through. Awesome!
@rb1957: The situation I simplified in the description is this:
4 suspended slabs with clear spans running E-W between slab bands. Slab bands are 2x thick as suspended slabs and run about half of the clear span length. Slab bands run N-S, supported on columns.
Here was my design process for those interested:
1) Find an upper bound for the clear span. Maximum positive moment = wL2/8. Negative moments estimated to be wL2/12
2) Use the Approximate Moment Coefficients applied to the 4-clear span continuous beam. These didn't necessarily apply because the spans vary in some locations by more than 20%.
3) Run a Moment Distribution spreadsheet to capture the continuous span behaviour.
I knew that #1 was an upper bound that wouldn't quite capture the negative moment in the interior spans.
I didn't have high regard for the results for #2 because the varying span lengths.
#3 captured the essence of the continuous behaviour and let me run skip loading cases to really get a picture of the negative moment. However, what I was leaving out was that my "pins" were actually 8' wide sections that were 2x as thick as the slab. So I (apparently) wasn't capturing the critical negative moment at the support as accurately as I should. A colleague ran it in an analysis program, increasing the stiffness 4' on either side of the pin.