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1Formulas and methods
Beam support reactions
Equilibrium
ΣFx = 0, ΣFy = 0, ΣM = 0
Uniform load
resultant w·L at the middle of the load
Moment
M = F·d
Method
Draw a free-body diagram and replace each support by its reactions.
Replace every distributed load by a single force at its centroid.
Take moments about one support to find the reaction at the other.
Use ΣFy = 0 to find the remaining reaction, and check with a second moment equation.
Shear force & bending moment
Shear and moment
V = ΣF on one side, M = ΣF·d on one side
Bending stress
σ = M·y/I
Rectangle
I = bh³/12
Section modulus
W = I/ymax
Simply supported, uniform load
Mmax = wL²/8
Method
Find the support reactions from equilibrium of the whole beam.
Cut the beam at the section you need and keep one side.
Shear force: sum of the vertical forces on that side. Bending moment: sum of their moments about the cut.
For the maximum moment, find where the shear force is zero.
Truss: method of joints
Method of joints
ΣFx = 0, ΣFy = 0 at each joint
Method of sections
ΣM = 0 about a cut point
Member force
positive = tension, negative = compression
Method
Find the support reactions for the whole truss.
Method of joints: start at a joint with at most two unknown member forces and use ΣFx = 0 and ΣFy = 0.
Method of sections: cut through the member you need and take moments about a point where the other unknown members meet.
Assume tension; a negative answer means compression.
Beam deflection
Point load at midspan
δ = PL³/(48EI)
Uniform load, simply supported
δ = 5wL⁴/(384EI)
Cantilever, end load
δ = PL³/(3EI)
Cantilever, uniform load
δ = wL⁴/(8EI)
Superposition
δ = δ1 + δ2
Column buckling
Euler load
Pcr = π²EI/(KL)²
Effective length factor
K = 1 pinned–pinned, 0.5 fixed–fixed, 0.7 fixed–pinned, 2 fixed–free
Critical stress
σcr = Pcr/A
Slenderness
λ = KL/r, r = √(I/A)
2Practice problems
1.Beam support reactionsMedium
The simply supported beam (pin at A, roller at B) carries a linearly varying load that falls from 4 kN/m at A to zero at B. A point load P also acts at 2.5 m from A. Find the vertical support reaction RB.
L = 5 mw0 = 4 kN/mP = 10 kN at 2.5 m
RB = kN
2.Beam support reactionsHard
The simply supported beam has a pin at A and a roller at B. A load P acts at 5.5 m from A, inclined at 45° to the horizontal, and a vertical load Q acts at 3.5 m from A. Find the magnitude of the total reaction force RA at the pin A.
L = 6 mP = 55 kN at 5.5 m, θ = 45°Q = 45 kN at 3.5 m
RA = kN
3.Shear force & bending momentMedium
The cantilever is fixed at A. It carries a uniformly distributed load w over its whole length and a point load P at 3 m from A. Find the bending moment Mx at the section x = 0.5 m from the fixed support A. Use sagging moments positive and upward shear on the left face positive.
L = 3 mP = 20 kN at 3 mw = 10 kN/m from 0 to 3 mx = 0.5 m
Mx = kN·m
4.Shear force & bending momentHard
Find the bending moment Mx at the section x = 3 m from support A. Use sagging moments positive and upward shear on the left face positive.
L = 6 mP = 50 kN at 1.5 mw = 8 kN/m from 0 to 6 mx = 3 m
Mx = kN·m
5.Truss: method of jointsMedium
Use the method of joints to find the force FAB in member AB. Give tension as positive and compression as negative.
span = 8 mheight = 2 mB is 3 m from Avertical load = 30 kN
FAB = kN
6.Truss: method of jointsHard
Exactly one member of this truss carries no force under these loads. Which is the zero-force member? Click it in the diagram.
B: 20 kN ↓C: 40 kN ↓D: 40 kN ↓H: 35 kN ←
1member AB
2member BC
3member CD
4member DE
5member FG
6member GH
7member AF
8member HE
9member BF
10member CG
11member DH
12member FC
13member HC
7.Beam deflectionMedium
A simply supported beam carries a uniformly distributed load w over its whole span. Find the maximum deflection δmax, at midspan.
w = 4 kN/mL = 8 mE = 200 GPa (steel)I = 36 × 10⁶ mm⁴
δmax = 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 = 30 kNw = 15 kN/mL = 1.5 mE = 11 GPa (timber)I = 57 × 10⁶ mm⁴
δmax = mm
9.Column bucklingMedium
A column of length L made of steel is fixed at the base and pinned at the top. Using Euler’s formula, find its critical buckling load Pcr.
