Method of Joints for Trusses

The method of joints finds the force in every member of a truss by treating each pin as a particle in equilibrium. Find the support reactions first, then start at a joint with no more than two unknown member forces, apply ΣFx = 0 and ΣFy = 0, and move joint by joint until every member is solved.

Last updated

What makes a structure a truss

A truss is a set of straight members joined at their ends by pins, with loads applied only at the joints. Under those assumptions every member is a two-force member: it is pulled or pushed only along its own axis, so its force is a single number, tension or compression.

A plane truss is statically determinate and stable when m = 2j − 3, where m is the number of members and j the number of joints, and the members are arranged in triangles. If m is larger, the truss is indeterminate and needs deformation compatibility from mechanics of materials.

The method, step by step

Treat the whole truss as one rigid body and find the reactions with the three equilibrium equations. Then cut out one joint at a time and draw its free body diagram: the external loads, the reactions if it is a support, and one force along each member that meets there.

Assume every unknown member force is tension, drawn pulling away from the joint. A positive answer then means tension, a negative answer compression, and you can carry the signed value straight into the next joint without redrawing arrows.

Zero-force members

Two rules spot members that carry no load under a given loading, which saves equations and catches errors. At an unloaded joint with only two non-collinear members, both are zero-force members. At an unloaded joint with three members, two of them collinear, the third is a zero-force member.

Zero-force members are not useless: they brace compression members against buckling and carry load when the loading changes.

Key formulas

Formulas used on this page, with the textbook each is cited from
FormulaExpressionWhereCited from
Joint equilibriumΣFx = 0, ΣFy = 0 (at every joint)F = forces on the pin (N or kN): external loads, reactions and member forcesHibbeler, Engineering Mechanics: Statics
Member force componentsFx = F·(Δx / L), Fy = F·(Δy / L)F = member force (kN), Δx and Δy = member run and rise (m), L = √(Δx² + Δy²) = member length (m)Beer & Johnston, Vector Mechanics for Engineers: Statics
Determinacy of a plane trussm = 2j − 3m = number of members, j = number of joints (both dimensionless counts); 3 = number of independent support reactionsMeriam & Kraige, Engineering Mechanics: Statics

Worked examples

Example: A three-member truss with a vertical and a horizontal load

Given

  • A triangular truss with joints A at (0, 0), C at (4 m, 0) and apex B at (2 m, 1.5 m). Members AB, BC and AC.
  • A is a pin support and C is a roller on a horizontal surface.
  • Joint B carries 12 kN downward and 4 kN horizontally to the right.

Find

  • The support reactions and the force in each member, stating tension (T) or compression (C).

Solution

  1. Geometry: AB and BC each have a run of 2 m and a rise of 1.5 m, so L = 2.5 m and the direction ratios are 0.8 (horizontal) and 0.6 (vertical).L = √(2² + 1.5²) = 2.5 m
  2. Moments about A for the whole truss give the roller reaction at C (counterclockwise positive):ΣM_A: Cy(4) − 12(2) − 4(1.5) = 0 → Cy = 7.5 kN ↑
  3. Force balance gives the pin reactions at A:ΣFy: Ay + 7.5 − 12 = 0 → Ay = 4.5 kN ↑; ΣFx: Ax + 4 = 0 → Ax = −4 kN (4 kN ←)
  4. Joint A, with F_AB and F_AC assumed in tension. ΣFy isolates F_AB:4.5 + 0.6·F_AB = 0 → F_AB = −7.5 kN
  5. ΣFx at A then gives F_AC:−4 + 0.8(−7.5) + F_AC = 0 → F_AC = 10 kN
  6. Joint C. ΣFy isolates F_BC (BC points up and to the left from C):7.5 + 0.6·F_BC = 0 → F_BC = −12.5 kN
  7. Check ΣFx at C, then both equations at B:C: −10 − 0.8(−12.5) = 0 ✓; B: 4 + 6 − 10 = 0 ✓, −12 + 4.5 + 7.5 = 0 ✓

Answer: Ax = 4 kN ←, Ay = 4.5 kN ↑, Cy = 7.5 kN ↑. F_AB = 7.5 kN (C), F_BC = 12.5 kN (C), F_AC = 10 kN (T). The horizontal load makes the two rafters carry different forces even though the truss is symmetric.

