S diagramLeft to right, jump after jump
Scan from left to right. Every force moves the graph — and the type of load decides how.
- Point Sharp turn — a jump the size of the force
- Distributed Diagonal line
- Triangular Parabola
Force up → the graph rises · force down → it falls. At the end — it must close at 0.
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01
Why does it work? (30 seconds)
- S at a point = the sum of the vertical forces to the left of the point.
- Every force you pass → the sum changes by exactly its size → a jump.
- A distributed load adds a little in every centimetre → the graph falls gradually → a diagonal line.
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02
A beam of 8 m — 6 steps
Beam and S diagram — the same x axis · scroll the drawing sideways - x = 0AY up → jump to 6.5
- 0–2No load → straight line
- x = 26 t down → 6.5 − 6 = 0.5
- 2–4No load → straight line
- 4–82 t/m → diagonal line: 0.5 − 2·4 = −7.5
- x = 8BY up → −7.5 + 7.5 = 0 closed ✓
- ZS crosses 0 on the diagonal line → Z = S / Q = 0.5 / 2 = 0.25 m after x = 4 → x = 4.25
That's it. 6 steps, and the graph closes at 0 — a sign that the reactions are correct.
And if S crosses 0 in a jump? For example a point force that takes S down from +3.8 to −1.2. No diagonal line crosses — there is no Z. That is fine: the point of the force is the place of Mmax.
A concentrated moment? It does not change S at all — it only rotates.
- x = 0
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03
4 pitfalls everyone falls into
- Starting from the end instead of from the reaction. The graph starts at the point where the first force meets the beam.
- The resultant instead of the load. You get a jump of 8 at x = 6 instead of a diagonal line.
- Q from another segment in Z. Take the Q of the segment where S crosses 0.
- It did not close at 0 — and you carry on. That is a mistake in the reactions. Go back there before M.
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