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Cheatsheet: Structural Analysis Methods

1. Fundamental Equilibrium Methods

1.1 Static Equilibrium Equations

Equation Description
ΣFx = 0 Sum of horizontal forces equals zero
ΣFy = 0 Sum of vertical forces equals zero
ΣM = 0 Sum of moments about any point equals zero

1.2 Determinacy and Stability

Condition Criteria
Statically Determinate r = 3n where r = reactions, n = number of rigid bodies
Statically Indeterminate r > 3n; degree of indeterminacy = r - 3n
Unstable r < 3n="" or="" reactions="">

1.3 Support Reactions

Support Type Restraints/Reactions
Roller 1 reaction perpendicular to surface
Pin/Hinge 2 reactions (Rx, Ry)
Fixed 3 reactions (Rx, Ry, M)

2. Truss Analysis

2.1 Truss Determinacy

Parameter Formula
Member Equation m + r = 2j where m = members, r = reactions, j = joints
Statically Determinate m + r = 2j
Degree of Indeterminacy i = (m + r) - 2j

2.2 Method of Joints

  • Apply equilibrium at each joint: ΣFx = 0, ΣFy = 0
  • Begin at joint with ≤2 unknown forces
  • Tension: force pulls away from joint (positive)
  • Compression: force pushes toward joint (negative)
  • Zero-force members: unloaded joint with 2 non-collinear members

2.3 Method of Sections

  • Cut through ≤3 members to isolate section
  • Apply ΣFx = 0, ΣFy = 0, ΣM = 0 to free body
  • Take moments about points to eliminate unknowns
  • Useful for finding forces in specific members without analyzing entire truss

3. Beam Analysis

3.1 Shear and Moment Relationships

Relationship Equation
Load-Shear dV/dx = -w(x)
Shear-Moment dM/dx = V(x)
Load-Moment d²M/dx² = -w(x)
Change in Shear ΔV = -∫w(x)dx
Change in Moment ΔM = ∫V(x)dx = area under shear diagram

3.2 Sign Conventions

  • Positive shear: left side up, right side down
  • Negative shear: left side down, right side up
  • Positive moment: compression on top (sagging)
  • Negative moment: tension on top (hogging)

3.3 Key Diagram Properties

  • Maximum moment occurs where V = 0
  • Point load causes jump in shear diagram
  • Point load causes slope change in moment diagram
  • Distributed load causes linear variation in shear
  • Distributed load causes parabolic variation in moment
  • Concentrated moment causes jump in moment diagram only

3.4 Common Beam Formulas

Loading/Support Maximum Values
Simply supported, uniform load w Mmax = wL²/8 at midspan; Vmax = wL/2 at supports
Simply supported, center point load P Mmax = PL/4 at midspan; Vmax = P/2 at supports
Cantilever, uniform load w Mmax = wL²/2 at fixed end; Vmax = wL at fixed end
Cantilever, end point load P Mmax = PL at fixed end; Vmax = P at fixed end
Fixed-fixed, uniform load w Mmax = wL²/12 at supports; Mspan = wL²/24

4. Deflection Methods

4.1 Double Integration Method

Step Equation
Governing equation EI(d²y/dx²) = M(x)
First integration EI(dy/dx) = ∫M(x)dx + C₁ (slope equation)
Second integration EIy = ∫∫M(x)dx² + C₁x + C₂ (deflection equation)
  • Boundary conditions: y = 0 at supports, dy/dx = 0 at fixed ends
  • Solve for constants C₁ and C₂ using boundary conditions

4.2 Moment-Area Method

4.2.1 Theorems

Theorem Statement
First Theorem θB/A = (1/EI)∫M dx = area of M/EI diagram between A and B
Second Theorem tB/A = (1/EI)∫Mx dx = moment of M/EI diagram between A and B about B
  • θB/A = angle change from A to B
  • tB/A = vertical deviation of B from tangent at A
  • Use conjugate beam analogy: load = M/EI, shear = slope, moment = deflection

