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Design Considerations for Bored Tunnels at Close Proximity<br />

Dazhi Wen, John Poh, Yang Wah Ng<br />

Land Transport Authority, S<strong>in</strong>gapore<br />

ABSTRACT<br />

In <strong>the</strong> various stages of <strong>the</strong> Circle L<strong>in</strong>e (CCL) <strong>in</strong> S<strong>in</strong>gapore, civil eng<strong>in</strong>eers constantly face <strong>the</strong><br />

challenge to achieve <strong>the</strong> optimum alignment through heavily built-up areas. Both construction risks<br />

and site constra<strong>in</strong>ts have to be taken <strong>in</strong>to account when select<strong>in</strong>g <strong>the</strong> alignment. In CCL Stage 3, <strong>the</strong><br />

tw<strong>in</strong> bored tunnels are aligned with a m<strong>in</strong>imum separation of 2.3m <strong>in</strong> order to avoid tunnell<strong>in</strong>g directly<br />

under build<strong>in</strong>gs. This paper describes <strong>in</strong> detail <strong>the</strong> design considerations for <strong>the</strong> pre-cast re<strong>in</strong>forced<br />

concrete segmental l<strong>in</strong><strong>in</strong>g for <strong>the</strong> bored tunnels of CCL Stage 3. The effect of <strong>the</strong> second tunnel<br />

construction on <strong>the</strong> first tunnel is exam<strong>in</strong>ed. The methodology for evaluat<strong>in</strong>g <strong>the</strong> additional load<strong>in</strong>g on<br />

<strong>the</strong> first tunnel l<strong>in</strong><strong>in</strong>g due to <strong>the</strong> second tunnel construction is also presented<br />

1. INTRODUCTION<br />

The proposed Circle L<strong>in</strong>e Stage 3 (CCL3) is a medium capacity rail system. It cont<strong>in</strong>ues from Circle<br />

L<strong>in</strong>e Stage 2 network from Bartley station. After leav<strong>in</strong>g Bartley station <strong>the</strong> tunnels pass under an area<br />

of private residential houses at Lorong Gambir and St. Gabriel’s Secondary School before enter<strong>in</strong>g <strong>the</strong><br />

Serangoon public hous<strong>in</strong>g estates and Serangoon Station. The tunnels cont<strong>in</strong>ue to travel under<br />

Serangoon area and <strong>the</strong>n enter Lorong Chuan station, after which <strong>the</strong>y pass under <strong>the</strong> CTE and arrive<br />

at <strong>the</strong> Bishan station. Leav<strong>in</strong>g Bishan station, <strong>the</strong> tunnels will be under <strong>the</strong> private residential area of<br />

Jalan B<strong>in</strong>chang and Pemimp<strong>in</strong> Drive before reach<strong>in</strong>g <strong>the</strong> last station of CCL3 at Marymount station.<br />

Altoge<strong>the</strong>r <strong>the</strong>re are five underground stations connected by tunnels. The total length is approximately<br />

5.7km. In order to avoid underp<strong>in</strong>n<strong>in</strong>g of <strong>the</strong> residential houses and high-rise residential flats, <strong>the</strong> tw<strong>in</strong><br />

bored tunnels have to be aligned at very close distance of less than one tunnel diameter. The tunnels at<br />

Lorong Gambir are <strong>the</strong> closest with a m<strong>in</strong>imum clearance of 2.3m, see Figure 1.<br />

Serangoon Ave. 1<br />

St. Gambriel’s<br />

Secondary<br />

School<br />

M<strong>in</strong>imum clearance<br />

between tunnels: 2.3m<br />

Gambir Walk<br />

To Serangoon station<br />

Figure 1. Tunnels at Lorong Gambir<br />

F19 1


Figure 2 shows <strong>the</strong> general arrangement of <strong>the</strong> segments. The pre-cast re<strong>in</strong>forced concrete segmental<br />

l<strong>in</strong><strong>in</strong>gs are designed by <strong>the</strong> LTA <strong>in</strong>-house team. The <strong>in</strong>ternal diameter of <strong>the</strong> tunnels is 5.8 metres<br />

def<strong>in</strong>ed by space requirements. The thickness of <strong>the</strong> l<strong>in</strong><strong>in</strong>g is designed to be 275mm. A segment length<br />

of 1.4m is adopted. Each r<strong>in</strong>g consists of five ord<strong>in</strong>ary segments plus a key segment. Curved bolts are<br />

