I. MOMENT DISTRIBUTION METHOD
A. Fundamental Concepts
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Distribution Factor (DF): Ratio of stiffness of a member to the sum of stiffnesses of all members meeting at a joint.
For a beam/column with far end fixed: stiffness = $$\displaystyle \frac{4EI}{L} $$; far end pinned: stiffness = $$\displaystyle \frac{3EI}{L} $$.
$$DF_{ij} = \frac{K_{ij}}{\sum K_{ij}}$$
where $$\displaystyle K_{ij} $$ is stiffness of member $i$ at joint $j$.
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Carry-Over Factor (COF): Fraction of moment carried over to the far end when a moment is applied at one end.
For prismatic member:
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Far end fixed → $$\displaystyle COF = 0.5 $$
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Far end pinned → $$\displaystyle COF = 0 $$
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Fixed-End Moments (FEM): Moments at ends of a member when both ends are fixed, due to external loads.
Key cases (span $L$, load $w$ or $P$):
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UDL: $$\displaystyle M_{AB} = \frac{wL^2}{12} $$, $$\displaystyle M_{BA} = -\frac{wL^2}{12} $$
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Point load at midspan: $$\displaystyle M_{AB} = \frac{PL}{8} $$, $$\displaystyle M_{BA} = -\frac{PL}{8} $$
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Temperature: $$\displaystyle M_{AB} = \frac{EI \alpha \Delta T}{L} $$ (symmetric), sign depends on heating/cooling.
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Sinking support: $$\displaystyle M_{AB} = -\frac{6EI \Delta}{L^2} $$, $$\displaystyle M_{BA} = \frac{6EI \Delta}{L^2} $$.
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Relative Stiffness: For members with uniform $EI$, stiffness $$\displaystyle \propto \frac{I}{L} $$.
For beams: $$\displaystyle K = \frac{I}{L} $$; for columns: $$\displaystyle K = \frac{I}{L} $$ (consider joint rotations).
[!TIP] When joint is rigidly connected, use $$\displaystyle \frac{4EI}{L} $$ for far-end fixed; if pinned, use $$\displaystyle \frac{3EI}{L} $$.
B. Application to Continuous Beams
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Procedure:
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Calculate DFs at each joint (except supports).
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Compute FEMs for all spans under given loads.
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Lock all joints (apply FEMs).
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Release joints one by one: apply unbalanced moment = -(sum of fixed-end moments + carried-over moments), distribute using DFs, carry over half to far ends.
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Repeat cycles until moments are negligible (typically < 1% of largest moment).
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Stopping Criteria: Iterate until the algebraic sum of moments at any joint is nearly zero.
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Drawing Diagrams:
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Bending Moment Diagram (BMD): Sum of FEMs + distributed moments + carry-overs at each section. Sketch on tension side.
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Shear Force Diagram (SFD): Compute from loads and support reactions (obtained from moment equilibrium).
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C. Application to Rigid Frames
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Frames with Sway: Lateral displacement causes additional moments. Two methods:
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Sway Correction: Analyze for non-sway loads first, then apply artificial joint rotations to eliminate sway, compute sway moments, and combine.
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Direct Analysis: Include column sidesway effects by treating frame as having an additional degree of freedom.
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Joints: Rigid joints distribute moments; pinned/roller supports have zero moment.
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Treatment of Supports: Fixed ends have no rotation; pinned ends have zero moment but rotation allowed.
D. Numerical Problems
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Symmetric Loading: Exploit symmetry to reduce calculations (half structure).
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Asymmetric Loading: Full analysis required.
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Different Stiffnesses: Use actual $EI/L$ values for DFs and COFs.
II. KANI'S METHOD (ROTATION INVERSION METHOD)
A. Basic Principles
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Based on rotation distribution and inversion of moments at joints.
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No separate carry-over step; inversion implicitly accounts for carry-over.
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Distribution factors are same as in moment distribution: $$\displaystyle DF = \frac{K_i}{\sum K} $$.
B. Procedure for Beams and Frames
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Calculate DFs at each joint.
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Start at one joint (usually leftmost), apply unbalanced moment (sum of FEMs) and distribute.
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Move to next joint: the distributed moment from previous joint becomes the "inverted" moment (opposite sign) at this joint, added to existing FEMs, then distribute.
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Continue until all joints processed; repeat cycles if needed.
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Final moments are the algebraic sum of all distributed moments at each joint end.
