2014
DOI: 10.1061/(asce)gm.1943-5622.0000307
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Simplified Mapping Rule for Bounding Surface Simulation of Complex Loading Paths in Granular Materials

Abstract: This paper presents a bounding surface plasticity model that can be used to simulate complex monotonic and cyclic loading paths.A new mapping rule that only uses the last stress reversal point is introduced to describe the stress-strain behavior of granular soils during loading and unloading. This mapping rule is easy to implement and is suitable for highly erratic cyclic loading conditions, e.g., those induced by earth-quake or traffic loading. The application and performance of the model are demonstrated usi… Show more

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Cited by 35 publications
(17 citation statements)
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“…However, the fractional derivative and integral do not commute as shown in the following Eq. (14) ( ) (14) 3 Connections between the fractional order and fractal dimension…”
Section: Definitionsmentioning
confidence: 99%
See 2 more Smart Citations
“…However, the fractional derivative and integral do not commute as shown in the following Eq. (14) ( ) (14) 3 Connections between the fractional order and fractal dimension…”
Section: Definitionsmentioning
confidence: 99%
“…Some of the models [8,14,23] can simulate the real stress strain behaviour but are complex, whereas others [6,12] are relatively simple but cannot take into account the deformation and degradation of granular soils under complicated loading conditions. Most importantly, these models [7,16] can only simulate the cyclic behaviour of granular soils for very limited loading cycles, say less than 100 cycles.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The plastic potential function for soils can be derived from consideration of the energy dissipated during plastic deformation by equating the total plastic work input with the energy dissipated in plastic deformation . This results in the following expression for the plastic potential function g(),,,pqθp0={truet˜0.25emq+A0.25emMcs()θpA1()p/p0A110.25em1.56emitalicfor0.25emA1truet˜0.25emq+Mcs()θpln()p/p05.719998emitalicfor0.25emA=1, where p 0 controls the size of the plastic potential and A is a material constant dependent on the mechanism and amount of energy dissipation (not to be confused with the A parameter of the three‐point time discretisation scheme).…”
Section: Bounding Surface Plasticity Modelmentioning
confidence: 99%
“…The mapping rule adopted in the original model could not be efficiently applied in a boundary value problem with highly variable loading paths due to its complex mapping procedure and memory requirements. To tackle this problem, Kan et al [11] introduced a single stress point radial mapping rule which has a simpler procedure and is more amenable to complex loading paths. 3 In this paper a general method is presented for the treatment of overshooting.…”
Section: Introductionmentioning
confidence: 99%