Donnell | $ {\varepsilon _{x_ {\rm{D}}}} $ | $ {\varepsilon _{\theta_ {\rm{D}}}} $ | $ {\gamma _{x\theta_ {\rm{D}}}} $ |
Reissner | $ {\varepsilon _{x_ {\rm{D}}}} $ | ${\varepsilon _{\theta_ {\rm{D}}} }+z\dfrac{1}{ { {r^2} } }\dfrac{ {\partial v} }{ {\partial \theta } }$ | ${\gamma _{x\theta_ {\rm{D}}} }+z\dfrac{1}{r}\dfrac{ {\partial v} }{ {\partial x} }$ |
Sanders | $ {\varepsilon _{x_ {\rm{D}}}} $ | ${\varepsilon _{\theta_ {\rm{D}}} }+z\dfrac{1}{ { {r^2} } }\dfrac{ {\partial v} }{ {\partial \theta } }$ | ${\gamma _{x\theta_ {\rm{D}}} }+z\left(\dfrac{3}{ {2r} }\dfrac{ {\partial v} }{ {\partial x} } - \dfrac{1}{ {2{r^2} } }\dfrac{ {\partial u} }{ {\partial \theta } }\right)$ |
Love | $ {\varepsilon _{x_ {\rm{D}}}} $ | ${\varepsilon _{\theta_ {\rm{D}}} }+z\dfrac{1}{ { {r^2} } }\dfrac{ {\partial v} }{ {\partial \theta } }$ | ${\gamma _{x\theta_ {\rm{D}}} }+z\dfrac{2}{r}\dfrac{ {\partial v} }{ {\partial x} }$ |