designed for both <strong>the</strong> radial and circumferential jo<strong>in</strong>ts. A composite hydrophilic and elastomeric<br />

gasket is specified on <strong>the</strong> draw<strong>in</strong>g. The r<strong>in</strong>gs have a maximum taper of 40mm. The radial jo<strong>in</strong>ts are<br />

convex to convex jo<strong>in</strong>ts. This type of jo<strong>in</strong>ts allows some articulation to take place. Because <strong>the</strong> radial<br />

jo<strong>in</strong>ts are staggered from r<strong>in</strong>g to r<strong>in</strong>g, <strong>the</strong> l<strong>in</strong><strong>in</strong>g is considered <strong>in</strong> <strong>the</strong> normal load comb<strong>in</strong>ations as a<br />

cont<strong>in</strong>uous r<strong>in</strong>g. The circumferential jo<strong>in</strong>ts are flat jo<strong>in</strong>ts.<br />

Figure 2. General arrangement of tunnel segments<br />

The concrete for <strong>the</strong> segments is specified to be grade 60 concrete with a 28-day compressive strength<br />

of 60 N/mm 2 . Silica fume is required <strong>in</strong> <strong>the</strong> concrete mix under <strong>the</strong> contract to reduce <strong>the</strong> permeability<br />

and <strong>the</strong> chlorite diffusion rate of <strong>the</strong> segments. The extrados of <strong>the</strong> segments is also required to be<br />

coated with epoxy.<br />

2. DESIGN OF REINFORCED CONCRETE SEGMENTAL LINING<br />

2.1 Design concept<br />

It has been well established that tunnel l<strong>in</strong><strong>in</strong>g <strong>in</strong> soft ground will redistribute <strong>the</strong> ground load<strong>in</strong>g. The<br />

ground load<strong>in</strong>g act<strong>in</strong>g on a circular tunnel l<strong>in</strong><strong>in</strong>g can be divided <strong>in</strong>to two components: <strong>the</strong> uniform<br />

distributed radial component and <strong>the</strong> distortional component. The uniform distributed radial<br />

component will only produce hoop thrust and <strong>the</strong> l<strong>in</strong><strong>in</strong>g will deform <strong>in</strong> <strong>the</strong> radial direction with <strong>the</strong><br />

shape of <strong>the</strong> r<strong>in</strong>g rema<strong>in</strong><strong>in</strong>g circular. The distortional component will produce bend<strong>in</strong>g moments <strong>in</strong> <strong>the</strong><br />

l<strong>in</strong><strong>in</strong>g, and <strong>the</strong> crown and <strong>in</strong>vert will be squatted (move <strong>in</strong>wards) and at <strong>the</strong> axial level <strong>the</strong> l<strong>in</strong><strong>in</strong>g will<br />

move outwards, Figure 3. The soil pressure at <strong>the</strong> crown and <strong>in</strong>vert will be reduced as a result of <strong>the</strong><br />

<strong>in</strong>ward movement and <strong>the</strong> soil pressure at <strong>the</strong> axial level will be <strong>in</strong>creased due to <strong>the</strong> outward<br />

movement of <strong>the</strong> l<strong>in</strong><strong>in</strong>g. The redistribution of ground pressure around <strong>the</strong> r<strong>in</strong>g and <strong>the</strong> l<strong>in</strong><strong>in</strong>g<br />

de<strong>format</strong>ion will cont<strong>in</strong>ue until a balance is achieved. The stability of <strong>the</strong> tunnel l<strong>in</strong>ed by concrete<br />

segments thus depends on a cont<strong>in</strong>uous support / pressure around r<strong>in</strong>g. Any cavity <strong>in</strong> <strong>the</strong> space<br />

between <strong>the</strong> tunnel l<strong>in</strong><strong>in</strong>g and <strong>the</strong> ground will result <strong>in</strong> excessive distortional load<strong>in</strong>g on <strong>the</strong> l<strong>in</strong><strong>in</strong>g and<br />

may subject <strong>the</strong> r<strong>in</strong>g to undergo excessive distortion, caus<strong>in</strong>g unacceptable crack<strong>in</strong>g of <strong>the</strong> segments.<br />

F19 2


Deformed r<strong>in</strong>g<br />

Deformed<br />

r<strong>in</strong>g<br />

Figure 3. Tunnel l<strong>in</strong><strong>in</strong>g subjected to uniform distributed load<strong>in</strong>g and distortional load<strong>in</strong>g<br />

