aircircpubs SIDD pipe bedding and Ontario Provincial Standards

更新时间:2023-07-16 18:06:01 阅读: 评论:0

SIDD pipe bedding and Ontario provincial
standards
Zhao, J.Q.; Daigle, L.
NRCC-44694
A version of this paper is published in / Une version de ce document   trouve dans: Proceedings of  the International Conference on Underground Infrastructure Rearch, Kitchener, Ontario, June 11-13, 2001, pp. 143-152
The OPSS on rigid pipes are bad on the tradi-tional indirect method. In this method, designs of rigid pipe rely on the Marston-Spangler theory for earth loads in trench and embankment installations (ACPA 1992; OCPA 1986). Recently, analys of pipe-soil interactions using the finite element method have resulted in the development of a direct design method. This method, commonly referred to as the Standard Installation Direct Design (SIDD) standard (ASCE/ANSI 1993), provides a different earth pressure distribution around the pipe for each of the four standard installation types. Becau of the due consideration of lateral earth support and re-duced reaction at the pipe invert, the SIDD method can provide significant savings in the pipe design and its installation. The SIDD method is not cur-rently included in the OPSS.
ABSTRACT: The current OPSS and OPSD that provide specifications for drainage pipes in Ontario, are shown to be a simplified and more conrvative version of the traditional Marston-Spangler method. The SIDD method was developed through extensive finite element analys. It improves the pipe installation prac-tice by lesning the requirements in bedding and compaction, and allowing the u of native backfill materi-als. There is potential cost-savings in using the SIDD method. The SIDD standard adopted by ASCE/ANSI, however, ems to have misd a few important pieces of design information and is inconsistent with the original SIDD rearch publication in the definition of soil types. The paper shows that an improved version of the SIDD method should be considered for adoption as an alternative in the OPSS, while the traditional Marston-Spangler method is maintained in the standards.
(3)  (4)    where A  = a constant corresponding to pipe shape and for circular pipe A =1.431; N  = a parameter which is a function of the distribution of the vertical load and horizontal reaction; x = a parameter which is a function of the area of the vertical projection of the pipe over which active lateral pressure is effec-tive ; q  = the ratio of the total lateral pressure to the total vertical load; k  = the ratio of the unit lateral soil pressure to unit vertical soil pressure (Rankine’s co-efficient of active earth pressure and k  = 0.33 will usually be sufficiently accurate); C c  = the load coef-ficient for positive projection pipe; H = cover depth; and B c  = pipe outside diameter. As shown in Equations 3 and 4, bedding factors for embankment conditions are not readily available since they not only depend on bedding class, but also depend on the ratio of cover depth to pipe out-side diameter, embankment type and the effective pipe area for active lateral pressure.  Using the same conditions as the positive projection ca of the
covering a wide variety of conditions, four standard types of standard installations, each with a unique pressure distribution, were introduced by ACPA (1993) and adopted by ASCE (ASCE/ANSI 1993) and by AASHTO (1996). It ems, however, to be a step backward becau the design practice has gone from a four-class bedding approach to FEM, and now back to another four-type installation approach. In this regard, Kellogg (1993) states: “With the popularity of numerical methods of analysis, classical approaches to the problems have  been waning. However, in the everyday practice of engineering, even in the computer age, clod-form solutions bad upon classical me-chanics and solutions to boundary-value differen-tial equations are still needed. The time and cost to prepare sophisticated numerical models for analysis simply cannot be justified in the market-place, except for the most complex and critical civil engineering structures.”
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galesCL
No compac-
tion re-
quired, ex-
cept if CL,
u  85% CL
† D0 = outside diameter of the pipe. Soil symbols as per Uni-
fied Soil Classification System (USCS) (ASTM D 2487 1993).
Of the four standard installation types, type 4 is of the lowest quality that requires no compaction (except for CL backfill soils), whereas type 1 is of the highest quality that requires well graded materi-als compacted to a minimum of 95% of the Maxi-mum Standard Proctor density. Special care
is re-quired for the middle bedding (directly beneath pipe invert) where the soil needs to be kept loo in order to transfer the loads to the haunch area, thereby re-ducing stress concentration at the invert of the pipe (ASCE/ANSI 1993; Meyer et al. 1993). Excessive compaction of the middle bedding, and insufficient compaction of the haunch area can result in pipe cracking (Wilson 1985).
The ASCE/ANSI Standard (1993) provides the pressure distribution diagram, which is called Heger pressure distribution, and its coefficients (Figure 4); however, it falls short by not providing formulas and coefficients to determine maximum thrusts, bending moments and shears for each of the four standard in-stallations (ASCE/ANSI 1993). The formulas and coefficients are provided in ACPA (1993) so that designers can u them to calculate design forces. Simpson Gumpertz & Heger Inc. provides SPIDA analysis rvice at a cost of US$15 to US$75 per de-sign (Heger et al. 1985). Figure 4. Heger pressure distribution diagram and coefficients (ACPA 1993).
3.3 Field performance verification
Sargand et al. (1994) independently instrumented a 600 mm diameter concrete pipe installed using the SIDD Type 3 installation in laboratory. They pointed out that to that date only a few installations had been instrumented and monitored for perform-ance verification of pipe-soil systems that were lai
d according to the SIDD standards. Their monitored results showed that the SIDD method is good at pre-dicting moments before the formation of cracks, but not so good after the formation of cracks in concrete pipe. Furthermore, measured thrusts were consistent with the predictions of the SIDD only for low sur-face pressures. Two reasons were given for the mismatch between the experimental and theoretical results:
• The SIDD FEM model is not capable of simulat-ing the behavior of a cracked pipe ction ade-
quately. Although Heger et al. (1985) state that
SPIDA can model uncracked and cracked pipe
ction by using different stiffness for the
beam elements that reprent the pipe ction,
the work by Sargand et al. (1994) showed that
SPIDA needs improvement in modeling the pipe
ction so that formation of cracks can be ade-
quately accounted for.
• SIDD assumes symmetry in geometry and load-ing, which is a common assumption in order to
VAF
Installation
Type
1
2
3
4
VAF
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1.40
1.40
1.45
HAF
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0.37
0.30
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0.62
0.85
1.05
1.45
A2
0.73
0.55
0.35
0.00
A3
1.35
1.40
1.40
1.45
A4
0.19
0.15
0.10
0.00
A5
0.08
0.08
0.10
0.11
A6
0.18
0.17
0.17
0.19
a
1.40
1.45
1.45
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b
0.40
0.40
0.36
0.30
c
0.18
0.19
0.20
0.25
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0.10
0.12
0.00
f
0.05
0.05
0.05
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0.80
0.82
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0.90
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0.80
0.70
0.60
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