Uniformly distributed loadOne force in the middle — for reactions only
A distributed load = a row of small forces. For the reactions, replace them with one force.
- Resultant P = Q · L — L of the segment, not of the beam
- Position exactly in the middle of the segment
- For reactions only in S and M you work with the load itself
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01
Why is it allowed — and why for reactions only? (30 seconds)
- The resultant gives the supports the same moment as all the small forces together → the reactions come out exact.
- But inside the beam the load is spread out and does not land at one point → in S it is a sloped line, not a jump.
- Where does S cross 0? Z = S / Q — how many metres the load needs to "eat" S.
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02
A 6 m beam — from the load to Mmax
Beam, S diagram and M diagram — the same x axis. Positive M is drawn below the axis, as in BST · scroll the drawing sideways - Resultant2 · 6 = 12 t in the middle → x = 3
- ReactionsΣMA: 12·3 − BY·6 = 0 → BY = 6 t, and the beam is symmetric → also AY = 6 t
- SStarts at 6, goes down along a sloped line → 6 − 2·6 = −6 → BY closes it to 0 ✓
- ZZ = 6 / 2 = 3 m
- MmaxArea of the triangle up to Z: 3 · 6 / 2 → Mmax = 9 t·m, at Z
That's it. A resultant for the reactions, a sloped line in S, one triangle for Mmax.
One-second check: a simple beam with a uniform load along the whole length: Mmax = Q·L² / 8 = 2·36 / 8 = 9 ✓
- Resultant
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03
4 pitfalls everyone falls into
- The resultant goes into S. You get a jump of 12 in the middle instead of a sloped line — and all of M is wrong.
- L of the whole beam. When the load is only on part of it — L is the length of the segment.
- The resultant in the middle of the beam. It is in the middle of the load's segment.
- Q from another segment in Z. Take the Q of the segment where S crosses 0.
The full page — for BST PRO subscribers
The solved example, the pitfalls and the printable PDF — in the BST PRO binders.
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Solve a beam in BST BST draws S and M, finds Z and calculates Mmax — step by step
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