Journal of Structural and Construction Engineering (Transactions of AIJ)
Online ISSN : 1881-8153
Print ISSN : 1340-4202
ISSN-L : 1340-4202
EVALUATION OF PΔ EFFECT FOR SYMMETRICAL BRACED FRAMES
Masae KIDOKeigo TSUDA
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2020 Volume 85 Issue 771 Pages 771-778

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Abstract

1. Introduction

 The objective of this study is to examine the amplification factor of moment and rotation angle due to the PΔ effect for symmetrical braced frames. A sub-assemblage frame is analyzed by using the buckling slope deflection method, and amplification factors are obtained. An approximate formula for estimating the amplification factors is presented.

2. Analytical work

 The sub-assemblage frame shown in Fig. 2 is analysed, taking the geometric nonlinear effect into consideration. It is assumed that the slope θA= θA1 = θA2 and θB= θB1 = θB2 and the beam moments of node A and B are distributed to upper and lower column according to the column stiffness. Equation (6) is obtained by the fundamental formula of buckling slope deflection method. Moment equation at point A and B becomes Eqs. (10) and (13), respectively, where GA and GB are G factors defined as Eqs. (12) and (14). From the story equation (Eq. (15)) together with moment equations, the rotation angle R of the member AB and the moment MAB and MBA of node A and B are obtained as Eqs. (16), (17) and (18). In absence of axial force P, the rotation angle R and the moment MAB and MBA become Eqs. (20), (21) and (22), and then the amplification factors are obtained by Eqs. (23), (24) and (25).

3. Results and discussions

 As the analytical parameters, G factors GA(=GB), slenderness ratios γ axial load ratios ny and non-dimensional horizontal stiffness k* are selected, and they vary as follows: G factors GA(=GB) : 0 (rigid beams), 0.5, 1, 2.5 and 5, slenderness ratio γ: 20, 40 and 80, axial load ratio ny: 0.1, 0.3, 0.5, 0.7, non-dimensional horizontal stiffness k*: 0, 1, 5. Figure 5 shows R/0R-Z relations and M/0M-Z relations. The dotted lines and solid lines show the R/0R-Z relations and M/0M-Z relations, respectively. A similar tendency is observed between R/0R and M/0M. Figure 6 and 7 show the effect of axial load ratio ny and G factors. From Fig. 6, it is shown that the ratios R/0R and M/0M become large as the axial load ratio increases. Approximate effective length factor Kdsn has been proposed by Eq. (27), and using this, the amplification factors am can be obtained by Eq. (31). In Fig. 5, 6 and 7, white circles indicate the results obtained using Eq. (31). The values of am agree well with the R/0R and M/0M, and the relative error is shown in Fig. 8. While the error increases as the value Z becomes large, the am fits with an error of 2% or less when Z is smaller than 1. Figure 9 shows the limit Zα where the amplification factors is guaranteed below the value of α=1.05.

4. Conclusions

 The conclusions derived from this study are as follows:

 1) The amplification factors of the moments and rotation angle are presented by Eqs. (23) - (25). The governing parameters are G factors, Z and k* defined in Eqs. (12), (14), (9) and (5).

 2) The amplification factors can be approximately calculated by using Eq. (31).

 3) The limit value of Z to assure the restriction of the amplification factors is proposed by Eq. (35).

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© 2020 Architectural Institute of Japan
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