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Table 3 Chord deformations of VATM by two-point Gauss quadrature.

From: Theoretical and Experimental Study of Effective Shear Stiffness of Reinforced ECC Columns

Member

Force

Unit load

Length

Rigidity

Deformation

F

f

l

EA

Ffl/EA

AB

cotα

cotα

x 1 L

\( E_{s} \left[ {\frac{{A_{st} }}{2} + \frac{{\gamma \left( {1 - \xi } \right)bh}}{n}} \right] \)

\( \frac{{x_{1} L\cot^{2} \alpha }}{{E_{s} \left[ {\frac{{A_{st} }}{2} + \frac{{\gamma \left( {1 - \xi } \right)bh}}{n}} \right]}} \)

BC

(2 − x 1)cotα/2

(2 − x 1)cotα/2

(1 − 2 x 1) L

\( E_{s} \left[ {\frac{{A_{st} }}{2} + \frac{{\gamma \left( {1 - \xi } \right)bh}}{n}} \right] \)

\( \frac{{L\cot^{2} \alpha \left( {1 - x_{1} } \right)^{2} \left( {1 - 2x_{1} } \right)}}{{4E_{s} \left[ {\frac{{A_{st} }}{2} + \frac{{\gamma \left( {1 - \xi } \right)bh}}{n}} \right]}} \)

CD

cotα/2

cotα/2

x 1 L

\( E_{s} \left[ {\frac{{A_{st} }}{2} + \frac{{\gamma \left( {1 - \xi } \right)bh}}{n}} \right] \)

\( \frac{{x_{1} L\cot^{2} \alpha }}{{4E_{s} \left[ {\frac{{A_{st} }}{2} + \frac{{\gamma \left( {1 - \xi } \right)bh}}{n}} \right]}} \)

EF

− cotα/2

− cotα/2

x 1 L

\( E_{s} \left( {\frac{{A_{st} }}{2} + \frac{\xi bh}{n}} \right) \)

\( \frac{{x_{1} L\cot^{2} \alpha }}{{4E_{s} \left( {\frac{{A_{st} }}{2} + \frac{\xi bh}{n}} \right)}} \)

FG

− x 1cotα/2

− x 1cotα/2

(1 − 2 x 1) L

\( E_{s} \left( {\frac{{A_{st} }}{2} + \frac{\xi bh}{n}} \right) \)

\( \frac{{x_{1}^{2} \left( {1 - 2x_{1} } \right)L\cot^{2} \alpha }}{{4E_{s} \left( {\frac{{A_{st} }}{2} + \frac{\xi bh}{n}} \right)}} \)

GH

0

0

x 1 L

\( E_{s} \left( {\frac{{A_{st} }}{2} + \frac{\xi bh}{n}} \right) \)

0

  1. Note x 1 = 0.21.