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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 has a pin at A and a roller at B. It carries a point load P at 2 m from A and a counter-clockwise couple M at 4.5 m from A. Find the vertical reaction RA, taking upward as positive.
L = 5 mP = 35 kN at 2 mM = 10 kN·m (counter-clockwise) at 4.5 m
RA = kN
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 7 m from A, a uniformly distributed load w on the whole part CD and a point load Q at 2 m from A. Find the magnitude of the reaction moment MA at the wall.
AC = 3 mAD = 8 mP = 35 kN at 7 mw = 5 kN/m from 3 to 8 mQ = 40 kN at 2 m
MA = kN·m
3.Shear force & bending momentMedium
Find the bending moment Mx at the section x = 0.5 m from support A. Use sagging moments positive and upward shear on the left face positive.
L = 4 mw = 2 kN/m from 0 to 4 mx = 0.5 m
Mx = kN·m
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 = 6.5 mw = 8 kN/m from 0 to 6.5 msupports at x = 0 and x = 5 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 = 5 mheight = 4 mB is 2 m from Avertical load = 60 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 = 3 mB is 3 m from Avertical load = 30 kNhorizontal load = 20 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 = 10 kN/mL = 5 mE = 200 GPa (steel)I = 12 × 10⁶ mm⁴
δmax = mm
8.Beam deflectionHard
A simply supported timber beam of rectangular section, 100 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 = 4.5 mE = 11 GPa (timber)b = 100 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 = 1 mE = 200 GPa (steel)d = 30 mm
Pcr = kN
10.Column bucklingHard
A solid round column of length L made of steel is fixed at the base and pinned at the top. It must carry 10 kN with a factor of safety of 2 against buckling. Find the smallest diameter d.
P = 10 kNn = 2L = 6 mE = 200 GPa (steel)
d = mm
3Solutions
1.Beam support reactions
Answer: RA = 23 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.
Moments about A
Counter-clockwise positive.
ΣMA = 0: RB·5 − 35·2 + 10 = 0
RB = 60/5 = 12 kN
Vertical equilibrium
RA = 35 − 12 = 23 kN
Answer
RA = 23 kN
A negative reaction acts downward.
2.Beam support reactions
Answer: MA = 138.5 kN·m
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 = 5·5 = 25 kN at 2.5 m from C
ΣMC = 0: RD·5 = 35·4 + 25·2.5
RD = 40.5 kN
VC = 60 − 40.5 = 19.5 kN
Part AC
The hinge force VC acts downward on AC (equal and opposite to its action on CD).
RA = 40 + 19.5 = 59.5 kN
MA = 40·2 + 19.5·3 = 138.5 kN·m
Answer
MA = 138.5 kN·m
3.Shear force & bending moment
Answer: Mx = 1.75 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 = 2·4 = 8 kN, acting at x̄ = 2 m
ΣMA = 0: RB·4 = 2·4·2
RB = 16/4 = 4 kN
ΣFy = 0: RA = 8 − 4 = 4 kN
Cut at x = 0.5 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 = 4·0.5 − 2·0.5·0.25 = 1.75 kN·m
Answer
Mx = 1.75 kN·m
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 = 8·6.5 = 52 kN, acting at x̄ = 3.25 m
ΣMA = 0: RB·5 = 8·6.5·3.25
RB = 169/5 = 33.8 kN
ΣFy = 0: RA = 52 − 33.8 = 18.2 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 = −40.25 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·5 = 60·2 → Cy = 24 kN
ΣFy = 0: Ay = 60 − 24 = 36 kN
Joint A
Assume every member is in tension (pulling away from the joint). Only AB has a vertical component at A.
sin α = 4/4.472 = 0.8944
ΣFy = 0: Ay + FAB·sin α = 0
FAB = −36/0.8944 = −40.25 kN
Answer
FAB = −40.25 kN (compression)
6.Truss: method of joints
Answer: FBC = −7.906 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 = 30·3 − 20·3 → Cy = 7.5 kN
ΣFy = 0: Ay = 30 − 7.5 = 22.5 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 = 3/3.162 = 0.9487, cos γ = 1/3.162 = 0.3162
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 = 10 N/mm, L = 5000 mm
EI = 2.4 × 10¹² N·mm²
Deflection
δmax = 5wL⁴/(384EI) = 5·10·5000⁴/(384·2.4 × 10¹²) = 33.91 mm
Answer
δmax = 33.91 mm
8.Beam deflection
Answer: hreq = 179.9 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 = (12·4.854 × 10⁷/100)1/3 = 179.9 mm
Answer
hreq = 179.9 mm
In practice, choose the next standard depth above this value.
9.Column buckling
Answer: Pcr = 19.62 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 = 2·10000 = 20000 N
KL = 0.7·6000 = 4200 mm
Solve for the diameter
d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·20000·4200²/(π³·200000))^(1/4) = 43.68 mm
Answer
d = 43.68 mm
Check: the slenderness KL/r is 384.6, so the column is slender and Euler applies.