Various design methods are available for segmental l<strong>in</strong><strong>in</strong>g design. The Design Criteria of <strong>the</strong> Land<br />

Transport Authority (LTA) of S<strong>in</strong>gapore accept <strong>the</strong> methods of cont<strong>in</strong>uum model by Muir Wood<br />

(1975) modified by Curtis (1976), bedded beam model by Duddeck et al (1982) or <strong>the</strong> f<strong>in</strong>ite element<br />

method. The l<strong>in</strong><strong>in</strong>g for <strong>the</strong> CCL3 bored tunnel is designed us<strong>in</strong>g <strong>the</strong> cont<strong>in</strong>uum model. The method<br />

assumes that <strong>the</strong> l<strong>in</strong><strong>in</strong>g deforms <strong>in</strong> an elliptical shape and <strong>the</strong> ground is an elastic cont<strong>in</strong>uum. The hoop<br />

thrust and moment <strong>in</strong>duced by <strong>the</strong> soil-structure <strong>in</strong>teraction are evaluated accord<strong>in</strong>gly.<br />

2.2 Design analyses<br />

The tunnels are to be constructed through soft ground with a tunnel bor<strong>in</strong>g mach<strong>in</strong>e (TBM). The<br />

vertical pressure applied to <strong>the</strong> l<strong>in</strong><strong>in</strong>g is thus <strong>the</strong> full overburden pressure. Distortional load<strong>in</strong>g is<br />

derived by us<strong>in</strong>g <strong>the</strong> appropriate K-factor <strong>in</strong> Curtis formulae accord<strong>in</strong>g to <strong>the</strong> soil condition at <strong>the</strong><br />

tunnel location. The follow<strong>in</strong>g K-factors are used <strong>in</strong> accordance with <strong>the</strong> LTA Design Criteria:<br />

Table 1. K-factor<br />

Soil Type<br />

K<br />

Estuar<strong>in</strong>e, Mar<strong>in</strong>e and Fluvial Clays 0.75<br />

Beach Sands, Old Alluvium, Completely Wea<strong>the</strong>red Granite, Fluvial Sands 0.5<br />

Completely Wea<strong>the</strong>red Sedimentary Rocks 0.4<br />

Moderately to Highly Wea<strong>the</strong>red Sedimentary or Granite Rocks 0.3<br />

A uniform surcharge of 75 kN/m 2 is considered <strong>in</strong> <strong>the</strong> design. The design ground water table is taken<br />

at both <strong>the</strong> ground surface (upper limit) and 3m (lower limit) below <strong>the</strong> surface.<br />

The design assumes that <strong>the</strong> segments <strong>in</strong> <strong>the</strong> permanent condition are short columns subject to<br />

comb<strong>in</strong>ed hoop thrust and bend<strong>in</strong>g moment. Both ultimate limit state (ULS) and serviceability limit<br />

state (SLS) are checked. Ultimate limit state design ensures that <strong>the</strong> load bear<strong>in</strong>g capacity of <strong>the</strong> l<strong>in</strong><strong>in</strong>g<br />

is not exceeded while serviceability limit state design checks both <strong>the</strong> crack-width and de<strong>format</strong>ion of<br />

<strong>the</strong> l<strong>in</strong><strong>in</strong>g. The follow<strong>in</strong>g factors are used <strong>in</strong> <strong>the</strong> limit state design:<br />

• Ultimate limit state: Load factor for overburden and water pressure = 1.4<br />

Load factor for surcharge = 1.6<br />

F19 3


• Serviceability limit state: Load factor for overburden, surcharge and water pressure = 1.0<br />

The overburden, surcharge and water pressure are assumed as loads on <strong>the</strong> tunnel, and <strong>the</strong> effects of<br />

ground arch<strong>in</strong>g around <strong>the</strong> tunnel are neglected for tunnels <strong>in</strong> soft ground. For re<strong>in</strong>forcement design<br />

for both <strong>the</strong> ULS and SLS, <strong>the</strong> thrust and moment are obta<strong>in</strong>ed assum<strong>in</strong>g a cont<strong>in</strong>uous l<strong>in</strong><strong>in</strong>g with full<br />

section moment of <strong>in</strong>ertia and short-term Young's modulus for <strong>the</strong> concrete. This is to obta<strong>in</strong> <strong>the</strong><br />

