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Similar material test study of dynamic failure of jointed rock mass with SHPB
LIU Hong-yan ,DENG Zheng-ding ,WANG Xin-sheng ,ZHANG Ji-hong ,ZHANG Li-min ,
. 2014, 35 (3 ):
659-665.
Failure modes of jointed rock mass with different joint dip angles, joint discontinuity degrees, joint sets, load strain ratios, joint filling thicknesses, joint filling types and slenderness ratios under split Hopkinson pressure bar(SHPB) tests are studied by means of similar material model tests. The results show that failure modes and dynamic strength of jointed rock mass are much related to joint configuration. For rock mass with single joint, its strength and failure characteristics are greatly controlled by the joint dip angle. The dynamic strength of the specimens with joint dip angles of 0° and 90°, whose failure modes are both tensile failure, is 90% and 71% of that of intact one, respectively. The dynamic strength of the specimen with joint dip angle of 60° is nearly zero. The dynamic strength of the specimens with joint dip angles of 30° and 45°, whose failure modes are mainly shear failure with partly tensile failure, is 50% and 18% of that of intact one, respectively. The peak strength of the specimens with 1/4, 1/2, 4/5 and 1 joint center continuity degree is 95%, 74%, 28% and 17% of that of intact one, respectively. With increase of joint discontinuity degree, the dynamic strength of specimen decreases. The dynamic strength of the specimens with 1, 2 and 3 groups of joints is 54%, 23% and 10% of that of intact one, respectively. Namely, with increase of joint group, the dynamic strength of specimen decreases greatly; but its failure mode does not change. With increase of joint filling thickness and strength reduction of joint fillings, the dynamic strength of specimen decreases gradually; but its failure mode does not change. The dynamic strength of the intact and jointed specimens both increase with increasing of load strain ratio; and the sensitivity to load strain ratio of the former is much higher than that of the latter, whose failure mode becomes more complicated accordingly. The dynamic strength of these two kinds of specimens both first increase then decrease with the slenderness ratio; that is to say, there exists a best slenderness ratio.
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