Trusses: Method of Sections

Introduction

The method of sections is used to determine forces in specific truss members without solving the entire truss joint-by-joint. By passing an imaginary cut through the truss and analyzing one section using equilibrium equations, internal member forces can be solved directly. This method is especially efficient when only a few member forces are required.

Method of Sections Procedure

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  1. Solve support reactions using global equilibrium.

  2. Cut a section through desired members.

  3. Isolate one side of the truss.

  4. Draw section free-body diagram.

  5. Assume unknown member forces are in tension.

  6. Apply equilibrium equations:

    1. Σ F x = 0 \Sigma F_{x} = 0

    2. Σ F y = 0 \Sigma F_{y} = 0

    3. Σ M = 0 \Sigma M = 0

  7. Positive result → \rightarrow tension

  8. Negative result → \rightarrow compression

Choosing the Best Cut

  • Pass through the target members.

  • Cut through no more than 3 unknown members (3 unknown forces).

  • Use moments around intersection points of unknown members or joints where multiple unknowns pass through.

Example:
Find the force in member LK and if the member is in tension or compression.

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1) Start with Global Equilibrium to solve for Reaction Forces at points A and G:

Σ F x = 0 = A x \Sigma F_{x} = 0 = A_{x}

Σ F y = 0 = A y + G y − 10 k N − 20 k N − 10 k N \Sigma F_{y} = 0 = A_{y} + G_{y} - 10\ kN - 20\ kN - 10\ kN

A y + G y = 40 k N A_{y} + G_{y} = 40\ kN

⟳ + Σ M G = 0 = ( A y ) ( 12 m ) − ( 10 k N ) ( 8 m ) − ( 20 k N ) ( 6 m ) − ( 10 k N ) ( 4 m ) ⟳^{+}\ \Sigma M_{G} = 0 = (A_{y})(12\ m) - (10\ kN)(8\ m) - (20\ kN)(6\ m) - (10\ kN)(4\ m)

Solving: A y = 20 k N A_{y} = 20\ kN

Substituting into A y + G y = 40 k N A_{y} + G_{y} = 40\ kN : G y = 20 k N G_{y} = 20\ kN

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2) Cut the truss vertically through member LK, and take moments about point C to cancel out LC and BC

Moment arm from F L K F_{LK} to point C is length LC, or 2 2 + 2 2 \sqrt{2^2+2^2}

Moment arm from A y A_{y} to point C is length AC, or 4 m 4\ m

⟳ + Σ M C = 0 = ( 20 k N ) ( 4 m ) + ( F L K ) ( 2 2 + 2 2 ) ⟳^{+}\ \Sigma M_{C} = 0 = (20\ kN)(4\ m) + (F_{LK})(\sqrt{2^2+2^2})

Solving: F L K = − 28.28 N F_{LK} = - 28.28\ N

F L K = 28.28 N ( C ) F_{LK} = 28.28\ N\ (C)