maximum moment <strong>in</strong> <strong>the</strong> r<strong>in</strong>g. For deflection check<strong>in</strong>g <strong>the</strong> Young's modulus of <strong>the</strong> concrete is<br />

reduced by 50% to account for concrete creep. The moment of <strong>in</strong>ertia of <strong>the</strong> segment is also reduced<br />

based on <strong>the</strong> recommendation by Muir Wood (1975) that:<br />

I = I j +I f (4/n) 2<br />

where I j is <strong>the</strong> moment of <strong>in</strong>ertia of <strong>the</strong> jo<strong>in</strong>t (I j = 0), n is <strong>the</strong> total number of segments <strong>in</strong> a r<strong>in</strong>g and I f<br />

is <strong>the</strong> full moment of <strong>in</strong>ertia before reduction. This is to obta<strong>in</strong> <strong>the</strong> maximum deflection <strong>in</strong> <strong>the</strong> r<strong>in</strong>g.<br />

The design analyses have been carried out for sections where <strong>the</strong> tunnels are expected to experience a<br />

maximum and m<strong>in</strong>imum overburden pressure and where <strong>the</strong> tunnels transverses different soil strata.<br />

The load comb<strong>in</strong>ations are listed <strong>in</strong> Table 2.<br />

Table 2. Load comb<strong>in</strong>ations<br />

LOAD<br />

COMBINATIONS<br />

Load Factor = 1.4<br />

and 1.6<br />

ULS<br />

SLS<br />

(crack width)<br />

SLS<br />

(deflection)<br />

1 2 3 4 5 6 7 8 9 10 11 12<br />

√ √ √ √ √<br />

Load Factor = 1.0 √ √ √ √ √ √ √<br />

75kN/m 2 Uniform<br />

Surcharge<br />

Water Table at<br />

Ground Surface<br />

Water Table 3m<br />

Below Ground<br />

Surface<br />

<strong>Full</strong> Section Moment<br />

of Inertia<br />

Reduced Section<br />

Moment of Inertia<br />

Short Term Concrete<br />

Young's Modulus<br />

Long Term Concrete<br />

Young's Modulus<br />

Additional Distortion<br />

of 15mm on<br />

Diameter<br />

√ √ √ √ √ √ √ √<br />

√ √ √ √ √<br />

√ √ √ √ √ √ √<br />

√ √ √ √ √ √ √ √<br />

√ √ √ √<br />

√ √ √ √ √ √ √ √<br />

√ √ √ √<br />

√<br />

√<br />

F19 4


2.3 Effect of <strong>the</strong> second tunnel construction on <strong>the</strong> first tunnel<br />

Typically for tw<strong>in</strong> bored tunnels, <strong>the</strong> second tunnel drive will be some distance beh<strong>in</strong>d <strong>the</strong> first tunnel<br />

drive. If <strong>the</strong>re is adequate clearance between <strong>the</strong> two tunnels, <strong>the</strong> effect of <strong>the</strong> second tunnel<br />

construction on <strong>the</strong> erected segmental l<strong>in</strong><strong>in</strong>g of <strong>the</strong> first tunnel is negligible. The rule of thumb is that<br />

<strong>the</strong> clearance between <strong>the</strong> two tunnels should not be less than one tunnel diameter. If <strong>the</strong> clearance<br />

between <strong>the</strong> tunnels is less than one tunnel diameter, <strong>the</strong> design should make allowance <strong>in</strong> <strong>the</strong> l<strong>in</strong><strong>in</strong>g of<br />

<strong>the</strong> first tunnel for <strong>the</strong> effect of <strong>the</strong> second tunnel construction.<br />

Ground movement due to <strong>the</strong> second tunnel construction will cause additional movements to <strong>the</strong> first<br />

tunnel besides that due to <strong>the</strong> ground load<strong>in</strong>g. The additional movements will result <strong>in</strong> additional<br />

distortion, which is <strong>the</strong> difference of <strong>the</strong> movements of <strong>the</strong> first tunnel at two diametrically opposite<br />

po<strong>in</strong>ts, such as at po<strong>in</strong>ts a and b, where po<strong>in</strong>t a is closest to and po<strong>in</strong>t b is <strong>the</strong> fur<strong>the</strong>st from <strong>the</strong> second<br />

tunnel, see Figure 4. Correspond<strong>in</strong>gly <strong>the</strong>re will also be an additional distortion between <strong>the</strong> crown<br />

and <strong>in</strong>vert of <strong>the</strong> tunnel. For design purpose, it is necessary to establish <strong>the</strong> maximum additional<br />

distortion to compute <strong>the</strong> maximum additional moment that <strong>the</strong> l<strong>in</strong><strong>in</strong>g will be subjected to. The<br />

maximum distortion will take place across <strong>the</strong> diameter along <strong>the</strong> l<strong>in</strong>e connected by <strong>the</strong> centres of <strong>the</strong><br />

two tunnels, i.e. po<strong>in</strong>ts a and b <strong>in</strong> Figure 4. This maximum distortion can be calculated based on <strong>the</strong><br />

