我们将从建立描述应力 σ {\displaystyle \sigma } ε {\displaystyle \varepsilon }
图 1 : (a) 作用于物体的外部力 P , {\displaystyle \mathbf {P} ,} A {\displaystyle A} 应力和应变的概念起源于考虑作用于物体上的力和物体的位移。从力开始，可以施加两种类型的力。首先是表面力，它可以是点力，也可以是作用在表面上的分布力。其次是体力，它作用于物体的每个元素，而不仅仅是表面（例如，重力、电场等）。
所关注的物体受到许多力的作用，这些力通过材料传递。在物体内部的任何一点，您可以想象将其切开以观察想象的切割表面上的力，如图 1 所示。这些力是切割面两侧的材料之间的相互作用。我们将物体中某点的应力定义为作用在该想象切割表面的力。
图 2 : 一个具有应力的无穷小长方体材料，根据 ( x 1 , x 2 , x 3 ) {\displaystyle (x_{1},x_{2},x_{3})} 您还记得，应力被定义为力除以作用力的面积。力 P {\displaystyle \mathbf {P} } θ {\displaystyle \theta } σ 33 = P cos θ A {\displaystyle \sigma _{33}={\frac {P\cos \!\theta }{A}}} P sin θ {\displaystyle P\sin \!\theta } x 1 {\displaystyle x_{1}} x 2 {\displaystyle x_{2}} ϕ {\displaystyle \phi } σ 31 = P sin θ cos ϕ A {\displaystyle \sigma _{31}={\frac {P\sin \!\theta \cos \!\phi }{A}}} σ 32 = P sin θ sin ϕ A {\displaystyle \sigma _{32}={\frac {P\sin \!\theta \sin \!\phi }{A}}}
这里需要注意的是，我们定义的坐标系使得 x 3 {\displaystyle x_{3}} ( x 1 , x 2 , x 3 ) {\displaystyle (x_{1},x_{2},x_{3})} ( x , y , z ) {\displaystyle (x,y,z)} σ 33 {\displaystyle \sigma _{33}} x 3 {\displaystyle x_{3}} x 3 {\displaystyle x_{3}} σ 31 {\displaystyle \sigma _{31}} σ 32 {\displaystyle \sigma _{32}} x 3 {\displaystyle x_{3}} x 1 {\displaystyle x_{1}} x 2 {\displaystyle x_{2}} 图2 所示。为了比较，一些教科书中使用的符号将写法向应力为 σ x {\displaystyle \sigma _{x}} σ 11 {\displaystyle \sigma _{11}} τ {\displaystyle \tau } τ x y {\displaystyle \tau _{xy}} σ 12 {\displaystyle \sigma _{12}}
σ = ( σ 11 σ 12 σ 13 σ 21 σ 22 σ 23 σ 31 σ 32 σ 33 ) {\displaystyle \sigma =\left({\begin{aligned}\sigma _{11}\quad \sigma _{12}\quad \sigma _{13}\\\sigma _{21}\quad \sigma _{22}\quad \sigma _{23}\\\sigma _{31}\quad \sigma _{32}\quad \sigma _{33}\end{aligned}}\right)} 图 1 中通过物体上某点切出的想象切片可以是任何平面，但作用力保持不变。这会导致表面法线的定义改变，并可能导致应力表达式发生变化。应力的物理存在不会改变，但描述方式会改变，即坐标系会发生改变。本节的其余部分将重点介绍应力坐标变换的表达和分析。
我们将从简化正在处理的图景开始。平面应力条件存在于薄的二维物体中，例如一张纸，该物体在平面外没有应力。这使我们能够写成 σ 33 = 0 {\displaystyle \sigma _{33}=0} x 3 {\displaystyle x_{3}} σ 13 = σ 23 = 0 {\displaystyle \sigma _{13}=\sigma _{23}=0}
图 3 ：(a) 平面应力条件下定义的面积 A {\displaystyle A} x 1 ′ {\displaystyle x_{1}'} x 1 {\displaystyle x_{1}} θ {\displaystyle \theta } x 1 {\displaystyle x_{1}} x 1 {\displaystyle x_{1}} (b) 图中显示了作用在该面积上的总应力的分量。对于该物体，零力方向为 x 3 {\displaystyle x_{3}} x 1 {\displaystyle x_{1}} x 2 {\displaystyle x_{2}} σ 11 {\displaystyle \sigma _{11}} σ 22 {\displaystyle \sigma _{22}} σ 12 = σ 21 {\displaystyle \sigma _{12}=\sigma _{21}}
想象一个新的区域，它定义在一个绕 x 3 {\displaystyle x_{3}} x 1 ′ {\displaystyle x_{1}'} x 1 {\displaystyle x_{1}} θ {\displaystyle \theta }
作用在该区域上的力的分量由原始应力作用在新区域的投影面上确定。
F 1 = σ 11 A cos θ + σ 12 A sin θ = S 1 A F 2 = σ 22 A sin θ + σ 12 A cos θ = S 2 A {\displaystyle {\begin{aligned}F_{1}=\sigma _{11}A\cos \!\theta +\sigma _{12}A\sin \!\theta =S_{1}A\\F_{2}=\sigma _{22}A\sin \!\theta +\sigma _{12}A\cos \!\theta =S_{2}A\end{aligned}}} [1 & 2] 其中元素 A cos θ {\displaystyle A\cos \!\theta } A sin θ {\displaystyle A\sin \!\theta } 图 3 (a) 所示，以及 S 1 {\displaystyle S_{1}} S 2 {\displaystyle S_{2}} x 1 {\displaystyle x_{1}} x 2 {\displaystyle x_{2}} σ 12 = σ 21 {\displaystyle \sigma _{12}=\sigma _{21}}
