岩土力学
巖土力學
암토역학
ROCK AND SOIL MECHANICS
2010年
1期
32-38
,共7页
杨磊%李术才%郭彦双%朱维申%林春金
楊磊%李術纔%郭彥雙%硃維申%林春金
양뢰%리술재%곽언쌍%주유신%림춘금
砂浆试件%声发射%裂隙间距%起裂应力%峰值强度
砂漿試件%聲髮射%裂隙間距%起裂應力%峰值彊度
사장시건%성발사%렬극간거%기렬응력%봉치강도
mortar material sample%acoustic emission%space between cracks%initiation stress%maximum stress
采用刚性伺服试验机和声发射仪器,研究了预置三维裂隙间距对砂浆材料力学特性的影响,总结了含裂隙试件的破坏过程.综合分析单轴压缩应力-应变曲线和声发射数据可知,含三维裂隙试件的破坏主要由预置裂隙扩展、贯通造成,破坏过程可以分为微裂纹萌生、预置裂隙起裂、扩展、贯通几个基本阶段,试件最终破坏型式为单斜面剪切破坏.裂隙间距d与椭圆形裂隙长轴2c之比(d/2c)在0~1范围内,随着d/2c值增大,试件起裂应力σ_ i和峰值强度σ _p有降低的趋势.当d/2c值从1/3增至2/3时,σ _i和σ _p发生突降,可见此范围为影响强度的敏感区间.d/2c值为1的试件σ _i和σ_ p最低,相对完整(无预置裂隙)试件分别降低了22.48 %和18.60 %.裂隙间距不同的试件σ_ i和σ_ p之比变化范围为83.1 %~78.9 %,且随d/2c值增大,σ_ i / σ_ p有下降趋势.可见裂隙间距越大,从起裂应力到峰值应力的承载空间越大,这对工程实践有一定参考价值.
採用剛性伺服試驗機和聲髮射儀器,研究瞭預置三維裂隙間距對砂漿材料力學特性的影響,總結瞭含裂隙試件的破壞過程.綜閤分析單軸壓縮應力-應變麯線和聲髮射數據可知,含三維裂隙試件的破壞主要由預置裂隙擴展、貫通造成,破壞過程可以分為微裂紋萌生、預置裂隙起裂、擴展、貫通幾箇基本階段,試件最終破壞型式為單斜麵剪切破壞.裂隙間距d與橢圓形裂隙長軸2c之比(d/2c)在0~1範圍內,隨著d/2c值增大,試件起裂應力σ_ i和峰值彊度σ _p有降低的趨勢.噹d/2c值從1/3增至2/3時,σ _i和σ _p髮生突降,可見此範圍為影響彊度的敏感區間.d/2c值為1的試件σ _i和σ_ p最低,相對完整(無預置裂隙)試件分彆降低瞭22.48 %和18.60 %.裂隙間距不同的試件σ_ i和σ_ p之比變化範圍為83.1 %~78.9 %,且隨d/2c值增大,σ_ i / σ_ p有下降趨勢.可見裂隙間距越大,從起裂應力到峰值應力的承載空間越大,這對工程實踐有一定參攷價值.
채용강성사복시험궤화성발사의기,연구료예치삼유렬극간거대사장재료역학특성적영향,총결료함렬극시건적파배과정.종합분석단축압축응력-응변곡선화성발사수거가지,함삼유렬극시건적파배주요유예치렬극확전、관통조성,파배과정가이분위미렬문맹생、예치렬극기렬、확전、관통궤개기본계단,시건최종파배형식위단사면전절파배.렬극간거d여타원형렬극장축2c지비(d/2c)재0~1범위내,수착d/2c치증대,시건기렬응력σ_ i화봉치강도σ _p유강저적추세.당d/2c치종1/3증지2/3시,σ _i화σ _p발생돌강,가견차범위위영향강도적민감구간.d/2c치위1적시건σ _i화σ_ p최저,상대완정(무예치렬극)시건분별강저료22.48 %화18.60 %.렬극간거불동적시건σ_ i화σ_ p지비변화범위위83.1 %~78.9 %,차수d/2c치증대,σ_ i / σ_ p유하강추세.가견렬극간거월대,종기렬응력도봉치응력적승재공간월대,저대공정실천유일정삼고개치.
The rigid serve-controlled test machine and acoustic emission equipment are used to study the influence of space between 3D-cracks on the mechanical feature of mortar material; and the failure process of samples with pre-existing cracks is concluded. The analysis of complete stress-strain curves and AE data indicates that sample failure is due to the propagation and coalescence of cracks. Failure process of samples with pre-existing cracks could be divided into the following stages: microcrack initiation, initiation of pre-existing cracks, crack propagation and crack coalescence. The failure pattern is shear failure along single inclined plane. When the ratio of cracks space d and length of elliptic crack long axis 2c ranging from 0-1, as the ratio grows, the initiation stress and maximum stress of samples reduce. With the ratio d/2c growing from 1/3 to 2/3, the initiation stress and maximum stress fall suddenly, showing that this space scope is the sensitive range. When the ratio d/2c =1, the initiation stress and maximum stress of sample fall 22.48 % and 18.60 % respectively corresponding to the sample without pre-existing cracks. The ratio of initiation stress to maximum stress of all different samples ranges from 83.1 % to 78.9 %. As the ratio d/2c grows, the ratio of initiation stress to maximum stress declines, which indicates that as space d grows, the loading range between initiation stress and maximum stress increase.