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The BST binders · Trusses binder · Solution methods · updated 27.9.2026

Method of jointsA whole truss, joint after joint

Every joint = a small puzzle of two equations: ΣFx = 0 and ΣFy = 0.

The only rule: enter only a joint with at most 2 unknown members.

  • 1 Reactions — ΣM about the pinned support
  • 2 Zero-force members — mark them in advance
  • 3 Joint with ≤ 2 unknowns → ΣFx, ΣFy
  • 4 Move on to the neighbouring joint
  1. 01

    The trick that saves most mistakes

    • Every unknown member — assume tension: the arrow leaves the joint.
    • Got plus → tension. Got minus → compression. No guessing — the sign decides.
    • A member already found in compression enters the next joint with an inward arrow and a positive magnitude. Never an inward arrow and a minus together.
    • Every component points where the arrow points: right and up — plus, left and down — minus. A tension member to the left of the joint: the arrow leaves to the left → minus.
    • An inclined member is decomposed: horizontal = N · cos α, vertical = N · sin α. Here α = 45° → 0.707 for both.
  2. 02

    A whole truss — 6 joints: 5 to solve, F to check

    A truss of 6 m and height 2 m, 4 t at D and 1 t at F. The order: A → C → D → E → B.

    N1N2N3N4N5N6N7N8N9AY = 3 tBY = 2 t4 t1 tACEBDF
    N3 dashed — zero-force member (joint C) · scroll the drawing sideways
    • Reactions
      ΣMA: 4·2 + 1·4 − BY·6 = 0 → BY = 2 t, and from ΣFy: AY = 3 t
    AY = 3N1N2A
    Joint A — two members, two unknowns
    4.2434 tN4N5D
    Joint D — N1 in compression enters the joint
    • Joint A
      ΣFy: 3 + N1·0.707 = 0 → N1 = −4.243 compression
      ΣFx: N2 + N1·0.707 = 0 → N2 = 3
    • Joint C
      N2 and N6 on one line, no load → N3 = 0 · ΣFx: −3 + N6 = 0 → N6 = 3
    • Joint D
      N1 in compression enters D: 4.243 · 0.707 = 3 to the right and 3 up → ΣFy: 3 − 4 − N5·0.707 = 0 → N5 = −1.414
      ΣFx: 3 + N4 + N5·0.707 = 0 → N4 = −2
    • Joint E
      N5 in compression enters E: 1 to the right, 1 down → ΣFy: N7 − 1 = 0 → N7 = 1 · ΣFx: −3 + 1 + N9 = 0 → N9 = 2
    • Joint B
      ΣFy: 2 + N8·0.707 = 0 → N8 = −2.828 compression, and ΣFx comes to zero check ✓

    That's it. 9 members, 5 joints — and at every joint only two short equations.

    All the results (for checking)
    Reactions: AY = 3 t, BY = 2 t
    MemberBetween jointsForceState
    N1A–D4.243 tCompression
    N2A–C3 tTension
    N3C–D0Zero-force member
    N4D–F2 tCompression
    N5D–E1.414 tCompression
    N6C–E3 tTension
    N7E–F1 tTension
    N8F–B2.828 tCompression
    N9E–B2 tTension
  3. 03

    4 pitfalls everyone falls into

    • Entering a joint with 3 unknowns. At D there are four at first — so we start at A.
    • Lever arms from different supports in the same ΣM. All lever arms — from the same point.
    • Inward arrow + minus. The sign is counted twice → at D you get N5 = −9.9 instead of −1.414.
    • Swapping sin and cos. At 45° it doesn't show — at another angle it ruins everything.

    Bonus: Finished? Substitute into the last joint — everything must come to zero. A free check.

Trusses binder · BST · beamsolvertool.com/en/learn/trusses/method-of-joints/

Solve a truss in BST BST guides you joint after joint, with a free body for every joint — or waits for you to solve on your own

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