S 1 = σ 11 cos θ + σ 12 sin θ S 2 = σ 22 sin θ + σ 12 cos θ {\displaystyle {\begin{aligned}S_{1}=\sigma _{11}\cos \!\theta +\sigma _{12}\sin \!\theta \\S_{2}=\sigma _{22}\sin \!\theta +\sigma _{12}\cos \!\theta \end{aligned}}} [3 & 4] 将图 3 (b) 所示的总应力投影到 x 1 ′ {\displaystyle x_{1}'}
σ 11 ′ = S 1 cos θ + S 2 sin θ {\displaystyle \sigma _{11}'=S_{1}\!\cos \!\theta +S_{2}\!\sin \!\theta } [5] 类似地，我们将切线投影到平面并得到
σ 12 ′ = S 2 cos θ − S 1 sin θ {\displaystyle \sigma _{12}'=S_{2}\!\cos \!\theta -S_{1}\!\sin \!\theta } [6] 得到
σ 11 ′ = ( σ 11 cos θ + σ 12 sin θ ) cos θ + ( σ 22 sin θ + σ 12 cos θ ) sin θ = σ 11 cos 2 θ + σ 22 sin 2 θ + 2 σ 12 sin θ cos θ {\displaystyle {\begin{aligned}\sigma _{11}'&=(\sigma _{11}\cos \!\theta +\sigma _{12}\sin \!\theta )\cos \!\theta +(\sigma _{22}\sin \!\theta +\sigma _{12}\cos \!\theta )\sin \!\theta \\&=\sigma _{11}\cos ^{2}\!\theta +\sigma _{22}\sin ^{2}\!\theta +2\ \sigma _{12}\sin \!\theta \cos \!\theta \end{aligned}}} [7] 和
σ 12 ′ = ( σ 22 sin θ + σ 12 cos θ ) cos θ − ( σ 11 cos θ + σ 12 sin θ ) sin θ = σ 12 ( c o s 2 θ − sin 2 θ ) + ( σ 22 − σ 11 ) sin θ cos θ {\displaystyle {\begin{aligned}\sigma _{12}'&=(\sigma _{22}\sin \!\theta +\sigma _{12}\cos \!\theta )\cos \!\theta -(\sigma _{11}\cos \!\theta +\sigma _{12}\sin \!\theta )\sin \!\theta \\&=\sigma _{12}(cos^{2}\!\theta -\sin ^{2}\!\theta )+(\sigma _{22}-\sigma _{11})\sin \!\theta \cos \!\theta \end{aligned}}} [8] 图 4 : 一个新的区域，它相对于图 3 中所示的原始区域旋转了 π 2 {\displaystyle {\frac {\pi }{2}}} 已知 σ 12 ′ = σ 21 ′ {\displaystyle \sigma _{12}'=\sigma _{21}'} σ 22 ′ {\displaystyle \sigma _{22}'} π {\textstyle \pi }
S 1 A = σ 11 A cos ( θ + π 2 ) + σ 12 A sin ( θ + π 2 ) S 1 = − σ 11 sin θ + σ 12 cos θ {\displaystyle {\begin{aligned}S_{1}A&=\sigma _{11}A\cos(\theta +{\pi \over 2})+\sigma _{12}A\sin(\theta +{\pi \over 2})\\S_{1}&=-\sigma _{11}\sin \!\theta +\sigma _{12}\cos \!\theta \end{aligned}}} [9] 和
S 2 A = σ 22 A sin ( θ + π 2 ) + σ 12 A cos ( θ + π 2 ) S 2 = σ 22 cos θ − σ 12 sin θ {\displaystyle {\begin{aligned}S_{2}A&=\sigma _{22}A\sin(\theta +{\pi \over 2})+\sigma _{12}A\cos(\theta +{\pi \over 2})\\S_{2}&=\sigma _{22}\cos \!\theta -\sigma _{12}\sin \!\theta \end{aligned}}} [10] 将总应力投影到法线方向得到
σ 22 ′ = S 1 cos ( θ + π 2 ) + S 2 sin ( θ + π θ ) = − S x 1 sin θ + S x 2 cos θ {\displaystyle {\begin{aligned}\sigma _{22}'&=S_{1}\cos(\theta +{\pi \over 2})+S_{2}\sin(\theta +{\pi \over \theta })\\&=-S_{x_{1}}\sin \!\theta +S_{x_{2}}\cos \!\theta \end{aligned}}} [11] 将公式 9 和10 代入公式 11 中的 S 1 {\displaystyle S_{1}} S 2 {\displaystyle S_{2}} σ 22 ′ {\displaystyle \sigma _{22}'}
σ 22 ′ = − ( − σ 11 sin θ + σ 12 cos θ ) sin θ + ( σ 22 cos θ − σ 12 sin θ ) cos θ = σ 11 sin 2 θ + σ 22 cos 2 θ − 2 σ 12 sin θ cos θ {\displaystyle {\begin{aligned}\sigma _{22}'&=-(-\sigma _{11}\sin \!\theta +\sigma _{12}\cos \!\theta )\sin \!\theta +(\sigma _{22}\cos \!\theta -\sigma _{12}\sin \!\theta )\cos \!\theta \\&=\sigma _{11}\sin ^{2}\!\theta +\sigma _{22}\cos ^{2}\!\theta -2\ \sigma _{12}\sin \!\theta \cos \!\theta \end{aligned}}} [12] 众所周知的三角恒等式