4.3 Conjugate Beam Method

  • Real beam load → Conjugate beam support reactions
  • Conjugate beam load = M/EI from real beam
  • Shear in conjugate beam = slope in real beam
  • Moment in conjugate beam = deflection in real beam
Real Beam Support Conjugate Beam Support
Fixed end Free end
Free end Fixed end
Pin/roller Pin/roller
Interior pin Interior hinge

4.4 Virtual Work/Unit Load Method

Application Formula
Beam deflection Δ = ∫(Mm/EI)dx where M = real moment, m = virtual moment
Truss deflection Δ = Σ(FfL/AE) where F = real force, f = virtual force
  • Apply unit load at location/direction of desired deflection
  • Calculate m or f from unit load
  • Calculate M or F from actual loads
  • Integrate or sum products

5. Influence Lines

5.1 Definition and Use

  • Shows variation of response (reaction, shear, moment) at specific point as unit load moves across structure
  • Used to determine critical load positions for maximum response
  • Ordinate = value of response when unit load is at that position

5.2 Müller-Breslau Principle

  • Remove restraint corresponding to desired response
  • Apply unit displacement in direction of response
  • Deflected shape is influence line (to scale)
  • Valid for statically determinate and indeterminate structures

5.3 Application for Maximum Response

  • Single concentrated load: place at maximum ordinate
  • Uniform distributed load: place over positive (or negative) region
  • Series of concentrated loads: use absolute maximum concepts
  • Maximum response = Σ(Pi × yi) where Pi = load, yi = influence ordinate

5.4 Common Influence Lines (Simply Supported Beam, Length L)

Response Maximum Ordinate
Reaction at A 1.0 at A, linear to 0 at B
Shear at x = a Jump from b/L to -a/L at x = a
Moment at x = a ab/L at x = a (triangular)

6. Indeterminate Structures - Force Method

6.1 Force Method Procedure

  1. Determine degree of indeterminacy (i)
  2. Select i redundant forces/moments
  3. Remove redundants to create determinate primary structure
  4. Apply actual loads to primary structure, find displacements at redundant locations
  5. Apply unit values of each redundant separately, find flexibility coefficients
  6. Solve compatibility equations: Δ = Δ₀ + f₁₁X₁ + f₁₂X₂ + ... = 0
  7. Superimpose to find final forces

6.2 Flexibility Coefficients

Term Definition
fij Displacement at i due to unit load at j
Maxwell's Law fij = fji (reciprocal deflections)

6.3 Compatibility Equations

  • For each redundant: total displacement = 0 (or known value)
  • Matrix form: [f]{X} = -{Δ₀} where [f] = flexibility matrix, {X} = redundants, {Δ₀} = primary structure displacements

7. Indeterminate Structures - Displacement Method

7.1 Slope-Deflection Equations

End Moment Equation
General form MAB = (2EI/L)(2θA + θB - 3ψ) + FMAB
MBA MBA = (2EI/L)(2θB + θA - 3ψ) + FMBA
  • θA, θB = rotations at A and B
  • ψ = (ΔB - ΔA)/L = chord rotation
  • FMAB, FMBA = fixed-end moments from applied loads
  • Apply equilibrium at each joint: ΣM = 0
  • Solve simultaneous equations for unknown rotations and deflections

7.2 Fixed-End Moments (FEM)

Loading FMAB / FMBA
Uniform load w FMAB = -wL²/12; FMBA = +wL²/12
Center point load P FMAB = -PL/8; FMBA = +PL/8
Point load P at distance a from A FMAB = -Pab²/L²; FMBA = +Pa²b/L²

7.3 Moment Distribution Method

7.3.1 Key Parameters

Term Formula
Stiffness K K = 4EI/L (far end fixed); K = 3EI/L (far end pinned)
Distribution Factor DF DFij = Kij / ΣKi (at joint i)
Carry-Over Factor COF COF = 1/2 (far end fixed); COF = 0 (far end pinned)

