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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 cantilever beam is fixed to the wall at A. It carries a uniformly distributed load w from the wall to 2 m and a point load P at 3.5 m from the wall. Find the magnitude of the reaction moment MA at the wall.
L = 4 mP = 55 kN at 3.5 mw = 6 kN/m from 0 to 2 m
MA = kN·m
2.Beam support reactionsHard
The simply supported beam has a pin at A and a roller at B. Find the vertical support reaction RA.
L = 10 mP = 10 kN at 3 mw = 4 kN/m from 1 to 3 m
RA = kN
3.Shear force & bending momentMedium
Find the bending moment Mx at the section x = 1 m from support A. Use sagging moments positive and upward shear on the left face positive.
L = 5 mw = 8 kN/m from 0 to 5 mx = 1 m
Mx = kN·m
4.Shear force & bending momentHard
Find the bending moment Mx at the section x = 1.5 m from support A. Use sagging moments positive and upward shear on the left face positive.
L = 5 mP = 60 kN at 1 mw = 4 kN/m from 0 to 5 mx = 1.5 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 = 6 mheight = 2 mB is 5 m from Avertical load = 55 kN
FAB = kN
6.Truss: method of jointsHard
Use the method of joints to find the force FBC in member BC. Give tension as positive and compression as negative.
span = 4 mheight = 2 mB is 1 m from Avertical load = 50 kNhorizontal load = 30 kN ←
FBC = kN
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 = 8 kN/mL = 3 mE = 200 GPa (steel)I = 23 × 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 = 15 kNw = 8 kN/mL = 1.5 mE = 11 GPa (timber)I = 23 × 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 = 5 mE = 200 GPa (steel)d = 25 mm
Pcr = kN
10.Column bucklingHard
A solid round column of length L made of steel is pinned at both ends. It must carry 75 kN with a factor of safety of 2 against buckling. Find the smallest diameter d.
P = 75 kNn = 2L = 4 mE = 200 GPa (steel)
d = mm
3Solutions
1.Beam support reactions
Answer: MA = 204.5 kN·m
Cantilever equilibrium: a fixed support can push up and also resist rotation, so it gives a vertical reaction RA and a reaction moment MA. ΣFy = 0 gives RA, and moments about the wall give MA = Σ(load × distance from the wall). A distributed load acts as its resultant at the centroid of the load diagram.
Resultant of the distributed load
W = 6·2 = 12 kN, x̄ = 1 m
Moment about the wall
MA = P·a + W·x̄ = 55·3.5 + 12·1 = 204.5 kN·m
Answer
MA = 204.5 kN·m
2.Beam support reactions
Answer: RA = 13.4 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 = 4·2 = 8 kN, acting at x̄ = 2 m
ΣMA = 0: RB·10 = 10·3 + 4·2·2
RB = 46/10 = 4.6 kN
ΣFy = 0: RA = 18 − 4.6 = 13.4 kN
Answer
RA = 13.4 kN
3.Shear force & bending moment
Answer: Mx = 16 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 = 8·5 = 40 kN, acting at x̄ = 2.5 m
ΣMA = 0: RB·5 = 8·5·2.5
RB = 100/5 = 20 kN
ΣFy = 0: RA = 40 − 20 = 20 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 = 20·1 − 8·1·0.5 = 16 kN·m
Answer
Mx = 16 kN·m
4.Shear force & bending moment
Answer: Mx = 52.5 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 = 4·5 = 20 kN, acting at x̄ = 2.5 m
ΣMA = 0: RB·5 = 60·1 + 4·5·2.5
RB = 110/5 = 22 kN
ΣFy = 0: RA = 80 − 22 = 58 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)
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·6 = 55·5 → Cy = 45.83 kN
ΣFy = 0: Ay = 55 − 45.83 = 9.167 kN
Joint A
Assume every member is in tension (pulling away from the joint). Only AB has a vertical component at A.
sin α = 2/5.385 = 0.3714
ΣFy = 0: Ay + FAB·sin α = 0
FAB = −9.167/0.3714 = −24.68 kN
Answer
FAB = −24.68 kN (compression)
6.Truss: method of joints
Answer: FBC = 4.507 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·4 = 50·1 − 30·2 → Cy = −2.5 kN
ΣFy = 0: Ay = 50 − −2.5 = 52.5 kN
ΣFx = 0: Ax = 30 kN
Joint C
The roller gives only a vertical reaction, so joint C has just two unknown member forces. Assume both in tension.
sin γ = 2/3.606 = 0.5547, cos γ = 3/3.606 = 0.8321
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 = 8 N/mm, L = 3000 mm
EI = 4.6 × 10¹² N·mm²
Deflection
δmax = 5wL⁴/(384EI) = 5·8·3000⁴/(384·4.6 × 10¹²) = 1.834 mm
Answer
δmax = 1.834 mm
8.Beam deflection
Answer: δmax = 6.253 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 = 15000 N, w = 8 N/mm, L = 1500 mm, EI = 2.53 × 10¹¹ N·mm²
Each load on its own
δP = PL³/(48EI) = 15000·1500³/(48·2.53 × 10¹¹) = 4.169 mm
δw = 5wL⁴/(384EI) = 5·8·1500⁴/(384·2.53 × 10¹¹) = 2.084 mm
Add them
δmax = 4.169 + 2.084 = 6.253 mm
Answer
δmax = 6.253 mm
9.Column buckling
Answer: Pcr = 6.056 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.
Required critical load
Pcr = n·P = 2·75000 = 150000 N
KL = 1·4000 = 4000 mm
Solve for the diameter
d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·150000·4000²/(π³·200000))^(1/4) = 70.55 mm
Answer
d = 70.55 mm
Check: the slenderness KL/r is 226.8, so the column is slender and Euler applies.