cos 2 θ = cos 2 θ + 1 2 sin 2 θ = 1 − cos 2 θ 2 2 sin θ cos θ = sin 2 θ cos 2 θ − sin 2 θ = cos 2 θ {\displaystyle {\begin{array}{lcl}\cos ^{2}\!\theta ={\cos 2\theta +1 \over 2}&\quad &\sin ^{2}\!\theta ={1-\cos 2\theta \over 2}\\2\sin \!\theta \cos \!\theta =\sin 2\theta &&\cos ^{2}\!\theta -\sin ^{2}\theta =\cos 2\theta \end{array}}} 分别应用于公式 7 、8 和12 中的 σ 11 ′ {\displaystyle \sigma _{11}'} σ 12 ′ {\displaystyle \sigma _{12}'} σ 22 ′ {\displaystyle \sigma _{22}'}
σ 11 ′ = σ 11 + σ 22 2 + σ 11 − σ 22 2 cos 2 θ + σ 12 sin 2 θ {\displaystyle {\begin{aligned}\sigma _{11}'&={\sigma _{11}+\sigma _{22} \over 2}+{\sigma _{11}-\sigma _{22} \over 2}\cos {2\theta }+\sigma _{12}\sin {2\theta }\end{aligned}}} [13] σ 22 ′ = σ 11 + σ 22 2 − σ 11 − σ 22 2 cos 2 θ − σ 12 sin 2 θ {\displaystyle {\begin{aligned}\sigma _{22}'&={\sigma _{11}+\sigma _{22} \over 2}-{\sigma _{11}-\sigma _{22} \over 2}\cos {2\theta }-\sigma _{12}\sin {2\theta }\end{aligned}}} [14] 和
σ 12 ′ = σ 22 − σ 11 2 sin 2 θ + σ 12 cos 2 θ {\displaystyle {\begin{aligned}\sigma _{12}'&={\sigma _{22}-\sigma _{11} \over 2}\sin 2\theta +\sigma _{12}\cos 2\theta \end{aligned}}} [15] 从这个推导中可以得到许多直接结果，从这些结果中我们可以获得更深入的见解。从 σ ′ {\displaystyle \sigma '} σ 11 ′ + σ 22 ′ = σ 11 + σ 22 {\displaystyle \sigma _{11}'+\sigma _{22}'=\sigma _{11}+\sigma _{22}} θ {\displaystyle \theta } σ {\displaystyle {\boldsymbol {\sigma }}}
第二个结果是，最大法向应力和剪切应力以周期为 π {\displaystyle \pi } π {\displaystyle \pi } π {\displaystyle \pi } π {\displaystyle \pi }
任何应力状态都可以旋转，以产生 σ 12 = σ 21 = 0 {\displaystyle \sigma _{12}=\sigma _{21}=0} σ p 1 {\displaystyle \sigma _{p1}} σ p 2 {\displaystyle \sigma _{p2}} σ p 3 {\displaystyle \sigma _{p3}} σ p 1 {\displaystyle \sigma _{p1}} σ p 2 {\displaystyle \sigma _{p2}}
我们知道 σ 12 = 0 {\displaystyle \sigma _{12}=0} 方程式 8 来表示 σ 12 ′ {\displaystyle \sigma _{12}'} σ {\displaystyle {\boldsymbol {\sigma }}} σ ′ {\displaystyle \sigma '} θ {\displaystyle \theta }
0 = σ 12 ′ = σ 21 ′ 0 = σ 12 ( cos 2 θ − sin 2 θ ) + ( σ 22 − σ 11 ) sin θ cos θ − ( σ 22 − σ 11 ) sin θ cos θ = σ 12 ( cos 2 θ − sin 2 θ ) sin θ cos θ cos 2 θ − sin 2 θ = σ 12 σ 11 − σ 22 {\displaystyle {\begin{aligned}0&=\sigma _{12}'=\sigma _{21}'\\0&=\sigma _{12}(\cos ^{2}\!\theta -\sin ^{2}\!\theta )+(\sigma _{22}-\sigma _{11})\sin \!\theta \cos \!\theta \\-(\sigma _{22}-\sigma _{11})\sin \!\theta \cos \!\theta &=\sigma _{12}(\cos ^{2}\!\theta -\sin ^{2}\!\theta )\\{\sin \!\theta \cos \!\theta \over \cos ^{2}\!\theta -\sin ^{2}\!\theta }&={\sigma _{12} \over \sigma _{11}-\sigma _{22}}\end{aligned}}} 得到
tan 2 θ = 2 σ 12 σ 11 − σ 22 {\displaystyle {\begin{aligned}\tan 2\theta &={2\ \sigma _{12} \over \sigma _{11}-\sigma _{22}}\end{aligned}}} [16] 如图 5 所示，通过绘制 tan 2 θ {\displaystyle \tan 2\theta } π {\textstyle \pi }
图 5 : t a n 2 θ {\displaystyle tan2\theta } π 2 {\displaystyle {\frac {\pi }{2}}} 对于一个简单的直角三角形，斜边为 c {\displaystyle c} a {\displaystyle a} b {\displaystyle b}
sin ξ = b c cos ξ = a c tan ξ = b a {\displaystyle {\begin{aligned}\sin \xi ={b \over c}\\\cos \xi ={a \over c}\\\tan \xi ={b \over a}\end{aligned}}} 这可以与勾股定理 a 2 + b 2 = c 2 {\displaystyle a^{2}+b^{2}=c^{2}}
