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Engineering reference // structural mechanics

Drawing No. EH–CS–014 // Civil & Structural Engineering

Structural Engineering Formula Sheet

A mechanics-first structural reference for preliminary member behavior. These equations describe elastic stress, deformation and idealized instability; they do not replace code-specific strength, stability, serviceability, connection, seismic, fire or load-combination requirements.

Fast reference, with engineering context

Use the equations directly for screening calculations, then open the linked EngineerHub tools for input handling and unit conversion. Formula applicability and major limitations are stated beside each relation.

Reference conventions

σ = P/AAxial normal stress
σ = My/IElastic bending stress
EIFlexural rigidity
Pcr = π²EI/(KL)²Euler elastic buckling

Simply supported beam under load

SIMPLY SUPPORTED BEAM · SHEAR AND MOMENT P L/2 L/2 SHEAR V +P/2 −P/2 MOMENT M Mmax = PL/4 δmax = PL³/48EI
Structural formulas connect external loading to internal force resultants, stresses and elastic deformation. Boundary conditions and load paths are part of the model.

01 // Axial stress, strain and elongation

For a prismatic member under concentric axial load in the linear-elastic range, stress is uniform and elongation follows Hooke’s law.

Core relation
σ = P/A
ε = σ/E   ;   δ = PL/(AE)
SymbolMeaningSI unitsUS customary
PAxial forceNlbf
ACross-sectional aream², mm²in²
σNormal stressPa, MPapsi, ksi
EYoung’s modulusPa, GPapsi, Msi
LMember lengthmin, ft
δAxial elongationm, mmin
Worked example — steel tie elongation

Given: P = 120 kN, A = 2000 mm², L = 2.0 m, E = 200 GPa.

σ = 120000/0.002 = 60 MPa
δ = PL/(AE) = 0.00060 m = 0.60 mm
Answer: σ = 60 MPa; δ = 0.60 mm.

US check: ≈8.70 ksi and 0.0236 in.

Concentric loading and linear elasticity are assumed.

Eccentricity creates bending. Net-section effects, holes, yielding, fracture and connection behavior require separate checks.

02 // Common section properties

Second moment of area controls bending stiffness; section modulus connects moment directly to extreme-fiber elastic bending stress.

Core relation
Irect = bh³/12   ;   Z = I/c
Icircle = πd⁴/64   ;   Jsolid circle = πd⁴/32
SymbolMeaningSI unitsUS customary
ISecond moment of aream⁴, mm⁴in⁴
ZElastic section modulusm³, mm³in³
JPolar second moment (circular shaft)m⁴, mm⁴in⁴
b,h,dSection dimensionsm, mmin
cNeutral-axis to extreme fiberm, mmin
Worked example — 100×200 mm rectangle

Given: b = 0.100 m, h = 0.200 m.

I = 0.1×0.2³/12 = 6.667×10⁻⁵ m⁴
Z = I/(h/2) = 6.667×10⁻⁴ m³
Answer: I = 6.667×10⁻⁵ m⁴; Z = 6.667×10⁻⁴ m³.

Use the axis corresponding to the actual bending direction.

Principal-axis orientation, composite sections, transformed sections and local plate behavior can materially change stiffness and strength.

03 // Elastic bending stress

For Euler–Bernoulli beam bending in the linear-elastic range, normal stress varies linearly from the neutral axis.

Core relation
σ = My/I
σmax = M/Z
SymbolMeaningSI unitsUS customary
MBending momentN·m, kN·mlbf·ft, kip·ft
yDistance from neutral axism, mmin
ISecond moment of aream⁴in⁴
ZElastic section modulusin³
σBending normal stressPa, MPapsi, ksi
Worked example — rectangular beam under moment

Given: M = 12 kN·m; b = 100 mm, h = 200 mm; I = 6.667×10⁻⁵ m⁴.

σmax = 12000×0.100/(6.667×10⁻⁵) = 18.0 MPa
Answer: σmax = 18.0 MPa.

US check: ≈2.61 ksi.

Formula gives elastic stress, not code design strength.

Lateral-torsional buckling, local buckling, plasticity, residual stress and compactness are not represented by My/I alone.

04 // Beam transverse shear

The general elastic beam shear relation uses first moment of area Q. For a rectangle, the maximum shear stress is 1.5 times the average.

Core relation
τ = VQ/(It)
Rectangle: τmax = 3V/(2A)
SymbolMeaningSI unitsUS customary
VInternal shear forceNlbf
QFirst moment of area about neutral axisin³
ISecond moment of aream⁴in⁴
tLocal section thicknessmin
τShear stressPa, MPapsi, ksi
Worked example — rectangular section

Given: V = 40 kN; rectangular area A = 0.020 m².

τavg = V/A = 2.0 MPa
τmax = 1.5×2.0 = 3.0 MPa
Answer: τmax = 3.0 MPa.

US check: ≈0.435 ksi.

The maximum for a rectangle occurs at the neutral axis.

Thin-walled open/closed sections and shear flow may be better handled with q = VQ/I. Steel-code web shear strength is a separate design check.

05 // Common elastic beam deflections

Closed-form deflection equations depend on support and loading. These examples assume constant E and I and small deflection.

