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Investigation of factors influencing the determination of ... - saimm

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An analytical solution to predict axial load along fully grouted bolts<br />

In <strong>the</strong> above equation, u r can be represented by an<br />

analytical function <strong>of</strong> <strong>the</strong> geometry <strong>of</strong> <strong>the</strong> tunnel and rock<br />

surface movement.<br />

where<br />

r o = tunnel radius.<br />

u ro is <strong>the</strong> total deformation <strong>of</strong> <strong>the</strong> excavation wall, and is<br />

written as9<br />

[7]<br />

[8]<br />

[9]<br />

[10]<br />

By dividing <strong>the</strong> bolting to n equal sections (Figure 2),<br />

and defining Δx′ = x′ - x′ = L , <strong>the</strong> expressions<br />

i+1 i ⁄(nr o )<br />

for <strong>the</strong> derivatives <strong>of</strong> u′ x′ at x′ = x′ are given as<br />

i<br />

or<br />

Equation [15] for i = 2, • • •, n can be written as;<br />

[16]<br />

[17]<br />

[18]<br />

T<br />

e<br />

c<br />

h<br />

n<br />

i<br />

c<br />

a<br />

l<br />

N<br />

o<br />

t<br />

e<br />

Parameters b, k, and f can be found from following<br />

Equations [9].<br />

[11]<br />

[12]<br />

These n-1 equations with two boundary conditions will<br />

form a tri-diagonal system <strong>of</strong> n + 1 linear algebraic equations<br />

with n + 1 unknowns, {u′ x′ (x′ i<br />

)}, thus we have<br />

[19]<br />

[13]<br />

where<br />

v = Poisson ratio <strong>of</strong> rock mass<br />

Po = in situ stress<br />

c = cohesion<br />

ϕ = friction angle<br />

r e = <strong>the</strong> boundary between <strong>the</strong> zone <strong>of</strong> plastic and elastic<br />

deformation<br />

By combining Equation [8] into Equation [7] and <strong>the</strong>n<br />

Equation [7] into Equation [6] and solving, <strong>the</strong> following<br />

numerical method has been developed. It is noted that <strong>the</strong><br />

numerical method was used as a powerful tool to solve <strong>the</strong><br />

developed analytical model.<br />

In this case <strong>the</strong> bolt was divided into equal parts, and<br />

<strong>the</strong>n <strong>the</strong> load distribution can be obtained by linking <strong>the</strong>se<br />

small sections toge<strong>the</strong>r. Thus to solve <strong>the</strong> reference equation<br />

(Equation [6]), dimensionless quantities are defined.<br />

A bolt under tension compresses <strong>the</strong> rock, which prevents<br />

bed separation and frictional forces developing between <strong>the</strong><br />

layers, but this does not mean that more tension creates<br />

better stability10. When a bolt is pre-tension loaded it would<br />

influence <strong>the</strong> shear strength <strong>of</strong> <strong>the</strong> joint with forces acting<br />

both perpendicular and parallel to <strong>the</strong> sheared joint by<br />

inducing confining pressure. A general rule for determining<br />

maximum pre-tension is that it should not exceed 60% <strong>of</strong> <strong>the</strong><br />

bolt yield strength or 60% <strong>of</strong> <strong>the</strong> anchorage capacity13. In this<br />

research <strong>the</strong> following two cases are examined;<br />

➤ Case 1—Bolt installed without face plate F x = 0 at x = 0<br />

and F x = 0 at x = L<br />

where<br />

Defining <strong>the</strong> normalized force F′ x = F x / (A b E b ), <strong>the</strong> above<br />

boundary conditions will be equivalent to:<br />

[20]<br />

[21]<br />

This can be written as;<br />

[14]<br />

Kr o<br />

2<br />

A b E b<br />

Kr o<br />

2,<br />

is a dimensionless quantity. By defining γ =<br />

Ab E b<br />

be written as,<br />

it can<br />

[15]<br />

Figure 2—Notation for numerical formulation<br />

The Journal <strong>of</strong> The Sou<strong>the</strong>rn African Institute <strong>of</strong> Mining and Metallurgy VOLUME 111 NOVEMBER 2011<br />

811<br />

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