3-D longitudinal and transverse cracking and the influence of non- uniform contact pressure on the stress intensity factors of these Cracks

It has been increasingly and consistently reported that cracking starts at the surface, especially for thicker pavements. The traditional model of bottom-up cracking is well understood and controlled by long life pavement designs. This means that future pavement management should focus on the surface layer deterioration. To this end, this study investigated the Stress Intensity Factors (SIF) of mode one (KI), mode two (KII) and mode three (KIII) cracking at the tip of longitudinal and transverse cracks and as such their influence on the possible continued propagation further into the pavement. The CAPA-3D finite element software was used to model the two cracking scenarios of the longitudinal and transverse cracks with non-uniform contact pressure The results highlighted the impact of the non-uniform contact pressure and the impact of the distance from the load to crack tip. It reveals the sharp changes seen as a tyre passes a crack and the SIFs generated at different positions under/ beside a crack. It is advised that the addition of the potential of crack propagation into the pavement be taken into account in the design of pavements.

[1]  R. Barsoum,et al.  Further application of quadratic isoparametric finite elements to linear fracture mechanics of plate bending and general shells , 1975 .

[2]  S. Benzley Representation of singularities with isoparametric finite elements , 1974 .

[3]  Andy Collop,et al.  Comparison of Small and Large Scale Wheel Tracking Devices , 2009 .

[4]  Linda M Pierce,et al.  Top-Down Cracking in Washington State Asphalt Concrete Wearing Courses , 2000 .

[5]  R. D. Henshell,et al.  CRACK TIP FINITE ELEMENTS ARE UNNECESSARY , 1975 .

[6]  M De Beer,et al.  Overview of South African Mechanistic Pavement Design Method , 1996 .

[7]  Imad L. Al-Qadi,et al.  Impact of Wide-Base Tires on Pavements: Results from Instrumentation Measurements and Modeling Analysis , 2012 .

[8]  David Cebon,et al.  A Theoretical Analysis of Fatigue Cracking in Flexible Pavements , 1995 .

[9]  Andy Collop,et al.  The effects non-uniform contact pressure distribution has on surface distress of flexible pavements using a finite element method , 2012 .

[10]  Esben Byskov,et al.  The calculation of stress intensity factors ssing the finite element method with cracked elements , 1970 .

[11]  B. Ruth,et al.  MECHANISMS OF SURFACE-INITIATED LONGITUDINAL WHEEL PATH CRACKS IN HIGH-TYPE BITUMINOUS PAVEMENTS , 1998 .

[12]  M De Beer,et al.  DETERMINATION OF PNEUMATIC TYRE/PAVEMENT INTERFACE CONTACT STRESSES UNDER MOVING LOADS AND SOME EFFECTS ON PAVEMENTS WITH THIN ASPHALT SURFACING LAYERS , 1997 .

[13]  Morris De Beer,et al.  Overview of the South African mechanistic pavement design analysis method , 1996 .

[14]  R Roque,et al.  EVALUATION OF TOP-DOWN CRACKING IN THICK ASPHALT PAVEMENTS AND THE IMPLICATIONS FOR PAVEMENT DESIGN , 2001 .

[15]  T. Pian,et al.  On the convergence of the finite element method for problems with singularity , 1973 .

[16]  Athanasios Scarpas,et al.  A Mechanics based Computational Platform for Pavement Engineering , 2005 .

[17]  P. F. Walsh The computation of stress intensity factors by a special finite element technique , 1971 .

[18]  Emmanuel G Fernando,et al.  Evaluation of Effects of Tire Size and Inflation Pressure on Tire Contact Stresses and Pavement Response , 2006 .

[19]  Andy Collop,et al.  Report on the Prediction of Surface-Initiated Longitudinal Wheel Path Cracking in Asphalt Pavements , 2004 .

[20]  Bhushan Lal Karihaloo,et al.  Comprehensive structural integrity , 2003 .

[21]  Gilbert Y. Baladi,et al.  Determining the Causes of Top-Down Cracks in Bituminous Pavements , 2003 .

[22]  Andy Collop,et al.  Stress Intensity Factors at the Tip of a Surface Initiated Crack Caused by Different Contact Pressure Distributions , 2012 .