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Chapter 10: Analysis of Statically Indeterminate Structures by the Force Method. CIVL3310 STRUCTURAL ANALYSIS. Professor CC Chang. Determinate or Indeterminate ?. Determinate. Equilibrium. Indeterminate. Yes. Structure. No. Why Indetermiante ?. Advantages.
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Chapter 10: Analysis of Statically Indeterminate Structures by the Force Method CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang
Determinate or Indeterminate ? Determinate Equilibrium Indeterminate Yes Structure No
Why Indetermiante ? • Advantages Smaller stresses and deflections
Why Indetermiante ? • Advantages Fail safe 1995 Oklahoma City bombing
Prices • Disadvantages Stresses due to support settlement
Prices • Disadvantages Stresses due to temperature changes
Symmetric Structures Axis of symmetry Structure Reflection Identical in geometry, supports and material properties
Decomposition of Loadings sum (A) (B) = (A)/2 (C) = Reflection of (B) (B)+(C) Symmetrical (B)-(C) Anti-symmetrical
Decomposition of Loadings + = • Loadings = Symmetrical + Anti-symmetric Loads
Analysis of Symmetrical Structures Loading Symmetrical Loading Anti-symmetrical Loading Symmetrical Structure Response Response 1 Response 2 +
Symmetrical Structures under Symmetrical Loads a a P P L P Moment & vertical displacement ≠ 0 Slope & axial displacement = 0 slope = 0 M ≠ 0 V ≠ 0
Symmetrical Structures under Anti-symmetrical Loads a a Slope ≠ 0 Moment & vertical displacement = 0 P L/2 L/2 P P Slope ≠ 0 M = 0 V = 0
Analysis 6 degrees of indeterminacy 4 degrees of indeterminacy 4 degrees of indeterminacy
Analysis of Statically Indeterminate Structures • Force methods • This chapter • Displacement methods • Next two chapters
Compatibility DB=0 By
Compatibility P P 1 1 C C D D = A B +
Compatibility • Settlement
Compatibility • Settlement
Least Work Method D=? P F M(P,F) U(P,F) • Castigliano’s theory P D
Least Work Method DF F M(P,F) U(P,F) P Obtain F
Least Work Method F DP M(P,F) Castigliano’s theorem Least work principle • Virtual work principle +dP P +dF Note: F does not do any work !
Least Work Method P1 Pm P2 Fn F2 F1 Strain energy Forces that do work Forces that do not do work