A simply supported beam carries a point load P at a = 3 m from support A. Find the deflection δP under the load.
P = 6 kNa = 3 mL = 5 mE = 11 GPa (timber)I = 23 × 10⁶ mm⁴
δP = mm
8.Beam deflectionHard
A simply supported beam carries a uniformly distributed load w and a point load P at midspan. Using superposition, find the midspan deflection δmax.
P = 12 kNw = 20 kN/mL = 6 mE = 70 GPa (aluminium)I = 84 × 10⁶ mm⁴
δmax = mm
9.Column bucklingMedium
A column of length L made of steel is fixed at both ends. Using Euler’s formula, find its critical buckling load Pcr.
L = 1 mE = 200 GPa (steel)d = 20 mm
Pcr = kN
10.Column bucklingHard
A column of length L made of aluminium is fixed at the base and free at the top. Find its slenderness and the critical buckling stress σcr from Euler’s formula.
L = 2.5 mE = 70 GPa (aluminium)d = 80 mm
σcr = MPa
3Solutions
1.Beam support reactions
Answer: RA = 20 kN
Static equilibrium: a body at rest has ΣFx = 0, ΣFy = 0 and ΣM = 0 about any point. Taking moments about one support removes that support’s reaction from the equation.
Free-body diagram
Replace the supports with reaction forces. A roller gives one vertical reaction; with only vertical loads the pin gives one vertical reaction too.
Equilibrium
Moments about A, counter-clockwise positive. Then vertical force balance.
ΣMA = 0: RB·8 = 50·6 + 60·7
RB = 720/8 = 90 kN
ΣFy = 0: RA = 110 − 90 = 20 kN
Answer
RA = 20 kN
2.Beam support reactions
Answer: RB = 29 kN
Static equilibrium: a body at rest has ΣFx = 0, ΣFy = 0 and ΣM = 0 about any point. Taking moments about one support removes that support’s reaction from the equation.
Free-body diagram
Replace the supports with reaction forces. A roller gives one vertical reaction; with only vertical loads the pin gives one vertical reaction too.
Equilibrium
Moments about A, counter-clockwise positive. Then vertical force balance.
UDL resultant: W = w·ℓ = 10·1 = 10 kN, acting at x̄ = 2.5 m
ΣMA = 0: RB·5 = 40·3 + 10·1·2.5
RB = 145/5 = 29 kN
ΣFy = 0: RA = 50 − 29 = 21 kN
Answer
RB = 29 kN
3.Shear force & bending moment
Answer: Mx = 13.5 kN·m
Method of sections: cut the beam where you want the internal forces and keep one side. The shear force V balances the vertical forces on that side, and the bending moment M balances their moments about the cut.
Support reactions
Equilibrium of the whole beam.
UDL resultant: W = w·ℓ = 4·6 = 24 kN, acting at x̄ = 3 m
ΣMA = 0: RB·6 = 4·6·3
RB = 72/6 = 12 kN
ΣFy = 0: RA = 24 − 12 = 12 kN
Cut at x = 1.5 m and keep the left part
Only forces left of the cut appear. A UDL portion acts as one force at the middle of that portion.
M = RA·x − (each load left of the cut × its distance to the cut)
Mx = 12·1.5 − 4·1.5·0.75 = 13.5 kN·m
Answer
Mx = 13.5 kN·m
4.Shear force & bending moment
Answer: Mx = 50.5 kN·m
Method of sections: cut the beam where you want the internal forces and keep one side. The shear force V balances the vertical forces on that side, and the bending moment M balances their moments about the cut.
Support reactions
Equilibrium of the whole beam.
UDL resultant: W = w·ℓ = 10·10 = 100 kN, acting at x̄ = 5 m
ΣMA = 0: RB·10 = 55·9 + 10·10·5
RB = 995/10 = 99.5 kN
ΣFy = 0: RA = 155 − 99.5 = 55.5 kN
Cut at x = 1 m and keep the left part
Only forces left of the cut appear. A UDL portion acts as one force at the middle of that portion.
M = RA·x − (each load left of the cut × its distance to the cut)
Mx = 55.5·1 − 10·1·0.5 = 50.5 kN·m
Answer
Mx = 50.5 kN·m
5.Truss: method of joints
Answer: member BF
Zero-force members: at a joint, the forces must balance in every direction. If a joint has no load and no support, and two of its three members are in line, then the balance across that line involves only the third member, so its force is zero. If only two members meet at an unloaded joint and they are not in line, both are zero.
Joint B
AB and BC lie on one straight line and the joint carries no load. Balancing forces across that line leaves only BF.
ΣF⊥ = 0 → FBF = 0
Check with the method of joints
Solving all joints gives these member forces (T = tension, C = compression).
Zero-force members: at a joint, the forces must balance in every direction. If a joint has no load and no support, and two of its three members are in line, then the balance across that line involves only the third member, so its force is zero. If only two members meet at an unloaded joint and they are not in line, both are zero.
Joint B
AB and BC lie on one straight line and the joint carries no load. Balancing forces across that line leaves only BF.
ΣF⊥ = 0 → FBF = 0
Check with the method of joints
Solving all joints gives these member forces (T = tension, C = compression).
Beam deflection: deflections come from integrating the curvature M/(EI) twice. Standard cases are tabulated, for example PL³/(3EI) for a cantilever with an end load and 5wL⁴/(384EI) for a simply supported beam under a full uniform load. Deflections from separate loads add (superposition).
Consistent units
Work in N and mm: P in N, w in N/mm (kN/m = N/mm), L in mm, E in N/mm² (GPa × 1000), I in mm⁴.
P = 6000 N, a = 3000 mm, b = 2000 mm, L = 5000 mm
EI = 2.53 × 10¹¹ N·mm²
Deflection under the load
δP = Pa²b²/(3EIL) = 6000·3000²·2000²/(3·2.53 × 10¹¹·5000) = 56.92 mm
Answer
δP = 56.92 mm
8.Beam deflection
Answer: δmax = 66.58 mm
Beam deflection: deflections come from integrating the curvature M/(EI) twice. Standard cases are tabulated, for example PL³/(3EI) for a cantilever with an end load and 5wL⁴/(384EI) for a simply supported beam under a full uniform load. Deflections from separate loads add (superposition).
Consistent units
Work in N and mm: P in N, w in N/mm (kN/m = N/mm), L in mm, E in N/mm² (GPa × 1000), I in mm⁴.
P = 12000 N, w = 20 N/mm, L = 6000 mm, EI = 5.88 × 10¹² N·mm²
Each load on its own
δP = PL³/(48EI) = 12000·6000³/(48·5.88 × 10¹²) = 9.184 mm
δw = 5wL⁴/(384EI) = 5·20·6000⁴/(384·5.88 × 10¹²) = 57.4 mm
Add them
δmax = 9.184 + 57.4 = 66.58 mm
Answer
δmax = 66.58 mm
9.Column buckling
Answer: Pcr = 62.01 kN
Euler buckling: a slender column becomes unstable at Pcr = π²EI/(KL)², where KL is the effective length: K = 1 for pinned–pinned, 2 for fixed–free, 0.7 for fixed–pinned and 0.5 for fixed–fixed. It buckles about the axis with the smallest I. The formula holds for slender columns, whose critical stress stays below the yield stress.
Euler buckling: a slender column becomes unstable at Pcr = π²EI/(KL)², where KL is the effective length: K = 1 for pinned–pinned, 2 for fixed–free, 0.7 for fixed–pinned and 0.5 for fixed–fixed. It buckles about the axis with the smallest I. The formula holds for slender columns, whose critical stress stays below the yield stress.