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How do engineers find the internal force in each member of a loaded truss?

Analyse a statically determinate pin-jointed truss using the method of joints to find the magnitude and nature (tension or compression) of the force in each member

A QCE Engineering Unit 3 answer on analysing pin-jointed trusses. Covers two-force members, the assumption of pin joints, the method of joints, and how to classify each member force as tension or compression with worked arithmetic.

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What this dot point is asking

QCAA wants you to take a pin-jointed truss carrying known loads and find the internal force in every member, stating whether each is in tension or compression. The standard tool is the method of joints: isolate each pin, treat it as a particle in equilibrium, and solve. This is the structural analysis step that turns a bridge or roof frame into a set of member forces you can later check against material limits.

The answer

What makes a truss special

A truss is an assembly of straight members connected at their ends by frictionless pins, with all external loads applied at the joints. These assumptions matter because they make every member a two-force member: a body with forces at only two points must carry a force directed along the line joining them. So each member is in pure tension (pulling its end joints together) or pure compression (pushing them apart), with no bending. That is what makes hand analysis possible.

A truss is statically determinate when the equilibrium equations alone are enough to find all member forces. The check is:

m+r=2jm + r = 2j

where mm is the number of members, rr the number of reaction components, and jj the number of joints. If this holds and the truss is stable, the method of joints will solve it.

The method of joints

The method treats each pin as a particle in equilibrium. A particle has no moment equation, so each joint gives exactly two equations:

βˆ‘Fx=0βˆ‘Fy=0\sum F_x = 0 \qquad \sum F_y = 0

The procedure:

  1. Find the support reactions from whole-structure equilibrium (βˆ‘Fx=0\sum F_x = 0, βˆ‘Fy=0\sum F_y = 0, βˆ‘M=0\sum M = 0).
  2. Pick a joint with no more than two unknown member forces.
  3. Draw the joint's free-body diagram. Assume each unknown member pulls away from the joint (tension positive).
  4. Resolve member forces into components using the member angles and solve.
  5. Carry the now-known forces to adjacent joints and repeat.

A positive result confirms the member is in tension. A negative result means the true force points the other way, so the member is in compression. Keep the sign convention consistent throughout.

Reading tension and compression

Tension members pull their joints inward and tend to stretch; compression members push their joints outward and tend to shorten. Compression members also risk buckling, so engineers often size them more generously than tension members of the same force. Labelling each solved member as T or C is part of a complete answer.

Why this matters for civil structures

Truss analysis is how roof frames, bridge spans and transmission towers are designed. Each member force feeds straight into a stress calculation (Οƒ=F/A\sigma = F/A) to choose a cross-section, and compression members get an extra buckling check. A single mis-signed force can lead to an undersized member, so the tension or compression label is as important as the magnitude.