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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. Find the vertical support reaction RA.
L = 5 mP1 = 60 kN at 1 mP2 = 55 kN at 3.5 m
RA = kN
2.Beam support reactionsHard
The simply supported beam has a pin at A and a roller at B. A load P acts at 3 m from A, inclined at 50° to the horizontal, and a vertical load Q acts at 5.5 m from A. Find the magnitude of the total reaction force RA at the pin A.
L = 6 mP = 35 kN at 3 m, θ = 50°Q = 80 kN at 5.5 m
RA = kN
3.Shear force & bending momentMedium
The simply supported beam carries two point loads. Find the maximum bending moment Mmax in the beam.
L = 6 mP1 = 55 kN at 1.5 mP2 = 45 kN at 3 m
Mmax = kN·m
4.Shear force & bending momentHard
The marks A to G split the beam into six equal parts. At which mark is the bending moment largest in size, sagging or hogging? Click it in the diagram.
30 kN @ 12 m45 kN @ 2 m
1A (x = 0 m)
2B (x = 2 m)
3C (x = 4 m)
4D (x = 6 m)
5E (x = 8 m)
6F (x = 10 m)
7G (x = 12 m)
5.Truss: method of jointsMedium
Use the method of joints to find the force FBC in member BC. Give tension as positive and compression as negative.
span = 5 mheight = 2 mB is 1 m from Avertical load = 50 kN
FBC = 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.
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 = 5 mE = 200 GPa (steel)I = 12 × 10⁶ mm⁴
δmax = mm
8.Beam deflectionHard
A simply supported beam carries a uniformly distributed load w. Its deflection may not exceed span/360. Find the smallest second moment of area Ireq that meets this limit.
w = 8 kN/mL = 8 mE = 70 GPa (aluminium)
Ireq = × 10⁶ mm⁴
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 = 3 mE = 200 GPa (steel)d = 50 mm
Pcr = kN
10.Column bucklingHard
A solid round column of length L made of steel is fixed at the base and free at the top. It must carry 100 kN with a factor of safety of 2.5 against buckling. Find the smallest diameter d.
P = 100 kNn = 2.5L = 1.5 mE = 200 GPa (steel)
d = mm
3Solutions
1.Beam support reactions
Answer: RA = 64.5 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·5 = 60·1 + 55·3.5
RB = 252.5/5 = 50.5 kN
ΣFy = 0: RA = 115 − 50.5 = 64.5 kN
Answer
RA = 64.5 kN
2.Beam support reactions
Answer: RA = 30.15 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 = 35·sin 50° = 26.81 kN
Ph = 35·cos 50° = 22.5 kN
Reactions
ΣMA = 0: RB·6 = 26.81·3 + 80·5.5 → RB = 86.74 kN
Ay = 26.81 + 80 − 86.74 = 20.07 kN
Ax = Ph = 22.5 kN
Resultant at A
RA = √(22.5² + 20.07²) = 30.15 kN
Answer
RA = 30.15 kN
3.Shear force & bending moment
Answer: Mmax = 108.8 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.
ΣMA = 0: RB·6 = 55·1.5 + 45·3
RB = 217.5/6 = 36.25 kN
ΣFy = 0: RA = 100 − 36.25 = 63.75 kN
Moment under each load
Keep the part left of each load.
under P1: M = RA·1.5 = 63.75·1.5 = 95.63 kN·m
under P2: M = RB·3 = 36.25·3 = 108.8 kN·m
Largest value
Mmax = 108.8 kN·m (under P2)
Answer
Mmax = 108.8 kN·m
4.Shear force & bending moment
Answer: E (x = 8 m)
Largest bending moment: M changes slope wherever the shear force changes, so its peaks sit where the shear force crosses zero: under a point load, inside a distributed load, or over a support of an overhang. At a fixed support of a cantilever the moment is largest at the wall. Compare the size of M at those places, sagging or hogging.
Support reactions
Take moments about one support, then use the vertical force balance.
R1 = 18.75 kN, R2 = 56.25 kN
Bending moment at every mark
Sum the moments of all forces on one side of the cut. Sagging is positive, hogging negative.
MA = 0, MB = 37.5, MC = −15, MD = −67.5, ME = −120 kN·m, MF = −60, MG = 0
Answer
Mark E: ME = −120 kN·m
5.Truss: method of joints
Answer: FBC = −22.36 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 = 50·1 → Cy = 10 kN
ΣFy = 0: Ay = 50 − 10 = 40 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 = 2/4.472 = 0.4472, cos γ = 4/4.472 = 0.8944
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 C
BC and CD 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 = 8 N/mm, L = 5000 mm
EI = 2.4 × 10¹² N·mm²
Deflection
δmax = 5wL⁴/(384EI) = 5·8·5000⁴/(384·2.4 × 10¹²) = 27.13 mm
Answer
δmax = 27.13 mm
8.Beam deflection
Answer: Ireq = 274.3 × 10⁶ mm⁴
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).
Deflection limit
δallow = L/360 = 8000/360 = 22.22 mm
Required second moment of area
I = 5wL⁴/(384·E·δallow) = 5·8·8000⁴/(384·70000·22.22) = 2.743 × 10⁸ mm⁴
Ireq = 274.3 × 10⁶ mm⁴
Answer
Ireq = 274.3 × 10⁶ mm⁴
9.Column buckling
Answer: Pcr = 137.3 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 = 2.5·100000 = 250000 N
KL = 2·1500 = 3000 mm
Solve for the diameter
d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·250000·3000²/(π³·200000))^(1/4) = 69.42 mm
Answer
d = 69.42 mm
Check: the slenderness KL/r is 172.9, so the column is slender and Euler applies.