Ah, you have asked what may be (say in old American game show parlance) “a $64,000 question”. In perhaps about enough over-simplification of the “Iowa” (named after/where much early research near Iowa State University, my alma mater a few years later, took place) ring deflection formula for buried flexible pipes to evoke argument, I believe at least the dependable pipe stiffness value was originally intended to be used as follows:
Ring Deflection = (a Factoring of Buried Load)/[(Pipe Stiffness) + (a Factoring of Sidefill Soil Stiffness)], and of course all to be in compatible units
Now, moving beyond that and looking in some more detail at only the one term you are curious about from the denominator, “pipe stiffness” has traditionally been determined either from ring loading tests (such as “three-edge bearing” or “parallel plate loading” tests) or from strength of materials ring (essentially “curved beam”) formulae relationships involving the modulus of elasticity (E) of the piping material. If I might misquote from Hamlet’s soliloquy, I believe “therein lies the rub”, at least with regard to low stiffness, viscoelastic piping materials.
Specifically, experimental pipe stiffness or P.S. is basically determined per ASTM D2412 standard test as the recorded laboratory load e.g. in pounds, distributed e.g. per axial inch on the pipe ring divided by the measured vertical ring deflection e.g. in inches at that load. Now in this regard, when ASTM D2412 external plastic pipe loading standard was founded, the developers of that standard required the pipe rings to be tested at a quite rapid rate of (e.g. of vertical) load application between parallel plates. The prescribed rate of laboratory (normally vertical) load application has been ½ inch diameter (12.5 mm) per second. I do not know why the founders of the ASTM standard chose such a rapid rate (perhaps more learned folks and maybe even in the industry will explain); however, I believe quick loading rates of course minimize testing times and cost and also perhaps more importantly maximize the determined stiffness value, even when some types of plastic pipes are formulated with (less expensive than resin derived e.g. from crude oil) fillers.
While significantly slower rates of load application would result in significantly lower values of pipe stiffness, I think many in the plastic pipe industry in general (and/or maybe even a well-known third-party researcher or two they have employed) has traditionally or historically basically advocated that this ASTM quite rapid-loading (or arguably short-term) stiffness or modulus is what should be plugged into the aforementioned buried formula/relationship, even though earth load in reality is of course MUCH more inexorably applied, in some cases for a buried design life of 50 or more years (or at least until the pipe fails)!
If you are curious as to the magnitude of difference (that may be surprising to many designers) between some typical short-term and longer-term pipe stiffness or modulus values for plastics, I think you could find some representative values now with at least some in-depth searches (as I don’t think this has traditionally been heavily advertised by the plastic pipe industry). E.g. see Section H 211.41 DESIGN OF PLASTIC PIPE in the manual of a very large USA utility at
and Table 2.3 page 9 at
etc.
With regard to my opening statement, I believe there have been a great many problems involving flexible plastic pipes and lofty expectations of pipe/soil strength and/or available construction/inspection quality to achieve same, and many with far more than “$64,000” at stake, and it appears that this may be a factor in the involvement of a former president of the American Society of Civil Engineers in some pipe matters as are reflected in a presentation not long ago at
I believe as is mentioned in that presentation, "profile-walled" pipes with invevitably some even higher strained local areas than solid-walled pipes can even further complicate the picture.