Mohr's Circle Calculator

Enter the normal stresses σx, σy and shear stress τxy for a 2D stress element to find the principal stresses, the maximum in-plane shear stress, and the orientation of the principal planes.

Quick Facts

Circle center
C = (σx + σy) / 2
Sits on the τ = 0 axis; the circle is symmetric about it.
Circle radius
R = √[((σx − σy)/2)² + τxy²]
Equals the maximum in-plane shear stress.
Principal stresses
σ1,2 = C ± R
Occur on planes where shear stress is zero.
Principal angle
θp = ½·atan2(2τxy, σx − σy)
Physical rotation from the x-axis to the σ1 plane.

Your Results

Calculated
Maximum Principal Stress (σ1)
-
σ1 = C + R
Minimum Principal Stress (σ2)
-
σ2 = C − R
Max In-Plane Shear Stress (τmax)
-
τmax = R = (σ1 − σ2) / 2
Principal Plane Angle (θp)
-
Measured from the x-axis to the σ1 plane

Ready

Enter σx, σy, and τxy, then press Calculate.

How Mohr's Circle Works for 2D Stress

Mohr's Circle is a graphical technique developed by Christian Otto Mohr for visualizing the 2D stress transformation equations. Given the normal stresses σx and σy acting on the faces of a small stress element, and the shear stress τxy acting on those same faces, every possible normal-shear stress pair (σ, τ) on a plane cut through that point traces out a circle in σ-τ space. This calculator plots that circle numerically and reads off its most useful landmarks: the principal stresses, the maximum in-plane shear stress, and the angle at which the principal planes occur.

Deriving the principal stresses and angle

The circle's center sits on the shear-free (τ = 0) axis at C = (σx + σy) / 2 — this is the average normal stress, which is invariant under rotation. Its radius is R = √[((σx − σy)/2)² + τxy²], derived directly from the stress transformation equations by treating σx, σy, and τxy as the legs of a right triangle in stress space. The circle crosses the τ = 0 axis at two points, the principal stresses: σ1 = C + R (the algebraically larger principal stress) and σ2 = C − R (the smaller one). The maximum in-plane shear stress τmax equals the radius R itself and occurs 90° around the circle from either principal stress — which corresponds to a physical rotation of only 45° from the principal planes, because Mohr's Circle doubles all angles. The angle from the x-axis to the σ1 plane is θp = ½ · atan2(2τxy, σx − σy).

Common mistakes

  • Forgetting the angle-doubling rule: a 90° arc on Mohr's Circle corresponds to only 45° of physical rotation of the stress element — always divide the circle angle by 2.
  • Mixing up σ1 and σ2 with σx and σy: the principal stresses are almost never equal to the input normal stresses unless τxy = 0, in which case the x-y axes already are the principal axes.
  • Sign convention slips: tensile (positive) and compressive (negative) normal stresses must be entered with consistent signs, and shear stress sign follows the convention used to derive the transformation equations (clockwise shear on the positive x-face is typically taken as positive).

Real-world applications

  • Mechanical and structural engineers use Mohr's Circle to check whether a shaft, beam, or pressure vessel wall reaches a critical combined stress state under combined bending, axial, and torsional loads.
  • Geotechnical engineers use the same construction (with normal and shear stress on a soil or rock plane) to evaluate failure against the Mohr-Coulomb failure criterion.
  • Machine design and fatigue analysis use the maximum shear stress and principal stresses from Mohr's Circle as inputs to failure theories such as maximum shear stress (Tresca) or distortion energy (von Mises).

Frequently Asked Questions

What is Mohr's Circle used for?
Mohr's Circle is a graphical method for 2D stress (or strain) transformation. Given the normal stresses σx, σy and shear stress τxy on an element, it lets you find the principal stresses, the maximum in-plane shear stress, and the normal/shear stress on a plane rotated to any angle — without re-deriving the transformation equations each time.
How do you find the principal stresses from Mohr's Circle?
Plot the circle's center at C = (σx + σy)/2 and compute its radius R = √[((σx − σy)/2)² + τxy²]. The principal stresses are where the circle crosses the shear-free (τ = 0) axis: σ1 = C + R (maximum) and σ2 = C − R (minimum).
What is the maximum in-plane shear stress?
The maximum in-plane shear stress equals the circle's radius, τmax = R = (σ1 − σ2)/2. It acts on planes oriented 45° from the principal planes, and is always accompanied by a normal stress equal to the circle's center, σavg = (σx + σy)/2.
Why is the angle on Mohr's Circle double the physical angle?
Mohr's Circle is constructed so that a 360° rotation around the circle corresponds to only a 180° physical rotation of the stress element. So the angle θp = 0.5·atan2(2τxy, σx − σy) computed from the circle must be halved to get the real-world angle from the x-axis to the principal plane.