C. Comparison with Moment Distribution Method
| Aspect | Moment Distribution | Kani's Method |
|---|---|---|
| Carry-over | Explicit separate step | Implicit via inversion |
| Ease | Systematic, widely taught | Less common, faster for some frames |
| Convergence | Similar | Similar |
| When to use | General purpose, educational | Frames with many joints, quick estimates |
III. FLEXIBILITY METHOD (FORCE METHOD)
A. Introduction
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Redundant: Force (reaction or internal) removed to make structure statically determinate.
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Primary Structure: Statically determinate base structure.
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Degree of Indeterminacy: $$\displaystyle r = \text{number of redundants} $$ (static indeterminacy).
B. Flexibility Coefficients
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Definition: $$\displaystyle f_{ij} $$ = displacement at $i$ due to unit load at $j$.
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Calculation: Use unit load method:
$$f_{ij} = \int \frac{m_i m_j}{EI} dx$$
where $$\displaystyle m_i, m_j $$ are moments from unit loads.
- Muller Breslau Principle: To find $$\displaystyle f_{ij} $$, remove restraint at $i$, apply corresponding displacement (unit), the resulting deflected shape gives influence line for $$\displaystyle f_{ij} $$.
C. Compatibility Equations
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For each redundant $$\displaystyle X_k $$: $$\displaystyle \sum_{j=1}^{r} f_{kj} X_j + \Delta_k^0 = 0 $$
where $$\displaystyle \Delta_k^0 $$ is displacement at $k$ due to external loads (from primary structure).
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Solve simultaneous equations for $$\displaystyle X_j $$.
D. Application to Beams and Frames
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Selection of Redundants: Choose reactions or internal forces (e.g., moment at fixed end).
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Numerical Examples: Typically 1-2 redundants for continuous beams.
IV. STIFFNESS METHOD (DISPLACEMENT METHOD)
A. Introduction
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Degrees of Freedom (DOF): Independent displacements/rotations (e.g., joint rotations, translations).
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Unknowns: Usually joint displacements.
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Stiffness Coefficient $$\displaystyle k_{ij} $$: Force at $i$ due to unit displacement at $j$ (with others zero).
B. Formation of Equilibrium Equations
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Assemble global stiffness matrix $[K]$ from element stiffness matrices.
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Apply boundary conditions (modify $[K]$ and force vector $\{F\}$).
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Solve $$\displaystyle [K]\{D\} = \{F\} $$ for displacements $\{D\}$.
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Compute reactions from element stiffness equations.
C. Application to Beams and Frames
- Beam Elements: Local stiffness matrix (2 DOF per node: transverse displacement, rotation).
$$\begin{bmatrix} k_{11} & k_{12} \\ k_{21} & k_{22} \end{bmatrix} = \frac{EI}{L^3} \begin{bmatrix} 12 & 6L \\ 6L & 4L^2 \end{bmatrix}$$
(for far ends fixed).
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Frame Elements: Include axial effects; transform to global coordinates using transformation matrix.
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Assembly: Connect nodes, sum stiffness contributions.
D. Comparison with Flexibility Method
| Aspect | Flexibility Method | Stiffness Method |
|---|---|---|
| Unknowns | Redundant forces | Joint displacements |
| Matrix Size | $r \times r$ (small for low redundancy) | $n \times n$ (n = DOF) |
| Suitability | Low redundancy, supports settlements | High redundancy, computer-oriented |
| Advantage | Simple for few redundants | Systematic, suitable for programming |
V. PLASTIC ANALYSIS (ULTIMATE LOAD THEORY)
A. Fundamental Concepts
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Load Factor $\lambda$: Factor by which working load is multiplied to get ultimate load.
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Factor of Safety (FOS): $$\displaystyle \frac{\text{Ultimate load}}{\text{Working load}} $$ (in load factor form).
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Plastic Hinge: Zone where section yields fully, rotation occurs at constant moment $$\displaystyle M_p $$.
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Mechanism: Structure becomes kinematically unstable when enough plastic hinges form (for beam: $n+1$ hinges for $n$ spans).
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Theorems:
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Static Theorem: Any moment distribution satisfying equilibrium and $$\displaystyle M \leq M_p $$ gives upper bound collapse load.
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Kinematic Theorem: Collapse load from mechanism analysis is lower bound; true collapse load when both bounds coincide.
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B. Section Properties
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Plastic Modulus $$\displaystyle Z_p $$: $$\displaystyle Z_p = \frac{A}{2} (y_1 + y_2) $$ where $$\displaystyle y_1, y_2 $$ are distances from PNA to extreme fibers.
