Shear and Moment Diagram Calculator
Bending moment diagrams, maximum moment and bending stress, solved step by step
The Load-Shear-Moment Relationships
Load, shear and bending moment are three levels of the same story, linked by calculus:
Symbols and units:
- — distributed load intensity, newtons per metre (N/m), kN/m in practice
- — internal shear force, N or kN
- — internal bending moment, newton-metres (N·m), kN·m in practice
- — distance along the beam, metres (m)
Integrating gives the two rules that make diagrams quick:
- the change in shear between two points equals minus the area under the load diagram
- the change in moment equals the area under the shear diagram
The immediate consequence: the bending moment is maximum where the shear crosses zero, because that is where . Standard results follow directly — for a central point load on a simply supported span, for a uniform load on the same span, and at the wall of a cantilever.
The assumption people forget: these relations hold for statically determinate beams with small deflections.
From Bending Moment to Stress and Deflection
The bending moment produces a stress that varies linearly through the depth:
- — bending stress, pascals (Pa), tension on one face and compression on the other
- — bending moment at that section, N·m
- — distance from the neutral axis to the extreme fibre, m
- — second moment of area, m⁴; for a rectangle , so depth dominates
The ratio is the section modulus in m³, reducing the check to .
Stiffness is a separate question, governed by in N·m²:
Deflection scales with or , which is why long spans fail serviceability checks long before they fail on stress.
The assumption people forget: assumes a linear-elastic, initially straight, symmetric beam in pure bending — it is not valid past yield.
Common Mistakes to Avoid
- Looking for at midspan by habit — it sits where the shear crosses zero, which is midspan only for symmetric loading.
- Losing the minus sign in — shear falls, not rises, under a downward load.
- Mixing kN·m and N·m in — kN·m is N·m.
- Using the full depth as — it is the half-depth for a symmetric section, so m for a mm beam.
- Writing — that is about the base, not the neutral axis; bending uses .
- Confusing the shear and moment diagrams — the moment is the area under the shear plot, not a rescaled copy of it.
- Forgetting the fixed-end moment on a cantilever — the wall carries both a reaction force and a moment.
Examples
Frequently Asked Questions
Find the reactions, plot the shear from left to right, then integrate it: the change in bending moment between any two points equals the area under the shear diagram between them. Both diagrams must close back to zero at a free or simply supported end.
Wherever the shear force crosses zero, since dM/dx = V. For a simply supported beam with a central point load that is midspan, giving PL/4; for a uniform load it is also midspan, giving wL²/8; for a cantilever it is at the fixed end.
Use σ = Mc/I: the bending moment in N·m times the distance from the neutral axis to the extreme fibre in metres, divided by the second moment of area in m⁴. For a rectangle I = bh³/12 and c = h/2.
The shear force is the derivative of the bending moment, V = dM/dx, and the load is minus the derivative of the shear, w = −dV/dx. So the moment diagram is the running area under the shear diagram, and it peaks where the shear is zero.
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