a = σ 12 b = 1 2 ( σ 11 − σ 22 ) c = ± ( 1 4 ( σ 11 − σ 22 ) 2 + σ 12 2 ) 1 2 {\displaystyle {\begin{aligned}a&=\sigma _{12}\\b&={1 \over 2}(\sigma _{11}-\sigma _{22})\\c&=\pm \left({1 \over 4}(\sigma _{11}-\sigma _{22})^{2}+{\sigma _{12}}^{2}\right)^{1 \over 2}\end{aligned}}} 这些可以进一步组合，得到
sin 2 θ = ± σ 12 ( 1 4 ( σ 11 − σ 22 ) 2 + σ 12 2 ) 1 2 {\displaystyle {\begin{aligned}\sin 2\theta &=\pm {\sigma _{12} \over \left({1 \over 4}(\sigma _{11}-\sigma _{22})^{2}+{\sigma _{12}}^{2}\right)^{1 \over 2}}\end{aligned}}} [17] 和
cos 2 θ = ± 1 2 ( σ 11 − σ 22 ) ( 1 4 ( σ 11 − σ 22 ) 2 + σ 12 2 ) 1 2 {\displaystyle {\begin{aligned}\\\cos 2\theta &=\pm {{1 \over 2}(\sigma _{11}-\sigma _{22}) \over \left({1 \over 4}(\sigma _{11}-\sigma _{22})^{2}+{\sigma _{12}}^{2}\right)^{1 \over 2}}\end{aligned}}} [18] 这些方程式告诉我们，对于给定的应力状态， σ {\displaystyle \sigma } σ {\displaystyle \sigma }
将这些方程式代入公式 13 中的 σ 11 ′ {\displaystyle \sigma _{11}'}
σ p = σ 11 + σ 22 2 + σ 11 − σ 22 2 ( ± 1 2 ( σ 11 − σ 22 ) ( 1 4 ( σ 11 − σ 22 ) 2 + σ 12 2 ) 1 2 ) + σ 12 ( σ 12 ± ( 1 4 ( σ 11 − σ 22 ) 2 + σ 12 2 ) 1 2 ) = σ 11 + σ 22 2 + 1 4 ( σ 11 − σ 22 ) 2 ± ( 1 4 ( σ 11 − σ 22 ) 2 + σ 12 2 ) 1 2 + σ 12 2 ± ( 1 4 ( σ 11 − σ 22 ) 2 + 得到
= σ 11 + σ 22 2 ± ( 1 4 ( σ 11 − σ 22 ) 2 + σ 12 2 ) 1 2 {\displaystyle {\begin{aligned}&={\sigma _{11}+\sigma _{22} \over 2}\pm \left({1 \over 4}(\sigma _{11}-\sigma _{22})^{2}+{\sigma _{12}}^{2}\right)^{1 \over 2}\end{aligned}}} [19] 使用公式 19 代入公式 16 中，求解 θ {\displaystyle \theta } 0 < θ < π 4 {\displaystyle 0<\theta <{\pi \over 4}}
为了找到最大剪切应力，我们将简化的公式 15 对 σ 12 ′ {\displaystyle \sigma _{12}'} 0 {\displaystyle 0}
0 = d d θ ( σ 22 − σ 11 2 sin 2 θ + σ 12 cos 2 θ ) = 2 σ 22 − σ 11 2 cos 2 θ − 2 σ 12 sin 2 θ = ( σ 22 − σ 11 ) cos 2 θ − 2 σ 12 sin 2 θ {\displaystyle {\begin{aligned}0&={\operatorname {d} \over \operatorname {d} \!\theta }\left({\sigma _{22}-\sigma _{11} \over 2}\sin 2\theta +\sigma _{12}\cos 2\theta \right)\\&=2{\sigma _{22}-\sigma _{11} \over 2}\cos 2\theta -2\sigma _{12}\sin 2\theta \\&=(\sigma _{22}-\sigma _{11})\cos 2\theta -2\sigma _{12}\sin 2\theta \end{aligned}}} 得到关于 2 θ {\displaystyle 2\theta }
σ 22 − σ 11 2 σ 12 = sin 2 θ cos 2 θ = tan 2 θ {\displaystyle {\begin{aligned}\\{\sigma _{22}-\sigma _{11} \over 2\ \sigma _{12}}&={\sin 2\theta \over \cos 2\theta }=\tan 2\theta \end{aligned}}} [20] 注意到公式 20 和公式 16 是负倒数关系，这意味着 2 θ p {\displaystyle 2\theta _{p}} 2 θ M A X {\displaystyle 2\theta _{MAX}} π {\displaystyle \pi }
tan ϕ = a b tan ϕ + π 2 = − b a {\displaystyle {\begin{aligned}\tan \phi ={\frac {a}{b}}\\\tan \phi +{\frac {\pi }{2}}={\frac {-b}{a}}\end{aligned}}} 这意味着 2 θ p {\displaystyle 2\theta _{p}} 2 θ M A X {\displaystyle 2\theta _{MAX}} π {\displaystyle \pi } σ 12 M A X {\displaystyle \sigma _{12MAX}}
σ 12 M A X = ± [ ( σ 11 − σ 22 2 ) 2 + σ 12 2 ] 1 2 {\displaystyle \sigma _{12MAX}=\pm \left[\left({\sigma _{11}-\sigma _{22} \over 2}\right)^{2}+{\sigma _{12}}^{2}\right]^{1 \over 2}} [21] 一个方便可视化角度关系的方法是使用莫尔圆，我们将在下面推导。对 **方程** **13** 关于 σ 11 ′ {\displaystyle \sigma _{11}'} σ 12 ′ {\displaystyle \sigma _{12}'}