Example: A five-joint truss solved joint by joint

Given

  • Bottom chord joints A (0, 0), C (4 m, 0) and E (8 m, 0); top chord joints B (2 m, 3 m) and D (6 m, 3 m).
  • Members AB, AC, BC, BD, CD, CE and DE. A is a pin, E is a roller.
  • Loads: 10 kN downward at C and 6 kN downward at D.

Find

  • The force in every member, as tension (T) or compression (C).

Solution

  1. Check determinacy: 7 members and 5 joints.m = 2j − 3 = 2(5) − 3 = 7 ✓
  2. Each diagonal has a run of 2 m and a rise of 3 m, so L = √13 m and the direction ratios are 2/√13 = 0.555 and 3/√13 = 0.832.L = √(2² + 3²) = √13 = 3.606 m
  3. Reactions from moments about A and vertical balance:Ey(8) − 10(4) − 6(6) = 0 → Ey = 9.5 kN ↑; Ay = 16 − 9.5 = 6.5 kN ↑
  4. Joint A (two unknowns):6.5 + 0.832·F_AB = 0 → F_AB = −7.81 kN; 0.555(−7.81) + F_AC = 0 → F_AC = 4.33 kN
  5. Joint E, the same way:9.5 + 0.832·F_DE = 0 → F_DE = −11.42 kN; F_CE = −0.555(−11.42) = 6.33 kN
  6. Joint B (no load). ΣFy: the two diagonals must cancel; ΣFx then gives the top chord.F_BC = −F_AB = 7.81 kN; F_BD = −0.555(7.81) − 0.555(7.81) = −8.67 kN
  7. Joint D. ΣFy gives F_CD; ΣFx is the check.−0.832(F_CD + F_DE) − 6 = 0 → F_CD = −7.21 + 11.42 = 4.21 kN; 8.67 − 0.555(4.21) + 0.555(−11.42) = 0 ✓
  8. Joint C is a full check (vertical components of the diagonals against the 10 kN load):0.832(7.81) + 0.832(4.21) − 10 = 6.5 + 3.5 − 10 = 0 ✓

Answer: F_AB = 7.81 kN (C), F_AC = 4.33 kN (T), F_BC = 7.81 kN (T), F_BD = 8.67 kN (C), F_CD = 4.21 kN (T), F_CE = 6.33 kN (T), F_DE = 11.42 kN (C). The top chord is in compression and the bottom chord in tension, as in any simply supported truss with downward loads.

Common mistakes

In industry

Frequently asked questions

When should I use the method of sections instead?

When you need the force in only a few members in the middle of a large truss. A section cut gives three equations at once, so you can reach an interior member without solving every joint before it.

How do I know if a member is in tension or compression?

Assume tension, drawn pulling away from the joint. A positive result is tension and a negative result is compression.

Why can loads only be applied at the joints?

It keeps every member a two-force member with no bending. Real trusses have self-weight and some joint fixity, but these effects are usually small, and the self-weight is often split between the two end joints.

Can a truss have zero-force members and still be needed?

Yes. They brace other members against buckling, keep the shape stable, and carry load when the loading changes.

Does the method work for 3D trusses?

Yes, with three equations per joint (ΣFx, ΣFy, ΣFz). Start at a joint with no more than three unknowns.

Keep learning

All Statics lessons · All engineering subjects

See also

Sources

  1. R. C. Hibbeler, Engineering Mechanics: Statics, Pearson
  2. F. P. Beer, E. R. Johnston, D. F. Mazurek, Vector Mechanics for Engineers: Statics, McGraw Hill
  3. J. L. Meriam, L. G. Kraige, Engineering Mechanics: Statics, Wiley

COPLAIN AI PLATFORM

Generate yours automatically from your existing docs

Heading into manufacturing? Coplain turns engineering procedures into clear, audit-ready work instructions and job aids for the shop floor.

Generate yours automatically with Coplain →

Related Tools & Templates