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大连理工大学高等土力学第3章-3

大连理工大学高等土力学第3章-3
大连理工大学高等土力学第3章-3

高等土力学——No.9 Advanced Soil Mechanics

主讲老师:郭莹

土木工程学院岩土工程研究所

3. 6土的强度理论

3.6.2 土的经典强度理论

1. 特雷斯卡(Tresca)准则及其广义准则

2. 米泽斯(Von Mises)准则及其广义准则

3. 莫尔-库仑(Mohr-Coulomb)强度准则

4. 三个强度准则的讨论

1. 特雷斯卡(Tresca )准则与广义特雷斯卡(Extended Tresca )准则——单剪应力

132k

σσ?=0

2πsin 2=???????

+k J θ0

212πsin 12=???????

?

+I k J αθ()1

231I

k ασσ+=?广义形式

α、I 1反映平均

主应力影响

金属材料

或或

πsin =?????

+k J θ六棱柱的表面:

π平面上的特雷斯卡与米泽斯准则两个破坏面交点,数学处理时有困难

锥面——广义六棱柱面——特

雷斯卡

2. 米泽斯(Von Mises )和广义米泽斯(extended Von Mises )准则——三剪应力

()()()

2

2

132

322

216k

=?+?+?σσσσσσ2

2k

J =k

J =2k

q 3=oct

23

k

τ=或

12=??k I J α033

3

=??k p q α广义米泽斯——Drucker-Prager 准则

α、I 1反映平均

主应力影响

σ1

σ3

σ2

圆锥面——广义米泽斯准则

圆柱面——米泽斯准则

圆形应用起来更方便

3. 莫尔-库仑强度准则——单剪切角

()

f f τσ=莫尔(Mohr )单值函数

13

13sin 2c tan c σσ?σσ??=++f tan c τσ?

=+在一定的应力范围,线性关系-库仑公式

莫尔-库仑强度准则

(二维应力状态)

0cos cos sin sin 31

sin 321=+??

????+??θ?θ?c J I 0

cos cos sin sin 3131sin =+??

?

???+??θ?θ?c q p 莫尔-库仑强度准则的应力不变量表达式

三轴平面

莫尔-库仑强度准则的破坏面与破坏轨迹

三维空间

π平面

非规则六面体

非规则六边形:拉压不等

4. Tresca、Mises和Mohr-Coulomb

三个强度准则的讨论

1)Tresca和Mises都没有考虑平均主应力对土的抗剪强度的影响,不能反映土的摩擦特性;2)广义形式考虑了p,但没有考虑破坏面上正应力的影响;

3)Tresca准则是最大剪应力准则;Mises是最大八面体剪应力准则,两者与土的摩擦强度不同;4)三轴压缩和伸长试验,用Tresca和Mises(拉压相等)预测的强度相同,显然与实际不符;

三个准则在常规三轴压缩试验测得抗剪强度相等。

(θ=-30o)

三维应力空间及π平面(I

或p为常数)

1

π平面

用广义米泽斯及广义特雷斯卡准则预测伸长试验,得出不合实际的结果

o

36.9?′≥(θ= -30o )

(θ=30o )

砂土

用广义米泽斯及广义特雷斯卡准则,将有一个主应力为拉应力(<0)——不可能

Mohr-Coulomb强度准则反映了剪切面上剪应力与正应力的关系以及土作为散粒体的摩擦特性,是比较合理的,在土力学中得到了广泛的应用;

存在问题:

1)与中主应力无关;

2)包线假定线性,即?与围压无关;

应力水平很大时引起较大误差;

3)因为破坏面非光滑连接,数值计算不够方便.

广义Mises在应力空间的曲面和π平面的轨迹光滑,数值计算方便;为避免圆半径过大与实际不符,有时采用伸长圆或折中圆。

π平面-

规则六边形不规则六边形

以内切圆来替代

内切圆

广义米泽斯三轴压缩试验

三轴伸长试验

不同破坏准则在π平面上的轨迹

3. 6土的强度理论

3.6.3 近代的强度理论

1.莱特-邓肯(Lade-Duncan)破坏准则

2.松冈元-中井照夫(Matsuoka-Nakai)

破坏准则

3.双剪应力强度理论

4.隐式的破坏准则.

本构关系-包括应力应变与强度关系

土的强度,或者破坏是其应力应变过程的最后阶段,即在微小的应力增量下,会产生很大(或者不可控制)的应变增量。因而破坏是应力应变关系的最后阶段。——现代强度理论基本思想。

1.莱特-邓肯(Lade-Duncan)破坏准则

适用于砂土的弹塑性模型

不相关联的流动法则

屈服面、塑性势面、破坏面性状一致

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