σ 11 ′ − σ 11 + σ 22 2 = σ 11 − σ 22 2 cos 2 θ + σ 12 sin 2 θ {\displaystyle {\begin{aligned}\sigma _{11}'-{\sigma _{11}+\sigma _{22} \over 2}&={\sigma _{11}-\sigma _{22} \over 2}\cos {2\theta }+\sigma _{12}\sin {2\theta }\end{aligned}}} [22] σ 12 ′ = σ 22 − σ 11 2 sin 2 θ + σ 12 cos 2 θ {\displaystyle {\begin{aligned}\sigma _{12}'={\sigma _{22}-\sigma _{11} \over 2}\sin {2\theta }+\sigma _{12}\cos {2\theta }\end{aligned}}} [23] 对这两个表达式进行平方，
( σ 11 ′ − σ 11 + σ 22 2 ) 2 = ( σ 11 − σ 22 2 cos 2 θ + σ 12 sin 2 θ ) 2 {\displaystyle {\begin{aligned}\left(\sigma _{11}'-{\sigma _{11}+\sigma _{22} \over 2}\right)^{2}&=\left({\sigma _{11}-\sigma _{22} \over 2}\cos {2\theta }+\sigma _{12}\sin {2\theta }\right)^{2}\end{aligned}}} ( σ 12 ′ ) 2 = ( σ 22 − σ 11 2 sin 2 θ + σ 12 cos 2 θ ) 2 {\displaystyle {\begin{aligned}\left(\sigma _{12}'\right)^{2}&=\left({\sigma _{22}-\sigma _{11} \over 2}\sin 2\theta +\sigma _{12}\cos 2\theta \right)^{2}\end{aligned}}} 接下来，将它们加在一起得到
( σ 11 ′ − σ 11 + σ 22 2 ) 2 + σ 12 ′ 2 = ( σ 11 − σ 22 2 ) 2 ( cos 2 2 θ + sin 2 2 θ ) + σ 12 2 ( cos 2 2 θ + sin 2 2 θ ) ( σ 11 ′ − σ 11 + σ 22 2 ) 2 + σ 12 ′ 2 = ( σ 11 − σ 22 2 ) 2 + σ 12 2 {\displaystyle {\begin{aligned}\left(\sigma _{11}'-{\sigma _{11}+\sigma _{22} \over 2}\right)^{2}+{\sigma _{12}'}^{2}&=\left({\sigma _{11}-\sigma _{22} \over 2}\right)^{2}(\cos ^{2}\!2\theta +\sin ^{2}\!2\theta )+{\sigma _{12}}^{2}(\cos ^{2}\!2\theta +\sin ^{2}\!2\theta )\\{\left(\sigma _{11}'-{\sigma _{11}+\sigma _{22} \over 2}\right)^{2}}+{\sigma _{12}'}^{2}&=\left({\sigma _{11}-\sigma _{22} \over 2}\right)^{2}+{\sigma _{12}}^{2}\end{aligned}}} 得到的表达式是圆的方程： ( x − h ) 2 + y 2 = r 2 {\displaystyle (x-h)^{2}+y^{2}=r^{2}}
图 6 ：平面应力条件下的莫尔圆。初始应力状态为 σ {\displaystyle \sigma } θ {\displaystyle \theta } σ ′ {\displaystyle \sigma '} 2 θ {\displaystyle 2\theta } ( σ 11 ′ − σ 11 + σ 22 2 ) 2 ⏟ ( x − h ) 2 + σ 12 ′ 2 ⏟ y 2 = ( σ 11 − σ 22 2 ) 2 + σ 12 2 ⏟ r 2 {\displaystyle \underbrace {\left(\sigma _{11}'-{\sigma _{11}+\sigma _{22} \over 2}\right)^{2}} _{(x-h)^{2}}+\underbrace {{\sigma _{12}'}^{2}} _{y^{2}}=\underbrace {\left({\sigma _{11}-\sigma _{22} \over 2}\right)^{2}+{\sigma _{12}}^{2}} _{r^{2}}} [24] 从该表达式中，在图 6 中绘制了莫尔圆。对于给定的应力状态， σ {\displaystyle \sigma } h = σ 11 − σ 22 2 {\displaystyle h={\frac {\sigma _{11}-\sigma _{22}}{2}}} r = ( ( σ 11 − σ 11 2 ) 2 + σ 12 2 ) 1 2 {\displaystyle r=\left(\left({\frac {\sigma _{11}-\sigma _{11}}{2}}\right)^{2}+\sigma _{12}^{2}\right)^{\frac {1}{2}}} σ 11 {\displaystyle \sigma _{11}} σ 22 {\displaystyle \sigma _{22}} σ 12 {\displaystyle \sigma _{12}} 2 π {\displaystyle 2\pi } ϕ {\displaystyle \phi } 2 π {\displaystyle 2\pi } π {\displaystyle \pi } θ = π {\displaystyle \theta =\pi } π {\displaystyle \pi } θ = π {\displaystyle \theta =\pi } σ {\displaystyle \sigma }
从二维泛化到三维，我们从一个双轴平面应力系统过渡到一个三轴系统。确定主轴和角关系类似于二维情况，将在下面说明。注意，按照惯例，当三个主应力中的两个相等时，我们称该系统为“圆柱形”，如果所有三个主应力都相等，我们称该系统为“静水压力”或“球形”。
与双轴系统的情况类似，我们首先定义一个面积为 A {\displaystyle A} x 1 {\displaystyle x_{1}} x 2 {\displaystyle x_{2}} x 3 {\displaystyle x_{3}} 7 所示。该平面在 ( J {\displaystyle J} K {\displaystyle K} L {\displaystyle L}
