Trusses, Frames and Virtual Work
Analysis of plane trusses by the method of joints and method of sections, zero-force members, determinacy m = 2j − 3, and the principle of virtual work.
A truss is a structure of straight members joined at their ends by pins, loaded only at the joints. Every member is then a two-force member: it is either in tension or compression.
Determinacy
For a plane truss with m members, j joints and r support reactions:
- m + r = 2j: statically determinate (with r = 3, m = 2j − 3).
- m + r > 2j: indeterminate (redundant members).
- m + r < 2j: a mechanism (unstable).
Method of joints
Take one joint at a time, starting where there are at most two unknown member forces, and apply ΣFx = 0 and ΣFy = 0. Assume every unknown force is tensile (pulling away from the joint); a negative answer means compression.
Method of sections
To find the force in one member in the middle of a truss, cut through at most three members including it, and apply the three equilibrium equations to one side. Take moments about the point where the other two cut members meet: the equation then has only the wanted force.
Zero-force members
Spotting them saves time:
- At a joint with two non-collinear members and no load, both members carry zero force.
- At a joint with three members, two of them collinear, and no load, the third member carries zero force.
Principle of virtual work
If a body in equilibrium is given a small virtual displacement compatible with its constraints, the total virtual work done by the external forces is zero: Σ F·δs = 0.
It is useful for mechanisms such as levers, linkages and screw jacks: write each displacement in terms of one coordinate and solve one equation, without finding reactions.
Example (lever): effort P at 2 m from the fulcrum lifts a load W at 0.5 m. A small rotation δθ gives P(2 δθ) − W(0.5 δθ) = 0, so P = W/4.
Worked example
A triangular truss ABC has A pinned, B on a roller, AB = 4 m horizontal, and C at the apex 2 m above the midpoint of AB. A vertical load of 20 kN acts at C.
- By symmetry, R_A = R_B = 10 kN.
- At joint A: member AC is at angle α with tan α = 2/2 = 1, so α = 45°. Vertical: F_AC sin 45° + 10 = 0, so F_AC = −14.14 kN (compression).
- Horizontal: F_AB + F_AC cos 45° = 0, so F_AB = +10 kN (tension).
Practice
A plane truss has 7 joints and is supported by a pin and a roller (r = 3). How many members does it need to be just determinate?
Show answer and explanation
Answer: 11m = 2j − 3 = 14 − 3 = 11.
In the worked example, if the apex were 4 m above the midpoint of AB instead, what would be the compressive force in AC in kN? (Give 2 decimal places.)
Show answer and explanation
Answer: 11.18Now sin α = 4/√20 = 0.894, so F_AC = 10/0.894 = 11.18 kN in compression.
At an unloaded joint, three members meet; two of them are collinear. The force in the third member is:
Show answer and explanation
Answer: AResolving perpendicular to the collinear pair, only the third member has a component, so its force must be zero.
A lever has effort arm 1.5 m and load arm 0.3 m. Using virtual work, what effort lifts a load of 500 N?
Show answer and explanation
Answer: 100P × 1.5 δθ = 500 × 0.3 δθ, so P = 100 N.