Concentrated momentS does not jump, M jumps
A concentrated moment M₀ = rotation at one point. It has no force — and therefore:
- Reactions Enters ΣM at its full value — no lever arm
- S Does not jump because of it — it is not a force
- M Jumps by M₀ at the point where it acts
Same sign in both places: clockwise = +M₀ — both in ΣM and in the jump in M. Counter-clockwise = −M₀.
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01
Why? (30 seconds)
- M₀ does not push the beam up or down — it only rotates it → it has no place in ΣFy or in the S diagram.
- It is already 'force × lever arm' → it enters ΣM as it is, about any point you choose.
- Whoever passes the point in the M diagram 'feels' the whole rotation at once → a jump.
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02
A 6 m beam — with only a moment on it
Beam, S and M — the same x axis. Positive M is drawn below the axis, as in BST · scroll the drawing sideways - ΣMA6 − BY·6 = 0 → BY = 1 t upward
- ΣMBAY·6 + 6 = 0 → AY = −1 t — the minus: AY acts downward
- Check−1 + 1 = 0 ✓
- SAY downward → −1, a straight line to the end — M₀ does not move S → BY closes to 0
- 0–2Rectangle −1 · 2 = −2 → M = −2
- x = 2M₀ clockwise → −2 + 6 = +4 jump
- 2–6Rectangle −1 · 4 = −4 → 4 − 4 = 0 closes ✓
That's it. A reaction that pulls down, a completely flat S — and one jump in M.
And where is Mmax? There is no Z — S does not cross 0. The extreme values sit on both sides of the jump: −2 on the left, +4 on the right. The largest in magnitude: 4 t·m.
- ΣMA
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03
4 pitfalls
- M₀ times a distance in ΣM. It is already a moment — it goes in as it is.
- A jump in S. M₀ does not change S at all.
- 'Fixing' the minus of AY. The minus tells the direction — flip the arrow and keep the magnitude.
- A jump in the opposite direction. Clockwise = +M₀.
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 handles concentrated moments — in the reactions and in the jump in M
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