Vlasov torsion theory: Difference between revisions
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# shear stresses due to restrained warping | # shear stresses due to restrained warping | ||
# normal stresses due to restrained warping | # normal stresses due to restrained warping | ||
These stresses are combined with stresses due to axial, bending and shear loading. For example the total axial stress can be obtained as follows (Hoogenboom 2006): | |||
<tex>\;\;\;\sigma_{xx}\;=\; | |||
\frac{N}{A}\;+\; | |||
\frac{M_y}{I_y}\;z\;-\; | |||
\frac{M_z}{I_z}\;y\;+\; | |||
\frac{B}{I_{\omega}}\;\omega</tex> | |||
== External Links == | == External Links == | ||
Revision as of 05:36, 22 September 2009
Assumptions
- Warping can be constrained
- Derivative of section rotation about the axis of the twist is not constant
Differential Equation
The rotation of the beam cross-section follows the following differential equation (Hoogenboom 2006):
<tex>EI_{\omega}\;\frac{d^4 \phi}{dx^4}\;-\; GI_t\;\frac{d^2 \phi}{dx^2}\;=\; m_x</tex>
Refer to torsion page for the notation used in the above equation.
Stresses
According to Vlasov to the theory, the applied torque causes the following three types of stresses:
- shear stresses due to unrestrained torsion
- shear stresses due to restrained warping
- normal stresses due to restrained warping
These stresses are combined with stresses due to axial, bending and shear loading. For example the total axial stress can be obtained as follows (Hoogenboom 2006):
<tex>\;\;\;\sigma_{xx}\;=\; \frac{N}{A}\;+\; \frac{M_y}{I_y}\;z\;-\; \frac{M_z}{I_z}\;y\;+\; \frac{B}{I_{\omega}}\;\omega</tex>
External Links
- P.C.J. Hoogenboom: Vlasov Torsion Theory, October 2006
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| Topics | Warping · Bimoment |