000 03351nam a2200385 4500
005 20260817162533.0
008 270798 th eng
035 _a.b10083686
099 9 _aAIT Thesis no.ST-90-18
100 1 _aNirmalendran, Sivalingam
245 1 0 _aAnalytical modelling of microcracking and bridging in fracture of concrete, rock and ceramics
260 _aBangkok :
_bAsian Institute of Technology,
_c1990
300 _a46, A-4 p.
490 1 _aThesis ;
_vno. ST-90-18
500 _aA thesis submitted in partial fulfillment of the requirements for the degree of Master of Engineering, School of Engineering and Technology
502 _aThesis (M.Eng.) - Asian Institute of Technology, 1990
520 _aMicrocracking and bridging are major mechanisms in fracture of quasi-brittle materials such as concrete, rock and ceramics. An analytical model of fracture process zone which includes both microcracking and bridging is developed to estimate the effects of microcracking and bridging. While the material property on bridging is represented by the tension-softening curve, which is the inelastic component of post-peak behavior in tension test, that on microcracking is related to the pre-peak nonlinear behavior. Relationship between microcrack density and the stress level is determined from pre-peak stress-strain curve in uniaxial tension test. The material parameters on microcracking are identified through a microcracking law which relates the orientation and the density of microcracks to the state of stress at the point in question. The dominant microcracking parameter is found through the model. With the given material properties on bridging and microcracking, the model predicts the shape and size of the microcracking zone, the distribution of microcrack density and the length of bridging zone at each load level. Results of the present model are compared with those of the model which includes only bridging. It is shown that the increase in toughness due to microcracking varies for different materials but remain_s small portion of the total toughness for real materials. For the case that bridging is dominant, Dugdale-Barenblatt-type model, which includes bridging zone only, serves as a good model of fracture phenomena and provides reasonable estimate of, for example, the maximum load of structures.
650 0 _aFracture mechanics
700 1 _aHorii, Hideyuki,
_eChairperson
700 1 _aKarasudhi, Pisidhi,
_eExamination Committee
700 0 _aWorsak Kanok-Nukulchai,
_eExamination Committee
710 2 _aThe Government of Australia.,
_eScholarship Donor
810 2 _aAsian Institute of Technology.
_tThesis ;
_vno. ST-90-18
856 _3Full-Text
_uhttp://203.159.5.9/ait-thesis/detail.php?q=B18569
907 _a.b10083686
_bmnait
_cs
902 _a240410
998 _b2
_c951012
_dm
_ea
_fs
_g0
945 _lmnait
945 _lmnarc
942 _c22
942 _c40
909 _aBarcode : 30050120692446
_bCREATED : 2014-02-04
_cRECORD # : i1278607x
_dLPATRON : 0
_eLCHKIN : -
_f# RENEWALS : 0
_g# OVERDUE : 0
_hIUSE3 : 0
_iTOT CHKOUT : 0
_jTOT RENEW : 0
909 _aBarcode : 30050160068937
_bCREATED : 2016-08-04
_cRECORD # : i12931470
_dLPATRON : 0
_eLCHKIN : -
_f# RENEWALS : 0
_g# OVERDUE : 0
_hIUSE3 : 0
_iTOT CHKOUT : 0
_jTOT RENEW : 0
999 _c5348
_d5348