定义 ℓ {\displaystyle \ell } m {\displaystyle m} n {\displaystyle n} x 1 {\displaystyle x_{1}} x 2 {\displaystyle x_{2}} x 3 {\displaystyle x_{3}} x 1 {\displaystyle x_{1}} x 2 {\displaystyle x_{2}} x 3 {\displaystyle x_{3}} i ^ {\displaystyle {\hat {i}}} j ^ {\displaystyle {\hat {j}}} k ^ {\displaystyle {\hat {k}}}
图 7 : 穿过 x、y、z 坐标系的 3D 坐标平面 JKL ，其中 O {\displaystyle O} ℓ = cos θ 1 = i ^ ⋅ σ | σ | m = cos θ 2 = j ^ ⋅ σ | σ | ; n = cos θ 3 = k ^ ⋅ σ | σ | {\displaystyle \ell =\cos \theta _{1}={{\hat {i}}\cdot {\boldsymbol {\sigma }} \over |{\boldsymbol {\sigma |}}}\quad m=\cos \theta _{2}={{\hat {j}}\cdot {\boldsymbol {\sigma }} \over |{\boldsymbol {\sigma |}}};\quad n=\cos \theta _{3}={{\hat {k}}\cdot {\boldsymbol {\sigma }} \over |{\boldsymbol {\sigma |}}}}}} 应力沿 x 1 {\displaystyle x_{1}} x 2 {\displaystyle x_{2}} x 3 {\displaystyle x_{3}} S 1 {\displaystyle S_{1}} S 2 {\displaystyle S_{2}} S 3 {\displaystyle S_{3}}
S 1 = σ p ℓ ; S 2 = σ p m ; S 3 = σ p n {\displaystyle S_{1}=\sigma _{p}\ell ;\quad S_{2}=\sigma _{p}m;\quad S_{3}=\sigma _{p}n} 在双轴推导中，面积被投影到三个方向，在 **图 7** 中产生三角形，面积分别为 L O K = A ℓ {\displaystyle LOK=A\ell } J O L = A m {\displaystyle JOL=Am} J O K = A n {\displaystyle JOK=An}
S 1 A = σ p ℓ A = F x = L O K σ 11 + J O L σ 21 + J O K σ 31 + = A ℓ σ 11 + A m σ 21 + A n σ 31 {\displaystyle {\begin{aligned}S_{1}A=\sigma _{p}\ell A=F_{x}&=LOK\sigma _{11}+JOL\sigma _{21}+JOK\sigma _{31}+\\&=A\ell \sigma _{11}+Am\sigma _{21}+An\sigma _{31}\end{aligned}}} 所以，
σ p ℓ = σ 11 ℓ + σ 21 m + σ 31 n {\displaystyle {\begin{aligned}\sigma _{p}\ell &=\sigma _{11}\ell +\sigma _{21}m+\sigma _{31}n\end{aligned}}} [25] 通过类似的过程， F x 2 {\displaystyle F_{x_{2}}} F x 3 {\displaystyle F_{x_{3}}}
σ p m = σ 12 ℓ + σ 22 m + σ 32 n {\displaystyle {\begin{aligned}\sigma _{p}m&=\sigma _{12}\ell +\sigma _{22}m+\sigma _{32}n\end{aligned}}} [26] σ p n = σ 13 ℓ + σ 23 m + σ 33 n {\displaystyle {\begin{aligned}\sigma _{p}n&=\sigma _{13}\ell +\sigma _{23}m+\sigma _{33}n\end{aligned}}} [27] 这些方程可以重新整理为
0 = ( σ 11 − σ p ) ℓ + σ 12 m + σ 13 n {\displaystyle {\begin{aligned}0&=(\sigma _{11}-\sigma _{p})\ell +\sigma _{12}m+\sigma _{13}n\end{aligned}}} [28] 0 = σ 12 ℓ + ( σ 22 − σ p ) m + σ 23 n {\displaystyle {\begin{aligned}0&=\sigma _{12}\ell +(\sigma _{22}-\sigma _{p})m+\sigma _{23}n\end{aligned}}} [29] 0 = σ 13 ℓ + σ 23 m + ( σ 33 − σ p ) n {\displaystyle {\begin{aligned}0&=\sigma _{13}\ell +\sigma _{23}m+(\sigma _{33}-\sigma _{p})n\end{aligned}}} [30] 这一组方程可以解出 [ ℓ , m , n ] {\displaystyle \left[\ell ,m,n\right]} σ p {\displaystyle \sigma _{p}} σ p {\displaystyle \sigma _{p}} [ ℓ , m , n ] {\displaystyle \left[\ell ,m,n\right]} ℓ , m , {\displaystyle \ell ,m,} n {\displaystyle n}
d e t | σ 11 − σ p σ 12 σ 13 σ 12 σ 22 − σ p σ 23 σ 13 σ 23 σ 33 − σ p | {\displaystyle det\ \left|{\begin{matrix}\sigma _{11}-\sigma _{p}&\sigma _{12}&\sigma _{13}\\\sigma _{12}&\sigma _{22}-\sigma _{p}&\sigma _{23}\\\sigma _{13}&\sigma _{23}&\sigma _{33}-\sigma _{p}\end{matrix}}\right|} 设为零并解出特征值和随后的特征向量。
重新排列后，我们得到