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Plastic Neutral Axis (PNA): Axis dividing section into equal areas (for symmetric sections, coincides with elastic NA).
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Shape Factor $$\displaystyle S_f = \frac{Z_p}{Z_e} $$; typical values:
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Rectangle: $$\displaystyle S_f = 1.5 $$
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I-section: $$\displaystyle S_f \approx 1.1 - 1.2 $$
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T-section: $$\displaystyle S_f \approx 1.2 - 1.4 $$
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Circle: $$\displaystyle S_f = \frac{16}{3\pi} \approx 1.697 $$
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C. Calculation for Standard Sections
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Rectangular ($b \times d$):
$$\displaystyle Z_e = \frac{bd^2}{6} $$, $$\displaystyle Z_p = \frac{bd^2}{4} $$, $$\displaystyle S_f = 1.5 $$.
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I-section: Sum of $$\displaystyle Z_p $$ for flanges and web.
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Circular (radius $R$):
$$\displaystyle Z_e = \frac{\pi R^3}{4} $$, $$\displaystyle Z_p = \frac{4R^3}{3} $$, $$\displaystyle S_f = \frac{16}{3\pi} \approx 1.697 $$.
D. Analysis of Beams for Collapse
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Mechanism Method:
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Assume plastic hinge locations (usually at maximum moment points: supports, midspan, point loads).
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Write geometry compatibility (relative rotations).
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Compute collapse load $$\displaystyle w_u $$ from virtual work: $$\displaystyle \sum M_p \theta = \sum P \delta $$.
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Propped Cantilever: Hinges at fixed end, propped support, and midspan (for UDL) → collapse load $$\displaystyle w_u = \frac{8M_p}{L^2} $$.
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Continuous Beams: Identify span hinges and possible hinge at interior supports; consider different mechanisms.
E. Plastic Design of Steel Beams
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Given ultimate load $$\displaystyle w_u $$, compute required $$\displaystyle M_p = \frac{w_u L^2}{8} $$ (simply supported) etc.
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Select I-section with $$\displaystyle Z_p \geq \frac{M_p}{f_y} $$.
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Check compactness per codal provisions.
VI. INFLUENCE LINES FOR INDETERMINATE STRUCTURES
A. Muller Breslau Principle
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Statement: The influence line for any reaction/force is the deflected shape of the structure when the corresponding restraint is removed and a unit displacement (rotation or translation) is applied.
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Procedure:
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Remove restraint corresponding to the function (e.g., for reaction, remove support).
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Apply corresponding unit displacement (e.g., vertical translation for reaction).
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Determine deflected shape = influence line.
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Note: For indeterminate structures, the deflected shape is not linear; requires analysis (often using moment distribution or flexibility).
B. Influence Lines for Indeterminate Beams
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Reaction: Remove support, apply vertical displacement, compute using slope-deflection or moment distribution.
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Shear Force: Cut section, apply vertical displacement discontinuity.
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Bending Moment: Cut section, apply rotation discontinuity.
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Effect of Supports: Fixed ends cause curved influence lines; pinned/roller supports may have kinks.
C. Influence Lines for Frames
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Consider joint rotations; use slope-deflection or moment distribution to compute ordinates.
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For moment at a joint: remove moment restraint, apply unit rotation.
D. Numerical Examples
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Double Overhanging Beam: Use moment distribution to find reactions, then IL for shear/moment at section.
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Continuous Beams: Apply Muller Breslau with fixed ends; use conjugate beam or moment distribution.
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Propped Cantilever: Fixed at one end, propped at other; IL for reaction at prop: remove prop, apply vertical displacement, solve as indeterminate.
VII. ANALYSIS OF FRAMES UNDER LATERAL LOADS
A. Wind and Earthquake Loads
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Characteristics: Dynamic, directionally variable, magnitude depends on height/terrain.
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Codal Provisions (BIS):
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Wind: IS 875 (Part 3) – basic wind speed, risk coefficient, terrain, height, structure factor.
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Earthquake: IS 1893 – seismic zone, importance factor, response spectrum, base shear.
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Equivalent Static Method:
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Base Shear $$\displaystyle V_b = A_h W $$, where $$\displaystyle A_h = \frac{Z I S_a}{R g} $$ (seismic) or from wind pressure.
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Distribute $$\displaystyle V_b $$ to floors: $$\displaystyle F_i = \frac{w_i h_i}{\sum w_j h_j} V_b $$.
