- Practice · 8 marks
Derivation of plane stress transformation equations
Short answer
Wedge equilibrium yields σθ=(σx+σy)/2+((σx-σy)/2)cos2θ+τxy sin2θ and τθ=-((σx-σy)/2)sin2θ+τxy cos2θ. Principal stresses σ1,2=(σx+σy)/2±√[((σx-σy)/2)²+τxy²] occur where τθ=0; tan2θp=2τxy/(σx-σy). Maximum shear stress equals the radius of Mohr’s circle, on planes at 45° to principal planes.
For a body in a state of plane stress with stresses sigma_x, sigma_y and tau_xy, derive expressions for the normal and shear stresses on an inclined plane at angle theta. Hence obtain the principal stresses, the position of the principal planes and the maximum shear stress.
Sign convention
Tensile normal stress positive. Shear stress is positive when it acts in the direction on the face whose outward normal is . Angle is measured anticlockwise from the axis to the normal of the inclined plane.
sy (top face)
^ ^
+-----------+
| | txy on the +x face points up (+y)
<-| |-> sx
| |
+-----------+
sy (bottom face)
Equilibrium of a wedge
Take a triangular wedge with the inclined face of area , normal at . The areas of the vertical face and horizontal face are and .
Forces along the normal ():
Forces along the plane ():
Using double-angle identities:
Principal stresses
Principal planes have :
This gives two values of that differ by , so the two principal planes are apart. Substituting back:
(Equivalently .)
Maximum shear stress
Setting :
so (planes of maximum shear are at to the principal planes).
On these planes the normal stress is .
✓ Answer checked by Claude Opus 5.5 (high effort)
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