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International Journal of Architectural Heritage
Conservation, Analysis, and Restoration
Volume 17, 2023 - Issue 10
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Research Article

Rotational Performance of Traditional Straight Mortise-Tenon Joints with Gap: Theoretical Model and Numerical Analyses

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Pages 1701-1718 | Received 14 Feb 2022, Accepted 19 Apr 2022, Published online: 03 Jun 2022
 

ABSTRACT

Gaps are very common in the mortise-tenon (M-T) joints of traditional timber structures. To investigate the rotational behavior of straight M-T joints with gaps, the mechanical mechanism and contact states between the mortise and tenon for the straight M-T joints with gaps were analyzed. A moment-rotation theoretical model of straight M-T joint with gap, based on the embedded compressive and friction mechanisms of the contact surfaces, was proposed and verified by the cyclic loading tests of four 1/3.2-scaled straight M-T joint specimens with different gaps. To further predict the deformation modes and hysteretic behavior of the joint involving gap, nonlinear numerical analyses were performed using ABAQUS. Results indicated that the predictions of theoretical and numerical model were in good accordance with the experimental results. Then, the parametric analyses were carried out based on the validated finite element model, the effects on the rotational behavior of straight M-T joint of major parameters, such as the friction coefficient of wood, vertical gaps, and horizontal gaps, were analyzed. It is found that the initial rotational stiffness, yielding moment, peak moment, and ductility of the joint with gap increased with an increase in the friction coefficient. The initial rotational stiffness, yielding moment, and peak moment of the joint remarkably decreased with the increase of the vertical and horizontal gap. The ductility of joint significantly reduced with the increasing vertical gap, however, the joint slightly improved with an increase in the horizontal gap.

Disclosure statement

No potential conflict of interest was reported by the author(s).

Nomenclature

M-T=

Mortise-tenon

M - θ=

Moment-rotation

μ=

The friction coefficient

ε=

The strain of wood

fc,90=

The yield strength perpendicular to the grain of wood

εcu=

The ultimate strain perpendicular to the fiber direction of wood

xb=

The EC zone heights of the contact area II of the joint with gap

lb=

The lengths of the EC area II

bT=

The width of the tenon

=

The height of the tenon

bM=

The width of the mortise

L=

The diagonal line length of the tenon

θ=

The rotation of the joint

F1=

The compression force of the EC area I of the tenon

f1=

The friction force of the EC area I

ε1,max=

The maximum strain in the EC area I of the tenon

he=

Half the tenon height

θ0=

The slipping rotation

F2,e=

The compression force in the area II under the elastic state

d=

The distance from the loading point of the beam to the column surface

F2,p=

The compression force at EC zone II under elasto-plastic state

lp,II=

the plastic segment length of the EC area II

F1,p=

The compression force of EC area I

le,I=

The length of the elastic segment for the EC area I

le,II=

The length of the elastic segment in the EC zone II

Mp=

The bending moment of the straight M-T joint with gap under the plastic state

θy,I=

The rotation at which the EC zone I begins to get into the plastic state

DG=

The damage degree

δH=

The size of horizontal gap

MTG=

The M-T joint specimen with gaps

C3D8R=

The 3-D linear reduced integration solid element

EC=

Embedded compression

FE=

Finite element

σ=

The stress strength of wood

Ec,90=

The compressive elastic modulus perpendicular to the grain of wood

εcy=

The compressive yield strain perpendicular to the fiber direction of wood

xa=

The EC zone heights of the contact area I of the joint with gap

la=

The length of the EC area I

δ=

The height of the tenon being weakened

lT=

The length of the tenon

hM=

The height of the mortise

dC=

The diameter of the column

φ=

The angle between the diagonal line and the upper surface of the tenon

F=

The external load

F2=

The compression force of the EC area II of the tenon

f2=

The friction force of the EC area II

ε2,max=

The maximum strain in the EC area II of the tenon

Ms=

The bending moment of the joint in the slipping state

F1,e=

The compression force in the area I under the elastic state

Me=

The bending moment for the straight M-T joint with gap in the elastic contact state

F1,e=

The compression force at EC zone I under elasto-plastic state

le,II=

The elastic segment length of the EC area II

Mep=

The bending moment for the straight M-T joint with gap in the elasto-plastic state

F2,p=

The compression force of EC area II

lp,I=

The length of the plastic segment for the EC area I

lp,II=

The length of the plastic segment in the EC zone II

θy,II=

The rotation at which the EC area II starts to enter the plastic state

θu=

The ultimate rotation

Δu=

The referenced ultimate displacement

MT0=

The intact M-T joint specimen

3-D=

Three-dimensional

Additional information

Funding

The authors of this paper appreciatively acknowledge the funding support received from the National Natural Science Foundation of China (Grant No. 52178303),the Foundation Research Project of Shaanxi Province (Grant No. 2021 JC-44) and the Key Project of Collaborative Innovation Center of Shaanxi Provincial Department of Education (Grant No. 21JY026).

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