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Mohr's Circle 2D Stress Transformation Calculator

Transform 2D biaxial stress states to determine principal stresses, maximum shear planes, and equivalent Von Mises stress with a dynamic graphical Mohr's circle.

2D State of Stress (In-Plane)

Principal Stresses (σ₁, σ₂)
89.5 / -49.5 MPa
Max Shear Stress (τ_max)
69.5 MPa
Von Mises Stress (σ_vM)
122.0 MPa

Interactive Mohr's Circle Graphical Transformation

Radius R = 69.46 MPa

Transformation Formulas

1. Center & Radius of Mohr's Circle

Center coordinate (σ_avg, 0) and radius in 2D stress state.

2. Principal Normal Stresses (σ₁, σ₂)

Maximum and minimum normal stresses acting on planes of zero shear stress.

3. Maximum In-Plane Shear & Principal Orientation

Plane orientation to align with principal stress axes.

4. Von Mises Equivalent Stress

Ductile failure criterion for multiaxial stress states.

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Governing Equation

Analytical equations compliant with standard university curricula and professional engineering practice codes.

Engineering Reference & Technical Guide

Mohr's Circle 2D Stress Transformation Engineering Reference Guide

Peer-reviewed mathematical formulation, verified step-by-step worked engineering calculations, design codes, and practical guidelines.

Governing Theory & Derivation

Analytical physics and classical mechanics foundations

Mohr's Circle, developed by German civil engineer Christian Otto Mohr in 1882, is a graphical and analytical method for transforming plane stress tensors. Given normal stresses (σ_x, σ_y) and shear stress (τ_xy) on an orthogonal element, it determines the maximum normal (principal) stresses, maximum in-plane shear stress, and principal plane orientations.

1. Coordinate Transformation Equations

Equilibrium of an inclined wedged element rotated by an angle θ yields the normal and shear stress on the rotated plane:

2. Circle Radius and Center

Squaring and adding these equations yields the equation of a circle (σ - σ_avg)² + τ² = R² centered on the normal stress axis:

3. Principal Stresses and Maximum Shear

The principal stresses occur where shear stress is identically zero. Maximum in-plane shear stress equals the circle radius R:

Engineering Interpretation:Brittle materials (like cast iron and concrete) fail primarily under maximum tensile principal stress (Rankine criterion). Ductile materials (like structural steel and aluminum) fail by shear slip governed by Tresca (τ_max) or Von Mises equivalent stress.

Step-by-Step Worked Example

Biaxial Stress Transformation in a Pressurized Thin-Walled Vessel

Problem Statement

A strain gauge rosette on a pressure vessel skin reveals a plane stress state of σ_x = 80 MPa (longitudinal tension), σ_y = -40 MPa (transverse compression), and τ_xy = 35 MPa. Determine the principal stresses, maximum shear stress, principal angle, and Von Mises equivalent stress.

Given Parameters

Normal Stress X (σ_x)80 MPa
Normal Stress Y (σ_y)-40 MPa
Shear Stress (τ_xy)35 MPa

Detailed Calculation Steps

1Calculate Average Stress and Circle Radius

The circle center is at (20 MPa, 0) with a radius of 69.46 MPa.

2Determine Principal Normal Stresses

σ_1 represents the peak tensile stress on the material, and σ_2 represents peak compressive stress.

3Calculate Orientation of Principal Planes

Rotating the element 15.13° counter-clockwise aligns the element with the principal normal axes where shear stress vanishes.

4Compute Von Mises Equivalent Stress

Von Mises stress compares multi-axial stresses directly against a uniaxial tensile yield strength test.

Conclusion & Design Verification:For an AISI 1020 steel casing with yield strength S_y = 250 MPa, the factor of safety against yielding is 250 / 122.01 = 2.05.

Applicable Standards & Design Codes

Recognized engineering guidelines and criteria

ASME Boiler and Pressure Vessel Code (BPVC Section VIII)ASME

Rules for Construction of Pressure Vessels

Uses stress intensity (Tresca criterion) and distortion energy (Von Mises) for allowable stress limits.

ASTM E8 / E8MASTM International

Standard Test Methods for Tension Testing of Metallic Materials

Standard benchmark for uniaxial tensile yields used in equivalent stress comparisons.

Assumptions & Practical Limitations

Critical constraints for professional applications

  • Strictly 2D plane stress formulation (σ_z = τ_xz = τ_yz = 0). For 3D stress states, the out-of-plane principal stress (σ_3 = 0) must be checked for absolute maximum shear.
  • Applies only to linear, elastic, homogeneous, and isotropic materials.
  • Does not predict crack propagation or fracture mechanics in brittle materials with sharp stress raisers.

Frequently Asked Questions

Common technical engineering inquiries

Q:Why is Mohr's circle represented as 2θ instead of θ?

In coordinate transformations, the trigonometrical identity for transformed shear and normal stress involves double angles (cos 2θ and sin 2θ). Therefore, an actual physical rotation of angle θ on the material corresponds to a 2θ rotation around the center on Mohr's circle.

Q:How does Von Mises stress relate to Mohr's circle?

Mohr's circle identifies the principal stresses (σ_1 and σ_2). Von Mises stress takes these principal stresses and calculates the octahedral shear stress (distortion energy) representing the yield threshold for ductile materials.