L = 2 mE = 200 GPa (steel)d = 30 mm
Pcr = kN
10.Column bucklingHard
A column of length L made of steel is fixed at the base and pinned at the top. Find its slenderness and the critical buckling stress σcr from Euler’s formula.
L = 3 mE = 200 GPa (steel)d = 40 mm
σcr = MPa
3Solutions
1.Beam support reactions
Answer: RB = 8.333 kN
Static equilibrium: a body at rest has ΣFx = 0, ΣFy = 0 and ΣM = 0 about any point. Replace each distributed load by its resultant (its area) acting at the centroid of the load diagram, and take moments about a support to remove that support’s reaction from the equation.
Resultant of the triangular load
W = ½·4·5 = 10 kN
x̄ = L/3 = 1.667 m
Equilibrium
Moments about A, counter-clockwise positive. Then vertical force balance.
ΣMA = 0: RB·5 = 10·1.667 + 10·2.5
RB = 8.333 kN
RA = 20 − 8.333 = 11.67 kN
Answer
RB = 8.333 kN
2.Beam support reactions
Answer: RA = 44.68 kN
Static equilibrium: a body at rest has ΣFx = 0, ΣFy = 0 and ΣM = 0 about any point. Replace each distributed load by its resultant (its area) acting at the centroid of the load diagram, and take moments about a support to remove that support’s reaction from the equation.
Components of P
Pv = 55·sin 45° = 38.89 kN
Ph = 55·cos 45° = 38.89 kN
Reactions
ΣMA = 0: RB·6 = 38.89·5.5 + 45·3.5 → RB = 61.9 kN
Ay = 38.89 + 45 − 61.9 = 21.99 kN
Ax = Ph = 38.89 kN
Resultant at A
RA = √(38.89² + 21.99²) = 44.68 kN
Answer
RA = 44.68 kN
3.Shear force & bending moment
Answer: Mx = −81.25 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.
Keep the free-end part
P: −20·2.5 = −50 kN·m
w: −10·2.5²/2 = −31.25 kN·m
Mx = −50 − 31.25 = −81.25 kN·m
Answer
Mx = −81.25 kN·m
Negative means hogging: tension on the top face.
4.Shear force & bending moment
Answer: Mx = 73.5 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 = 8·6 = 48 kN, acting at x̄ = 3 m
ΣMA = 0: RB·6 = 50·1.5 + 8·6·3
RB = 219/6 = 36.5 kN
ΣFy = 0: RA = 98 − 36.5 = 61.5 kN
Cut at x = 3 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 = 61.5·3 − 50·(3 − 1.5) − 8·3·1.5 = 73.5 kN·m
Answer
Mx = 73.5 kN·m
5.Truss: method of joints
Answer: FAB = −33.8 kN
Method of joints: every pin of a truss is in equilibrium, so ΣFx = 0 and ΣFy = 0 at each joint. Start at a joint with at most two unknown member forces. A negative result means the member is in compression.
Support reactions
Equilibrium of the whole truss. Moments about A, counter-clockwise positive.
ΣMA = 0: Cy·8 = 30·3 → Cy = 11.25 kN
ΣFy = 0: Ay = 30 − 11.25 = 18.75 kN
Joint A
Assume every member is in tension (pulling away from the joint). Only AB has a vertical component at A.
sin α = 2/3.606 = 0.5547
ΣFy = 0: Ay + FAB·sin α = 0
FAB = −18.75/0.5547 = −33.8 kN
Answer
FAB = −33.8 kN (compression)
6.Truss: method of joints
Answer: member CG
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 G
FG and GH lie on one straight line and the joint carries no load. Balancing forces across that line leaves only CG.
ΣF⊥ = 0 → FCG = 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.
w = 4 N/mm, L = 8000 mm
EI = 7.2 × 10¹² N·mm²
Deflection
δmax = 5wL⁴/(384EI) = 5·4·8000⁴/(384·7.2 × 10¹²) = 29.63 mm
Answer
δmax = 29.63 mm
8.Beam deflection
Answer: δmax = 4.941 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 = 30000 N, w = 15 N/mm, L = 1500 mm, EI = 6.27 × 10¹¹ N·mm²
Each load on its own
δP = PL³/(48EI) = 30000·1500³/(48·6.27 × 10¹¹) = 3.364 mm
δw = 5wL⁴/(384EI) = 5·15·1500⁴/(384·6.27 × 10¹¹) = 1.577 mm
Add them
δmax = 3.364 + 1.577 = 4.941 mm
Answer
δmax = 4.941 mm
9.Column buckling
Answer: Pcr = 40.04 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.