0 = σ p 3 − ( σ 11 + σ 22 + σ 33 ) σ p 2 + ( σ 11 σ 22 + σ 22 σ 33 + + σ 33 σ 11 − σ 12 2 − σ 23 2 − σ 31 2 ) σ p − ( σ 11 σ 22 σ 33 + 2 σ 12 σ 23 σ 31 − σ 11 σ 23 2 − σ 22 σ 13 2 − σ 33 σ 12 2 ) {\displaystyle {\begin{aligned}0={\sigma _{p}}^{3}-&(\sigma _{11}+\sigma _{22}+\sigma _{33}){\sigma _{p}}^{2}\\&\quad +(\sigma _{11}\sigma _{22}+\sigma _{22}\sigma _{33}++\sigma _{33}\sigma _{11}-{\sigma _{12}}^{2}-{\sigma _{23}}^{2}-{\sigma _{31}}^{2})\sigma _{p}\\&\qquad \qquad -(\sigma _{11}\sigma _{22}\sigma _{33}+2\sigma _{12}\sigma _{23}\sigma _{31}-\sigma _{11}{\sigma _{23}}^{2}-\sigma _{22}{\sigma _{13}}^{2}-\sigma _{33}{\sigma _{12}}^{2})\end{aligned}}} [31] 该三次方程的三个根给出主应力， σ p 1 {\displaystyle \sigma _{p1}} σ p 2 {\displaystyle \sigma _{p2}} σ p 3 {\displaystyle \sigma _{p3}} 方程 28-30 以确定对应于 [ ℓ , m , n ] {\displaystyle \left[\ell ,m,n\right]} ℓ 2 + m 2 + n 2 = 1 {\displaystyle \ell ^{2}+m^{2}+n^{2}=1}
求解三次方程不是本文的重点，但方程 31 很重要，因为主应力前面的系数必须是不变的，也就是说，无论坐标系的方位如何，都必须存在相同的主坐标。从三次方程可以看出，三个不变量是
I 1 = ( σ 11 + σ 22 + σ 33 ) {\displaystyle {\begin{aligned}I_{1}=(\sigma _{11}+\sigma _{22}+\sigma _{33})\end{aligned}}} [32] I 2 = ( σ 11 σ 22 + σ 22 σ 33 + σ 33 σ 11 − σ 12 2 − σ 23 2 − σ 31 2 ) {\displaystyle {\begin{aligned}I_{2}=(\sigma _{11}\sigma _{22}+\sigma _{22}\sigma _{33}+\sigma _{33}\sigma _{11}-{\sigma _{12}}^{2}-{\sigma _{23}}^{2}-{\sigma _{31}}^{2})\end{aligned}}} [33] I 3 = ( σ 11 σ 22 σ 33 + 2 σ 12 σ 23 σ 31 − σ 11 σ 23 2 − σ 22 σ 13 2 − σ 33 σ 12 2 ) {\displaystyle {\begin{aligned}I_{3}=(\sigma _{11}\sigma _{22}\sigma _{33}+2\sigma _{12}\sigma _{23}\sigma _{31}-\sigma _{11}{\sigma _{23}}^{2}-\sigma _{22}{\sigma _{13}}^{2}-\sigma _{33}{\sigma _{12}}^{2})\end{aligned}}} [34] 这很有用，因为这些不变量关系决定了不同方向上应力之间的关系，即给定 σ {\displaystyle \sigma } σ 1 {\displaystyle \sigma _{1}} σ 2 {\displaystyle \sigma _{2}} σ 3 {\displaystyle \sigma _{3}}
现在，我们将把我们的解决方案推广到不仅包括主应力。就像我们之前做的那样，我们可以写出总的力
S x 1 A = F x 1 = σ 11 ℓ A + σ 12 m A + σ 31 n A {\displaystyle {\begin{aligned}S_{x_{1}}A=F_{x_{1}}=\sigma _{11}\ell A+\sigma _{12}mA+\sigma _{31}nA\end{aligned}}} S x 1 = σ 11 ℓ + σ 12 m + σ 33 n {\displaystyle {\begin{aligned}\qquad S_{x_{1}}=\sigma _{11}\ell +\sigma _{12}m+\sigma _{33}n\end{aligned}}} [35] S x 2 = σ 12 ℓ + σ 22 m + σ 23 n {\displaystyle {\begin{aligned}\qquad S_{x_{2}}=\sigma _{12}\ell +\sigma _{22}m+\sigma _{23}n\end{aligned}}} [36] S x 3 = σ 13 ℓ + σ 23 m + σ 33 n {\displaystyle {\begin{aligned}\qquad S_{x_{3}}=\sigma _{13}\ell +\sigma _{23}m+\sigma _{33}n\end{aligned}}} [37] 这些公式给出了总应力
S 2 = S x 1 2 + S x 2 2 + S x 3 2 {\displaystyle S^{2}={S_{x_{1}}}^{2}+{S_{x_{2}}}^{2}+{S_{x_{3}}}^{2}} [38] 由此，法向分量的投影为
σ ′ = S x 1 ℓ + S x 2 m + S x 3 n {\displaystyle \sigma '=S_{x_{1}}\ell +S_{x_{2}}m+S_{x_{3}}n} [39] 将 **公式** **34-36** 代入 **公式** **38** 中，得到
σ ′ = ( σ 11 ℓ + σ 12 m + σ 31 n ) ℓ + ( σ 12 ℓ + σ 22 m + σ 31 n ) m + ( σ 13 ℓ + σ 31 m + σ 33 n ) n {\displaystyle {\begin{aligned}\sigma '&=(\sigma _{11}\ell +\sigma _{12}m+\sigma _{31}n)\ \ell +(\sigma _{12}\ell +\sigma _{22}m+\sigma _{31}n)\ m+(\sigma _{13}\ell +\sigma _{31}m+\sigma _{33}n)\ n\end{aligned}}} 简化为
σ ′ = σ 11 ℓ 2 + σ 22 m 2 + σ 33 n 2 + 2 σ 12 ℓ m + 2 σ 23 m n + 2 σ 31 n ℓ {\displaystyle \sigma '=\sigma _{11}\ell ^{2}+\sigma _{22}m^{2}+\sigma _{33}n^{2}+2\sigma _{12}\ell m+2\sigma _{23}mn+2\sigma _{31}n\ell } [40] 剪切分量的幅值可以通过利用 S 2 = σ ′ 2 + τ 2 {\displaystyle S^{2}={\sigma '}^{2}+\tau ^{2}} σ 11 = σ p 1 {\displaystyle \sigma _{11}=\sigma _{p_{1}}} σ 22 = σ p 2 {\displaystyle \sigma _{22}=\sigma _{p_{2}}} σ 33 = σ p 3 {\displaystyle \sigma _{33}=\sigma _{p_{3}}} 公式 39 被改写为
