Mechanics of Materials · Chapter 8 of 10 · Advanced
Combined Loadings
Real parts rarely see one load at a time. Superposition lets you add the stresses from axial force, bending, torsion, and pressure, then transform them to find the worst case at a point.
Readiness check
This chapter combines the single-load formulas of earlier chapters. Tick only what you can do closed-notes.
- Compute axial stress P/A and bending stress Mc/I.
- Compute torsion stress Tr/J.
- Transform a stress state (principal stresses).
- Track tension and compression signs.
- Recall thin-wall geometry (r, t).
The core idea
When several loads act together, add the stress each would cause on its own, then transform the combined state to find the principal stresses at the critical point.
σ = P/A ± Mc/Ihoop σ = pr/t, long σ = pr/2tthen σ1,2 = σavg ± RBecause stresses are linear in load (within the elastic range), superposition holds: compute the axial, bending, torsional, and pressure stresses separately and sum the like components at a point. Then, since these may be normal and shear together, transform to principal stresses and maximum shear (Chapter 7). The art is choosing the critical point, usually where the contributions add rather than cancel.
The skills, taught in order
Combined loading is superposition plus transformation. Five skills cover the principle, pressure vessels, eccentric loading, shafts, and the general procedure.
8.1 The superposition principle
In the linear-elastic range, the stress from several loads equals the sum of the stresses from each load alone. Add only like components: normal stresses to normal, shear to shear. This reduces any combined problem to the single-load formulas already learned.
8.2 Thin-walled pressure vessels
A thin cylinder under internal pressure has a hoop (circumferential) stress σ = pr/t and a longitudinal stress σ = pr/2t, so the hoop stress is twice the longitudinal, which is why pipes split along their length. A sphere has σ = pr/2t in every direction.
| Vessel | Hoop / circumferential | Longitudinal / axial |
|---|---|---|
| Cylinder | pr/t | pr/2t |
| Sphere | pr/2t | pr/2t |
8.3 Eccentric loading (axial plus bending)
A load applied off the centroid is equivalent to a central load plus a moment M = Pe. The stress superposes: σ = P/A ± Mc/I. The eccentricity can push one face into tension even when the load is compressive, the reason masonry and short columns are kept within the middle third.
8.4 Combined bending and torsion
A shaft carrying a transverse load and a torque has, at its surface, a bending normal stress and a torsional shear stress at the same point. These form a plane-stress state that must be transformed (Chapter 7) into principal stresses and maximum shear for a failure check.
8.5 The general procedure
Identify the critical point (where contributions add), compute each load's stress there, superpose like components into σx, σy, τxy, then transform to σ1, σ2, and τmax. Compare the governing value with the material's strength.
Engineering connection: pressure vessels, crane hooks and C-frames (eccentric), and power shafts (bending plus torsion) are all combined-loading problems; this chapter unifies the whole course.
Worked example 1: a cylindrical pressure vessel
A cylindrical pressure vessel 1.5 m in diameter has a 12 mm wall and holds an internal gauge pressure of 2.5 MPa. Find the hoop and longitudinal stresses.
- ProblemFind the hoop and longitudinal stresses in the vessel in Figure 1.
- Given / findd = 1.5 m so r = 750 mm, t = 12 mm, p = 2.5 MPa. Find σh and σl.
- AssumptionsThin wall (t ≪ r), uniform stress through the thickness, closed ends.
- ModelApply the thin-walled cylinder formulas for hoop and longitudinal stress.
- Equationsσh = pr/t σl = pr/2t
- Solveσh = 2.5 × 750/12 = 156 MPa. σl = 2.5 × 750/(2 × 12) = 78 MPa.
- CheckThe hoop stress is exactly twice the longitudinal, as the formulas demand. The thin-wall ratio t/r = 12/750 = 0.016 ≪ 0.1, so the thin-wall assumption is valid.
- ConclusionThe hoop stress governs, which is why welded seams run lengthwise and why pipes burst with a longitudinal crack. The wall element is in biaxial tension, ready for a transformation check if needed.
Worked example 2: an eccentric load
A short rectangular post (100 mm × 150 mm) carries a 120 kN compressive load applied 40 mm off-center along the 150 mm direction. Find the stress on each face.
- ProblemFind the stress on each face of the post in Figure 2.
- Given / findP = 120 kN (compression), e = 40 mm, section 100 × 150 mm (c = 75). Find σ on both faces.
- AssumptionsShort post (no buckling), linear-elastic, eccentricity about one axis.
