The Chartership Forum

Reinforced Concrete Design / Flexural behaviour and section analysis

Deriving the moment of resistance

Three principles, no formula quoted — and a clear account of which step the code decides.

Lesson review: expert verification remains open

This lesson has received a full-context editorial review and a check of its technical explanations. Selected arithmetic has been checked separately. This is not independent engineering sign-off.

Checks needed for project use

  • A concrete-design reviewer must check the stated first-generation clauses, National Annex choices, detailing rules and factor sets. Numerical agreement alone does not establish code compliance.
  • A suitably qualified engineer must verify the adopted material model, standards clauses and design applicability independently.

These are educational models and exercises. Check their assumptions before using the results. The full technical content and every diagram have not yet been independently verified.

Concrete and steel calculations retain their stated first-generation Eurocode teaching basis. Use the standards and amendments specified for your project; do not mix generations without an appropriate design basis.

Read the lesson register and outstanding review notes

Why this matters

Almost every textbook presents the flexural design equation as something to be substituted into. It is not: it follows from three statements, two of which are pure mechanics. Deriving it once means you can rebuild it for a section shape nobody tabulated, and — more usefully — you can see exactly which step a National Annex could change.

By the end of this lesson you should be able to

  • State the three principles the derivation rests on
  • Derive MRd for a singly reinforced rectangular section
  • Identify which steps are mechanics and which are code choices
  • Explain what the rectangular stress block replaces, and why

What you should already know

  • How a section behaves, from zero load to failure (this module)
  • Strain compatibility (Module 1)
  • Equilibrium of forces and moments (Structural Analysis Fundamentals, Module 2)

From first principles

Moment of resistance of a singly reinforced section

We want to show: that MRd = As fyd (d − s/2), with the stress-block depth s fixed by equilibrium.

Moment of resistance of a singly reinforced sectionsectionx = 157strain0.003500.00742 (yielded)stressCTEquivalent stress block s = 126 mm

Forget formulae for a moment and picture the section at failure. The top is being crushed; the bottom is cracked open with the bars holding it together. So there is a push in the concrete near the top and a pull in the steel near the bottom. Nothing is pushing the beam along its length, so those two must be equal and opposite. They are equal and opposite forces on parallel lines — a couple — and the moment the section resists is simply the size of that force times the distance between them. That is the whole answer: find the force, find the distance, multiply. Everything else is working out how big the force is and where it acts.

Practice

For C30/37 concrete with αcc = 0.85 and γC = 1.5, what is the design compressive strength fcd, in N/mm²?

Practice

For reinforcement with fyk = 500 N/mm² and γS = 1.15, what is the yield strain, taking Es = 200 000 N/mm²?

Practice

A section has As = 1473 mm², fyd = 434.8 N/mm², b = 300 mm, d = 490 mm and η fcd = 17.0 N/mm². Using the derived expression, what is MRd, in kNm?

Summary

  • Three principles: material models, strain compatibility, equilibrium
  • Strain compatibility and equilibrium are mechanics; the stress block is a chosen model
  • γC, γS, αcc and the x/d limit are nationally determined
  • x is solved from C = T, never assumed
  • MRd = T z = As fyd (d − s/2)
  • Always check that the steel really has yielded — the derivation assumed it