What Mohr's circle shows
The stresses on a small element depend on which way the element is turned. Mohr's circle draws every possible orientation at once: each point on the circle is one face, with its normal stress across and its shear stress down. The two points where the circle crosses the σ axis have no shear; those are the principal stresses. The bottom and top of the circle are the largest shear, R.
Drawing it by hand
- Plot X at (σx, τxy) and Y at (σy, −τxy), with τ positive downward.
- Join them. The line crosses the σ axis at the center, C = (σx + σy) / 2.
- Draw the circle through X and Y. Its radius is R.
- Read σ1 = C + R and σ2 = C − R where the circle meets the σ axis.
- The angle on the circle from X to σ1 is 2θp. Turn the element half that much, the same way, to reach the principal faces.
Worked example
Take σx = −20 MPa, σy = 90 MPa and τxy = 60 MPa, the values the calculator starts with. C = (−20 + 90) / 2 = 35 MPa and R = √(55² + 60²) = 81.4 MPa, so σ1 = 116.4 MPa and σ2 = −46.4 MPa. 2θp = atan2(120, −110) = 132.5°, so σ1 acts on the face turned θp = 66.3° counterclockwise from x. The largest in-plane shear is 81.4 MPa, on faces turned 21.3°.
Questions
Which way is positive shear on the circle?
Books differ. This calculator plots τ positive downward, the convention in Hibbeler's Mechanics of Materials, so the circle turns the same way as the element. If your class plots τ upward, the circle is mirrored top to bottom; the principal stresses and the angles on the element are the same.
Is this the same as the transformation equations?
Yes. The circle is a picture of the σx′, σy′ and τx′y′ equations above. The calculator uses the equations for its numbers and the circle to show them.
What about three-dimensional stress?
This calculator is for plane stress, where σz, τxz and τyz are zero, which covers thin plates, beam webs and the surface of most members. It still accounts for the out-of-plane shear in the largest shear in any direction.