- ModelReplace the eccentric load by a central load plus M = Pe, then superpose axial and bending stresses.
- EquationsM = Pe σ = −P/A ± Mc/I I = bh³/12
- SolveA = 15 000 mm², so P/A = 8.0 MPa (compression). I = 100(150)³/12 = 2.81×10⁷ mm⁴; M = 120 000 × 40 = 4.8×10⁶ N·mm; Mc/I = ±12.8 MPa. Combined: −8.0 − 12.8 = −20.8 MPa on the near face, −8.0 + 12.8 = +4.8 MPa (tension) on the far face.
- CheckThe bending term (12.8) exceeds the axial (8.0), so one face flips into tension, the warning sign that the load is outside the middle third (e = 40 > h/6 = 25). A wider section or smaller eccentricity would keep it all in compression.
- ConclusionEccentric loading superposes axial and bending stress and can create unexpected tension, critical for concrete, masonry, and bolted joints that cannot take tension.
Misconceptions and diagnostics
| Mistake | Symptom | Diagnostic question | Correction |
|---|---|---|---|
| Adding normal and shear directly | Wrong combined stress | "Are these like components?" | Superpose normal with normal, shear with shear, then transform. |
| Hoop equals longitudinal | Pressure vessel under-designed | "Which stress is twice the other?" | For a cylinder, hoop = pr/t = twice the longitudinal pr/2t. |
| Ignoring the moment from eccentricity | Tension face missed | "Is the load on the centroid?" | An off-center load adds M = Pe; superpose its bending. |
| Wrong critical point | Stress checked where loads cancel | "Where do the contributions add?" | Pick the point where axial, bending, and torsion reinforce. |
Practice ladder
A spherical tank of 2 m diameter, 10 mm wall, holds 1.8 MPa. Find the wall stress.
Show answer
σ = pr/2t = 1.8 × 1000/(2 × 10) = 90 MPa, equal in all directions. Spheres are the most efficient pressure vessel for this reason.
For the Worked Example 2 post, what eccentricity keeps the whole section in compression?
Show answer
Tension is avoided while Mc/I ≤ P/A, i.e. e ≤ h/6 = 150/6 = 25 mm (the middle-third rule). At e = 25 mm the far face just reaches zero stress; beyond it, tension appears.
A 50 mm diameter shaft carries a bending moment giving 70 MPa and a torque giving 35 MPa shear at the surface. Find the maximum principal stress and τmax.
Show answer
σavg = 35, R = √(35² + 35²) = 49.5. σ1 = 35 + 49.5 = 84.5 MPa, σ2 = −14.5 MPa, τmax = 49.5 MPa. Superpose then transform, the standard shaft check.
Find a real combined-loading part (a pressurised pipe with wind load, a crane hook, a bike crank). Identify the loads, superpose the stresses at the critical point, and transform if needed.
What good work looks like
Each load's stress computed, like components summed at the critical point, and a transformation to principal stress or τmax where normal and shear coexist.
Working with AI, and proving it yourself
Use AI as an examiner, not a solver
Portfolio task
Analyse one combined-loading part: superpose the axial, bending, torsion, or pressure stresses at the critical point, then transform to the governing stress.
Retrieval and spaced review
Closed notes. Answer out loud, then reveal.
1. State the superposition principle for stress.
In the elastic range, total stress is the sum of the stresses from each load acting alone (like components added).
2. Give the hoop and longitudinal stresses for a cylinder.
σh = pr/t and σl = pr/2t; the hoop is twice.
3. How is an eccentric load handled?
As a central load plus M = Pe; σ = P/A ± Mc/I.
4. What is the middle-third rule?
Keep eccentricity within h/6 so no tension develops on the section.
5. What is the general combined-loading procedure?
Find each stress at the critical point, superpose like components, then transform to principal stresses and τmax.
Textbook mapping
| Item | Mapping |
|---|---|
| Primary source | Beer, Johnston, DeWolf and Mazurek, Mechanics of Materials (6th ed), Chapter 8 (Principal Stresses under a Given Loading) and thin-walled vessels |
| Cross-reference | Hibbeler, Ch. 8 · Gere and Goodno, Ch. 8 |
| Core topics | 8.1 Superposition · 8.2 Pressure vessels · 8.3 Eccentric loading · 8.4 Bending plus torsion · 8.5 General procedure |
| Engineering connection | Pressure vessels, eccentric columns and C-frames, and power shafts. |
| Read next | Chapter 9: Deflection of Beams. |