Core relation
Simply supported, center P: δmax = PL³/(48EI)
Simply supported UDL: δmax = 5wL⁴/(384EI)   ;   Cantilever tip P: δ = PL³/(3EI)
SymbolMeaningSI unitsUS customary
PPoint loadNlbf
wUniform line loadN/mlbf/ft
LSpanmft
EYoung’s modulusPapsi
ISecond moment of aream⁴in⁴
δElastic deflectionm, mmin
Worked example — center-loaded simple beam

Given: P = 10 kN, L = 4.0 m, E = 200 GPa, I = 6.667×10⁻⁵ m⁴.

δmax = 10000×4³/(48×200×10⁹×6.667×10⁻⁵)
δmax ≈ 0.00100 m = 1.00 mm
Answer: δmax ≈ 1.00 mm.

US check: ≈0.0394 in.

Serviceability limits are project/code dependent.

Shear deformation, variable stiffness, composite action, cracking, creep and second-order effects can make these formulas inadequate.

06 // Circular-shaft torsion

For Saint-Venant torsion of a circular shaft, shear stress varies linearly with radius and twist depends on GJ.

Core relation
τ = Tr/J
θ = TL/(GJ)
SymbolMeaningSI unitsUS customary
TTorqueN·mlbf·in
rRadius at evaluation pointmin
JPolar second momentm⁴in⁴
GShear modulusPapsi
LShaft lengthmin
θAngle of twistradrad or deg
Worked example — 50 mm solid shaft

Given: T = 500 N·m, d = 50 mm, L = 1.0 m, G = 79 GPa.

J = π(0.05)⁴/32 = 6.136×10⁻⁷ m⁴
τmax = T(d/2)/J = 20.37 MPa
θ = TL/(GJ) = 0.01031 rad = 0.591°
Answer: τmax ≈ 20.4 MPa; θ ≈ 0.591°.

US check: τmax ≈2.95 ksi.

Noncircular torsion requires different torsion constants and stress distributions.

Keys, splines, shoulders and notches create stress concentrations and are not included in this nominal shaft solution.

07 // Euler elastic column buckling

For an ideal slender column, Euler’s critical load depends on flexural rigidity and effective length.

Core relation
Pcr = π²EI/(KL)²
λ = KL/r   ;   r = √(I/A)
SymbolMeaningSI unitsUS customary
PcrEuler critical loadNlbf
KEffective length factordimensionlessdimensionless
LUnbraced/member lengthmft
rRadius of gyrationm, mmin
EYoung’s modulusPapsi
IBuckling-axis second momentm⁴in⁴
Worked example — pin-ended ideal column

Given: E = 200 GPa, I = 8.0×10⁻⁶ m⁴, L = 3.0 m, K = 1.0.

Pcr = π²×200×10⁹×8×10⁻⁶ / 3² = 1.755×10⁶ N
Answer: Pcr ≈ 1.75 MN.

US check: ≈394 kip.

Euler buckling is not a general column design equation.

Real columns have yielding, residual stress, imperfections, eccentricity, local buckling and frame interaction. Use the governing design code, e.g. AISC 360-22 for structural steel.

08 // Von Mises equivalent stress

For ductile isotropic materials, von Mises stress is a useful scalar measure of multiaxial deviatoric stress for yield screening.

Core relation
σvm = √(σₓ² − σₓσᵧ + σᵧ² + 3τₓᵧ²)
Uniaxial + torsion: σvm = √(σ² + 3τ²)
SymbolMeaningSI unitsUS customary
σx,σyNormal stressesMPaksi
τxyIn-plane shear stressMPaksi
σvmVon Mises equivalent stressMPaksi
Worked example — plane-stress combination

Given: σx = 100 MPa, σy = 40 MPa, τxy = 30 MPa.

σvm = √(100² − 100×40 + 40² + 3×30²)
σvm = 101.49 MPa
Answer: σvm ≈ 101.5 MPa.

US check: ≈14.72 ksi.

Von Mises is most appropriate for ductile isotropic yielding; it is not a universal failure criterion.

Brittle materials, composites, soils, concrete and anisotropic materials need failure criteria appropriate to their behavior.

09 // Quick formula summary

Compact print reference. Use the detailed sections above for definitions and limitations.

TopicEquationPurposeTool
Axialσ=P/A; δ=PL/AEAxial stress/deformationMaterial E
SectionI, Z, JGeometry/stiffnessBeam/column
Bendingσ=M/ZElastic flexureBeam/column
Shearτ=VQ/ItElastic transverse shearBeam/column
Deflectionδ=f(P,w,L,E,I)ServiceabilityBeam/column
Torsionτ=Tr/J; θ=TL/GJCircular shaftsStress
BucklingPcr=π²EI/(KL)²Ideal column instabilityBeam/column
Von MisesσvmDuctile yield screeningStress

10 // Assumptions & limitations

Fundamental equations are only useful when their assumptions match the actual problem.

11 // Technical references

AISC 360-22 is referenced for current structural-steel design context. The sheet intentionally stays with fundamental mechanics rather than reproducing code design equations without their applicability limits.

12 // Related EngineerHub tools