Here's some ball-park estimates for the part values.
Read the comments on the spreadsheet. The Altec response plots and the textbook circuit values don't quite match up. Normally a textbook constant-k filter design ends up with a Butterworth response.
I added a tweak parameter 'x' which you can see bends the circuit towards the plots. The way the bending is done is kind of in the spirit of a constant-k design. You can see the uncertainty in the part values is then 20%.
Some uncertainty from back-engineering the response can come from discrete cap and inductor values in the real unit. No doubt the inductor is a custom inductor, probably multi-tapped, so there's no reason the inductances have to stick to standard values. The tweaked cap values are perhaps closer to standard values.


It occurred to me later the reduced attenuation at freq/5 could be due to the DC resistance of the inductor.
The size of the inductor determines the resistance and the distortion. We have no distortion spec on the unit although we do have a maximum voltage. The attenuation at freq/10 could be used to work out a DC resistance for the inductor but each frequency setting will a different DC resistance because the inductor is different. Another issue is at the lower frequencies, where the size of the inductor is more demanding, the plots don't go low enough to see the attenuation at freq/10.
All in all there's not enough info in the catalog to split hairs.
All I can say is my tweak shouldn't be treated as the answer. The inductor DC resistances are an equally valid explanation, perhaps even more likely.
To get the right attenuation at freq/5 for the 1kHz range a DC resistance of around 15 to 20 ohms would be a good ball-park. However that could mean the DC resistance of the 70Hz range is somewhat higher - it can't be too high as it would change the roll-off too much.