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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 4.5 m and a point load P at 2 m from the wall. Find the magnitude of the reaction moment MA at the wall.
L = 6 mP = 60 kN at 2 mw = 10 kN/m from 0 to 4.5 m
MA = kN·m
2.Beam support reactionsHard
A compound beam is fixed to the wall at A, has an internal hinge at C (3 m from A) and rests on a roller at D (8 m from A). It carries a point load P at 4 m from A, a uniformly distributed load w on the whole part CD and a point load Q at 1 m from A. Find the reaction RD at the roller.
AC = 3 mAD = 8 mP = 75 kN at 4 mw = 8 kN/m from 3 to 8 mQ = 65 kN at 1 m
RD = kN
3.Shear force & bending momentMedium
Find the shear force Vx at the section x = 9 m from support A. Use sagging moments positive and upward shear on the left face positive.
L = 10 mw = 10 kN/m from 0 to 10 mx = 9 m
Vx = kN
4.Shear force & bending momentHard
The beam rests on a pin at A and a roller at B and overhangs B by 1.5 m to the free end C. A uniformly distributed load w acts over the whole length A–C. Find the bending moment MB at support B. Use sagging moments positive and upward shear on the left face positive.
L = 5.5 mw = 8 kN/m from 0 to 5.5 msupports at x = 0 and x = 4 m
MB = 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 = 4 mB is 7 m from Avertical load = 15 kN
FAB = kN
6.Truss: method of jointsHard
Use the method of joints to find the force FAC in member AC. Give tension as positive and compression as negative.
span = 6 mheight = 4 mB is 5 m from Avertical load = 35 kNhorizontal load = 20 kN →
FAC = 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 = 15 kN/mL = 1.5 mE = 11 GPa (timber)I = 84 × 10⁶ mm⁴
δmax = mm
8.Beam deflectionHard
A simply supported timber beam of rectangular section, 75 mm wide, carries a uniformly distributed load w over its whole span. Its midspan deflection may not exceed span/300. Find the smallest depth hreq of the section.
w = 1.5 kN/mL = 5 mE = 11 GPa (timber)b = 75 mm
hreq = mm
9.Column bucklingMedium
A column of length L made of steel is fixed at the base and free at the top. Using Euler’s formula, find its critical buckling load Pcr.
L = 5 mE = 200 GPa (steel)b × h = 30 × 60 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 mE = 70 GPa (aluminium)d = 80 mm
σcr = MPa
3Solutions
1.Beam support reactions
Answer: MA = 221.3 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 = 10·4.5 = 45 kN, x̄ = 2.25 m
Moment about the wall
MA = P·a + W·x̄ = 60·2 + 45·2.25 = 221.3 kN·m
Answer
MA = 221.3 kN·m
2.Beam support reactions
Answer: RD = 35 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. An internal hinge cannot carry a bending moment, which gives one extra equation: the moment about the hinge of the forces on either side is zero.
Part CD
The hinge has no moment, so moments about C on CD alone must balance.
W = 8·5 = 40 kN at 2.5 m from C
ΣMC = 0: RD·5 = 75·1 + 40·2.5
RD = 35 kN
VC = 115 − 35 = 80 kN
Answer
RD = 35 kN
3.Shear force & bending moment
Answer: Vx = −40 kN
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 = 10·10·5
RB = 500/10 = 50 kN
ΣFy = 0: RA = 100 − 50 = 50 kN
Cut at x = 9 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.
V = RA − (all downward loads left of the cut)
Vx = 50 − 10·9 = −40 kN
Answer
Vx = −40 kN
4.Shear force & bending moment
Answer: MB = −9 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. Maximum moment: since dM/dx = V, the bending moment has its peak where the shear force passes through zero, either at a point load or inside a distributed load.
Support reactions
Equilibrium of the whole beam, including the load on the overhang.
UDL resultant: W = w·ℓ = 8·5.5 = 44 kN, acting at x̄ = 2.75 m
ΣMA = 0: RB·4 = 8·5.5·2.75
RB = 121/4 = 30.25 kN
ΣFy = 0: RA = 44 − 30.25 = 13.75 kN
Cut at B and keep the overhang
The load on the overhang, w·a, acts at a/2 from B and makes the beam hog over the support.
MB = −w·a²/2 = −8·1.5²/2 = −9 kN·m
Answer
MB = −9 kN·m
5.Truss: method of joints
Answer: FAB = −3.779 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 = 15·7 → Cy = 13.13 kN
ΣFy = 0: Ay = 15 − 13.13 = 1.875 kN
Joint A
Assume every member is in tension (pulling away from the joint). Only AB has a vertical component at A.
sin α = 4/8.062 = 0.4961
ΣFy = 0: Ay + FAB·sin α = 0
FAB = −1.875/0.4961 = −3.779 kN
Answer
FAB = −3.779 kN (compression)
6.Truss: method of joints
Answer: FAC = 10.63 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·6 = 35·5 + 20·4 → Cy = 42.5 kN
ΣFy = 0: Ay = 35 − 42.5 = −7.5 kN
ΣFx = 0: Ax = −20 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 = 4/4.123 = 0.9701, cos γ = 1/4.123 = 0.2425
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 = 15 N/mm, L = 1500 mm
EI = 9.24 × 10¹¹ N·mm²
Deflection
δmax = 5wL⁴/(384EI) = 5·15·1500⁴/(384·9.24 × 10¹¹) = 1.07 mm
Answer
δmax = 1.07 mm
8.Beam deflection
Answer: hreq = 220 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.
bh³/12 = Ireq → h = (12·6.658 × 10⁷/75)1/3 = 220 mm
Answer
hreq = 220 mm
In practice, choose the next standard depth above this value.
9.Column buckling
Answer: Pcr = 2.665 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.
Smallest second moment of area
A rectangle buckles about its weak axis, using the smaller dimension cubed.
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.