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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 7 m from A and a counter-clockwise couple M at 6 m from A. Find the vertical reaction RA, taking upward as positive.
L = 8 mP = 25 kN at 7 mM = 30 kN·m (counter-clockwise) at 6 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 1 m from A, inclined at 50° to the horizontal, and a vertical load Q acts at 2.5 m from A. Find the angle α between the total reaction force at the pin A and the horizontal.
L = 5 mP = 20 kN at 1 m, θ = 50°Q = 30 kN at 2.5 m
α = °
3.Shear force & bending momentMedium
Find the bending moment Mx at the section x = 8 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 = 8 m
Mx = kN·m
4.Shear force & bending momentHard
The simply supported beam carries a uniformly distributed load over part of its span. Find the distance x0 from A to the section where the bending moment is largest.
L = 5 mw = 24 kN/m from 2 to 4 m
x0 = m
5.Truss: method of jointsMedium
Exactly one member of this truss carries no force under these loads. Which is the zero-force member? Click it in the diagram.
D: 35 kN ↓G: 40 kN ↓H: 10 kN ↓
1member AB
2member BC
3member CD
4member DE
5member FG
6member GH
7member AF
8member HE
9member BF
10member CG
11member DH
12member BG
13member DG
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 point load P at a = 6 m from support A. Find the deflection δP under the load.
P = 22 kNa = 6 mL = 8 mE = 200 GPa (steel)I = 8.5 × 10⁶ mm⁴
δP = mm
8.Beam deflectionHard
A propped cantilever is fixed at A and simply supported (propped) at B. It carries a uniformly distributed load w over its whole length. EI is constant. Find the reaction RB at the prop.
L = 6 mw = 15 kN/m
RB = kN
9.Column bucklingMedium
A column of length L made of steel is pinned at both ends. Using Euler’s formula, find its critical buckling load Pcr.
L = 6 mE = 200 GPa (steel)b × h = 25 × 80 mm
Pcr = kN
10.Column bucklingHard
A solid round column of length L made of steel is pinned at both ends. It must carry 145 kN with a factor of safety of 2.5 against buckling. Find the smallest diameter d.
P = 145 kNn = 2.5L = 5 mE = 200 GPa (steel)
d = mm
3Solutions
1.Beam support reactions
Answer: RA = 6.875 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·8 − 25·7 + 30 = 0
RB = 145/8 = 18.13 kN
Vertical equilibrium
RA = 25 − 18.13 = 6.875 kN
Answer
RA = 6.875 kN
A negative reaction acts downward.
2.Beam support reactions
Answer: α = 64.75 °
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 = 20·sin 50° = 15.32 kN
Ph = 20·cos 50° = 12.86 kN
Reactions
ΣMA = 0: RB·5 = 15.32·1 + 30·2.5 → RB = 18.06 kN
Ay = 15.32 + 30 − 18.06 = 27.26 kN
Ax = Ph = 12.86 kN
Direction at A
α = atan(Ay/Ax) = atan(27.26/12.86) = 64.75°
Answer
α = 64.75°
3.Shear force & bending moment
Answer: Mx = 80 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 = 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 = 8 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 = 50·8 − 10·8·4 = 80 kN·m
Answer
Mx = 80 kN·m
4.Shear force & bending moment
Answer: x0 = 2.8 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.
UDL resultant: W = w·ℓ = 24·2 = 48 kN, acting at x̄ = 3 m
ΣMA = 0: RB·5 = 24·2·3
RB = 144/5 = 28.8 kN
ΣFy = 0: RA = 48 − 28.8 = 19.2 kN
Zero shear
The shear force starts at RA, stays constant over any unloaded part and falls with slope w inside the load.
RA − w·(x0 − 2) = 0
x0 = 2 + 19.2/24 = 2.8 m
Answer
x0 = 2.8 m
5.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 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).
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 D
CD and DE lie on one straight line and the joint carries no load. Balancing forces across that line leaves only DH.
ΣF⊥ = 0 → FDH = 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.
P = 22000 N, a = 6000 mm, b = 2000 mm, L = 8000 mm
EI = 1.7 × 10¹² N·mm²
Deflection under the load
δP = Pa²b²/(3EIL) = 22000·6000²·2000²/(3·1.7 × 10¹²·8000) = 77.65 mm
Answer
δP = 77.65 mm
8.Beam deflection
Answer: RB = 33.75 kN
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). For a statically indeterminate beam, remove a redundant support and require the deflection there to be zero (compatibility).
Remove the prop
Without the prop the beam is a cantilever. Its free end would deflect under the load.
δload = wL⁴/(8EI)
Compatibility at the prop
The prop force RB alone lifts the free end by RBL³/(3EI). The prop holds B at zero deflection, so the two must cancel. EI cancels out.
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.
Required critical load
Pcr = n·P = 2.5·145000 = 362500 N
KL = 1·5000 = 5000 mm
Solve for the diameter
d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·362500·5000²/(π³·200000))^(1/4) = 98.34 mm
Answer
d = 98.34 mm
Check: the slenderness KL/r is 203.4, so the column is slender and Euler applies.