σ ′ = σ p 1 ℓ 2 + σ p 2 m 2 + σ p 3 n 2 {\displaystyle \sigma '=\sigma _{p_{1}}\ell ^{2}+\sigma _{p_{2}}m^{2}+\sigma _{p_{3}}n^{2}} [41] 对该公式进行平方运算，我们得到
σ ′ 2 = σ p 1 2 ℓ 4 + σ p 2 2 m 4 + σ p 3 2 n 4 + 2 σ p 1 σ p 2 ℓ 2 m 2 + 2 σ p 1 σ p 3 ℓ 2 n 2 + 2 σ p 2 σ p 3 m 2 n 2 p {\displaystyle {\sigma '}^{2}={\sigma _{p_{1}}}^{2}\ell ^{4}+{\sigma _{p_{2}}}^{2}m^{4}+{\sigma _{p_{3}}}^{2}n^{4}+2\sigma _{p_{1}}\sigma _{p_{2}}\ell ^{2}m^{2}+2\sigma _{p_{1}}\sigma _{p_{3}}\ell ^{2}n^{2}+2\sigma _{p_{2}}\sigma {p_{3}}m^{2}n_{2}^{p}} [42] 然后我们可以使用主成分并将公式 34-36 代入公式 37 得到
S 2 = σ 11 2 ℓ 2 + σ 22 2 m 2 + σ 33 2 n 2 {\displaystyle S^{2}={\sigma _{11}}^{2}\ell ^{2}+{\sigma _{22}}^{2}m^{2}+{\sigma _{33}}^{2}n^{2}} [43] 经过大量的代数运算并将公式 41 & 42 代入公式 40 ，我们得到
τ M A X 2 = ( σ 11 − σ 22 ) 2 ℓ 2 m 2 + ( σ 11 − σ 33 ) 2 ℓ 2 n 2 + ( σ 22 − σ 33 ) 2 m 2 n 2 {\displaystyle \tau _{MAX}^{2}=(\sigma _{11}-\sigma _{22})^{2}\ell ^{2}m^{2}+(\sigma _{11}-\sigma _{33})^{2}\ell ^{2}n^{2}+(\sigma _{22}-\sigma _{33})^{2}m^{2}n^{2}} [44] 通过这个解决方案，我们现在有三个可能的平面。一个平面平分 σ 11 {\displaystyle \sigma _{11}} σ 22 {\displaystyle \sigma _{22}} σ 11 {\displaystyle \sigma _{11}} σ 33 {\displaystyle \sigma _{33}} σ 22 {\displaystyle \sigma _{22}} σ 33 {\displaystyle \sigma _{33}} θ = π 4 {\textstyle \theta ={\pi \over 4}} cos π 4 = 2 2 {\textstyle \cos {\pi \over 4}={{\sqrt {2}} \over 2}} ℓ , m , n {\displaystyle \ell ,m,n} τ {\displaystyle \tau }
ℓ {\displaystyle {\boldsymbol {\ell }}} m {\displaystyle {\boldsymbol {m}}} n {\displaystyle {\boldsymbol {n}}} τ {\displaystyle {\boldsymbol {\tau }}}
0 {\displaystyle 0} 2 2 {\displaystyle {\frac {\sqrt {2}}{2}}} 2 2 {\displaystyle {\frac {\sqrt {2}}{2}}} 1 2 ( σ 22 − σ 33 ) {\displaystyle {\frac {1}{2}}(\sigma _{22}-\sigma _{33})}
2 2 {\displaystyle {\frac {\sqrt {2}}{2}}} 0 {\displaystyle 0} 2 2 {\displaystyle {\frac {\sqrt {2}}{2}}} 1 2 ( σ 11 − σ 33 ) {\displaystyle {\frac {1}{2}}(\sigma _{11}-\sigma _{33})}
2 2 {\displaystyle {\frac {\sqrt {2}}{2}}} 2 2 {\displaystyle {\frac {\sqrt {2}}{2}}} 0 {\displaystyle 0} 1 2 ( σ 11 − σ 22 ) {\displaystyle {\frac {1}{2}}(\sigma _{11}-\sigma _{22})}
按照惯例， σ 11 > σ 22 > σ 33 {\displaystyle \sigma _{11}>\sigma _{22}>\sigma _{33}}
τ M A X = σ 11 − σ 33 2 {\displaystyle \tau _{MAX}={\sigma _{11}-\sigma _{33} \over 2}} 图 8 ：一个 3D 莫尔圆包含三个圆，每个轴一个圆，并遵循 σ 11 > σ 22 > σ 33 {\displaystyle \sigma _{11}>\sigma _{22}>\sigma _{33}} 请注意，我们知道存在两个最大剪切应力平面，它们彼此旋转了 π {\textstyle \pi } ± 2 2 {\textstyle \pm {{\sqrt {2}} \over 2}}
由于这些轴向旋转是解耦的，我们可以使用莫尔圆来表示 3D 应力状态，如图 8 所示。
![{\displaystyle \sigma _{12MAX}=\pm \left[\left({\sigma _{11}-\sigma _{22} \over 2}\right)^{2}+{\sigma _{12}}^{2}\right]^{1 \over 2}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/27ff9153bf6b0751b8685013c678110499064b10)
![{\displaystyle \left[\ell ,m,n\right]}](https://wikimedia.org/api/rest_v1/media/math/render/svg/5a9dcae54880c69cb3b75a49b7ab30db68b7d800)