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Dynamic Analysis: Response spectrum (for multiple DOF) or time history (advanced).
B. Sway Frames
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Moment Distribution / Stiffness Method: Include sidesway by introducing joint translations as unknowns or using sway correction.
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Portal Method (Approximate):
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Assumptions:
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Points of contraflexure at mid-height of columns.
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Shear distributed equally among columns on each floor.
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Moment at exterior column = 2/3 of total moment at that level; interior column = 1/3.
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Cantilever Method: For tall frames, assume frame acts as cantilever; shear distributed proportional to $I/h$ of columns.
C. Combined Gravity and Lateral Load Analysis
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Sequential Analysis:
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Analyze for gravity loads (dead + live) → obtain fixed-end moments.
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Analyze for lateral loads with gravity FEMs as fixed-end moments (no joint translations from gravity).
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P-Δ Effects: Secondary moments due to joint displacements under lateral load; significant for tall flexible frames; may require iterative analysis.
VIII. SECTION PROPERTIES AND DESIGN (RELATED TO PLASTIC ANALYSIS)
A. Elastic Section Modulus ($$\displaystyle Z_e $$)
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$$\displaystyle Z_e = \frac{I}{y_{\max}} $$, where $I$ is second moment of area, $$\displaystyle y_{\max} $$ distance to extreme fiber.
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For rectangle: $$\displaystyle Z_e = \frac{bd^2}{6} $$.
B. Plastic Section Modulus ($$\displaystyle Z_p $$)
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$$\displaystyle Z_p = \sum A_i y_i $$ for each half about PNA.
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For rectangle: $$\displaystyle Z_p = \frac{bd^2}{4} $$.
C. Shape Factor
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$$\displaystyle S_f = \frac{Z_p}{Z_e} $$; indicates extra moment capacity beyond elastic theory.
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[!TIP] Shape factor > 1 for most sections; circle has highest (~1.7).
D. Calculation for Circular Section (Radius $R$)
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Elastic Modulus: $$\displaystyle I = \frac{\pi R^4}{4} $$, $$\displaystyle y_{\max} = R $$ → $$\displaystyle Z_e = \frac{\pi R^3}{4} $$.
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Plastic Modulus: PNA through center.
$$Z_p = 2 \int_0^R y \cdot 2\sqrt{R^2 - y^2} dy = 4 \int_0^R y \sqrt{R^2 - y^2} dy$$
Let $$\displaystyle u = R^2 - y^2 $$, $$\displaystyle du = -2y dy $$:
$$\int y \sqrt{R^2 - y^2} dy = -\frac{1}{2} \int \sqrt{u} du = -\frac{1}{3} u^{3/2}$$
Evaluate $0$ to $R$: $$\displaystyle \frac{R^3}{3} $$. So $$\displaystyle Z_p = 4 \cdot \frac{R^3}{3} = \frac{4R^3}{3} $$.
- Shape Factor: $$\displaystyle S_f = \frac{4R^3/3}{\pi R^3/4} = \frac{16}{3\pi} \approx 1.697 $$.
IX. KEY DEFINITIONS (FROM EXAM PATTERN)
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Load Factor: Factor by which working loads are multiplied to obtain ultimate loads for plastic design. $$\displaystyle \boxed{\lambda = \frac{\text{Ultimate load}}{\text{Working load}}} $$.
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Plastic Modulus ($$\displaystyle Z_p $$): Geometric property of cross-section; sum of first moments of areas above and below PNA about PNA. $$\displaystyle \boxed{Z_p = \frac{A}{2}(y_1 + y_2)} $$.
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Plastic Neutral Axis (PNA): Axis that divides the cross-section into two equal areas under plastic moment.
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Relative Stiffness: Stiffness of a member relative to others at a joint, used in moment distribution. For beam/column: $$\displaystyle \frac{I}{L} $$ (or $$\displaystyle \frac{4EI}{L} $$ if far end fixed).
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Distribution Factor (DF): Fraction of unbalanced moment distributed to a member at a joint. $$\displaystyle \boxed{DF_i = \frac{K_i}{\sum K}} $$.
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Factor of Safety (FOS): Ratio of ultimate strength to allowable stress. In plastic design, often incorporated via load factor. $$\displaystyle \boxed{FOS = \frac{f_u}{f_{\text{allow}}}} $$.
[!TIP] In exams, clearly define each term with formula where applicable. For plastic modulus and PNA, include a simple sketch of section showing PNA and areas.