7.3.2 Procedure

  1. Calculate fixed-end moments for all loaded members
  2. Calculate stiffness factors K and distribution factors DF at each joint
  3. Lock all joints, apply loads to get FEMs
  4. Release one joint at a time, distribute unbalanced moment using DF
  5. Carry over half the distributed moments to far ends (COF = 0.5)
  6. Repeat until moments converge
  7. Sum moments at each end of each member

8. Matrix Structural Analysis

8.1 Direct Stiffness Method

8.1.1 Local Element Stiffness Matrix (2D Truss Element)

  • k' = (AE/L)[1 -1; -1 1] for axial member
  • Degrees of freedom: u1, u2 (axial displacements at nodes)

8.1.2 Coordinate Transformation

Parameter Expression
Transformation matrix T = [cos θ sin θ 0 0; 0 0 cos θ sin θ]
Global stiffness [K] = [T]ᵀ[k'][T]

8.1.3 Assembly and Solution

  1. Formulate element stiffness matrices in local coordinates
  2. Transform to global coordinates using transformation matrix
  3. Assemble global stiffness matrix [K] by adding overlapping terms
  4. Apply boundary conditions (eliminate rows/columns for restrained DOFs)
  5. Solve [K]{u} = {F} for unknown displacements
  6. Back-calculate element forces using {f} = [k'][T]{u}

8.2 Beam Element Stiffness (Local Coordinates)

DOFs Components
Per node v (transverse displacement), θ (rotation)
Total per element 4 DOFs (v1, θ1, v2, θ2)
  • Stiffness matrix k' is 4×4 symmetric
  • k'11 = k'22 = 12EI/L³; k'12 = k'21 = 6EI/L²
  • k'33 = k'44 = 4EI/L; k'34 = k'43 = 2EI/L

9. Approximate Analysis Methods

9.1 Portal Method (Frames)

  • Assumes inflection points at mid-height of columns
  • Assumes inflection points at mid-span of beams
  • Interior columns carry twice the shear of exterior columns
  • Total horizontal force distributed: Vext = V/n, Vint = 2V/n
  • Use for frames with height/width ratio > 2

9.2 Cantilever Method (Frames)

  • Assumes inflection points at mid-height of columns
  • Assumes inflection points at mid-span of beams
  • Axial forces in columns proportional to distance from centroid
  • ΣMc = 0 at each floor level to find axial forces
  • Use for frames with height/width ratio <>

9.3 Trusses with Loads at Panel Points

  • Assume chord members resist moments as axial force couples
  • Chord force F = M/h where M = moment, h = truss depth
  • Web members resist shear
  • Vertical web force = V / (number of verticals)

10. Special Topics

10.1 Cables

10.1.1 Parabolic Cable (Uniform Horizontal Load w)

Parameter Formula
Sag equation y = (wx²)/(2H) where H = horizontal tension
Maximum sag ymax = (wL²)/(8H) at midspan
Cable length s ≈ L[1 + (8/3)(ymax/L)²] for small sag
Maximum tension Tmax = √(H² + V²) at supports where V = wL/2

10.1.2 Catenary Cable (Uniform Load Along Cable)

  • Shape: y = (H/w)[cosh(wx/H) - 1]
  • For heavy cables, chains, or self-weight dominant

10.2 Three-Hinged Arches

  • Statically determinate (3 equations + 1 condition at crown hinge)
  • Horizontal thrust H reduces moment compared to beam
  • At crown hinge: moment = 0 provides additional equation
  • For symmetric arch with center load: H = PL/(4h)
  • For uniform load: H = wL²/(8h)

10.3 Composite Structures

  • Transform section using modular ratio n = E1/E2
  • Transformed width = actual width × n
  • Calculate properties of transformed section
  • Stress in material 1: σ1 = My/I
  • Stress in material 2: σ2 = nMy/I
The document Cheatsheet: Structural Analysis Methods is a part of the PE Exam Course Civil Engineering (PE Civil).
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