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Dynamic Response of Pillar Workings Induced by Sudden Pillar Recovery

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Abstract

When residual pillars are extracted in a short time in room and pillar mining, the load transferred from the removed pillar acts on neighbouring pillar workings in a dynamic manner. This study aims to investigate the instability of large mined-out areas triggered by dynamic disturbance resulting from residual pillar recovery. A mechanical model combining the pressure arch theory (PAT) based method and structural dynamics was first established to assess the stress state and deformation of a pillar subjected to combined effects of static and dynamic loads. The process of residual pillar recovery and potential induced instability of neighbouring pillar workings in a five-pillar system was further numerically simulated in both static and dynamic modes, and the response of adjacent pillars was investigated. It was found that the induced disturbance to a pillar can be characterised by the dynamic amplification coefficient R, the ratio of the increased vertical pillar load to the transferred load. Rmax can exceed 1.5 or even approach 2 in practical pillar recovery using the blasting method. Modelling results showed that while pillar workings adjacent to a removed pillar remain stable in static analysis, violent and large-scale pillar collapses can be triggered in the event of quick pillar recovery of blasting method. Results indicated that when the dynamic effect of pillar recovery is not considered, the load undertaken by adjacent pillar workings would be largely underestimated. To ensure mining safety, the induced dynamic effect should be accounted for in the design of the pillar recovery method.

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Abbreviations

DEM:

Discrete element method

PAT:

Pressure arch theory

D :

Fraction of critical damping

E :

Elastic modulus of a pillar

EA:

Excavated area

e :

Extraction ratio

g :

Gravitational acceleration

H :

Depth of pillars

K :

Elastic stiffness of a pillar

LTD:

Load transfer distance

m :

Mass of a pillar

R :

Dynamic amplification coefficient

r :

Pillar radius

T :

Natural vibration period of a pillar

t 0 :

Load transfer duration

U :

Total released energy in extraction

U d :

External energy from the dynamic disturbance

U f :

Energy needed to be consumed in fracturing rock masses

U s :

Strain energy stored in the rock mass to be extracted

w e :

Effective width for non-square pillars

y s :

Pillar deformation increment

ZI:

Area of zone of influence

α :

Damping coefficient

ρ :

Rock density

σ cri :

Critical stress

σ d :

Dynamic vertical pillar load

σ d :

Dynamic transferred vertical pillar load

\({\sigma _{{H_{\rm{max} }}}}\) :

The maximum horizontal principal stress

σ s :

Static (final) vertical pillar load

σ s :

Static (final) transferred vertical pillar load

σ V :

Vertical stress

σ v :

Vertical pillar load

\(\sigma _{{\text{v}}}^{{{\rm{max}}}}\) :

The maximum vertical pillar load

Ω:

Natural vibration frequency of a pillar

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Acknowledgements

This research is supported by financial grants from the National Basic Research Program of China (2015CB060200), the National Natural Science Foundation of China (No. 41772313) and the Hunan Natural Science Foundation (2015JJ4067). The authors are very grateful to the financial contribution and convey their appreciation of the organization for supporting this basic research.

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Correspondence to Wenzhuo Cao.

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Zhou, Z., Zhao, Y., Cao, W. et al. Dynamic Response of Pillar Workings Induced by Sudden Pillar Recovery. Rock Mech Rock Eng 51, 3075–3090 (2018). https://doi.org/10.1007/s00603-018-1505-2

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  • DOI: https://doi.org/10.1007/s00603-018-1505-2

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