<strong>the</strong>ory of elasticity by us<strong>in</strong>g <strong>the</strong> volume loss due to <strong>the</strong> construction of <strong>the</strong> second tunnel.<br />

y<br />

p<br />

Second<br />

tunnel<br />

r o<br />

x<br />

a<br />

First<br />

tunnel<br />

b<br />

Figure 4. Two tunnels at close proximity<br />

Assum<strong>in</strong>g that <strong>the</strong> ground is a homogeneous, isotropic, l<strong>in</strong>early elastic mass, <strong>the</strong> radial movement of<br />

<strong>the</strong> ground at a radial distance r from <strong>the</strong> centre of <strong>the</strong> second tunnel can be derived based on <strong>the</strong><br />

<strong>the</strong>ory of elasticity as follows:<br />

u = u o r o /r (1)<br />

The volume loss dur<strong>in</strong>g tunnell<strong>in</strong>g can be expressed as:<br />

Vs = {πr o 2 - π( r o - u o ) 2 }/ πr o<br />

2<br />

(2)<br />

Equation (2) gives:<br />

u o = r o {1-√(1-Vs)} (3)<br />

F19 5


Us<strong>in</strong>g equation (1) and (3):<br />

At po<strong>in</strong>t a, u a = u o r o /r a , where r a is <strong>the</strong> distance of po<strong>in</strong>t a to <strong>the</strong> centre of <strong>the</strong> second tunnel.<br />

At po<strong>in</strong>t b, u b = u o r o /r b , where r a is <strong>the</strong> distance of po<strong>in</strong>t a to <strong>the</strong> centre of <strong>the</strong> second tunnel.<br />

The maximum diametrical distortion, δ d is def<strong>in</strong>ed as δ d = u a - u b<br />

The radial distortion is given by:<br />

δ r = δ d /2 (4)<br />

Morgan (1961) showed that <strong>the</strong> bend<strong>in</strong>g moment due to distortion over radius is given by:<br />

M = (3EIδ r )/ r o<br />

2<br />

(5)<br />

Based on equations (4) and (5), <strong>the</strong> additional distortional moment <strong>in</strong> <strong>the</strong> first tunnel l<strong>in</strong><strong>in</strong>g due to <strong>the</strong><br />

second tunnel construction can be calculated. The total bend<strong>in</strong>g moments for structural design of <strong>the</strong><br />

segments are superimposed by add<strong>in</strong>g <strong>the</strong> additional distortional moment to <strong>the</strong> moment due to ground<br />

load<strong>in</strong>g, assum<strong>in</strong>g <strong>the</strong> hoop thrust rema<strong>in</strong>s unchanged.<br />

3. ALLOWABLE ADDITIONAL DISTORTION FOR CONSTRUCTION<br />

The method outl<strong>in</strong>ed <strong>in</strong> Section 2.3 above can be used to make allowance <strong>in</strong> <strong>the</strong> design of <strong>the</strong> tunnel<br />

l<strong>in</strong><strong>in</strong>g to cater for <strong>the</strong> effect of <strong>the</strong> second tunnel construction on <strong>the</strong> first tunnel. However, it is<br />

difficult to monitor such effect dur<strong>in</strong>g construction as <strong>the</strong> method relies on <strong>the</strong> prompt assessment of<br />

<strong>the</strong> volume loss generated by <strong>the</strong> second tunnel construction. This back analysis of <strong>the</strong> volume loss is<br />

typically not readily available at <strong>the</strong> time of tunnel construction. It is thus not practicable to use<br />

volume loss as a controll<strong>in</strong>g parameter dur<strong>in</strong>g construction. In order to overcome this shortcom<strong>in</strong>g, it<br />

is proposed to use <strong>the</strong> conventional convergence monitor<strong>in</strong>g as a means to ensure that <strong>the</strong> additional<br />

distortion of <strong>the</strong> first tunnel due to <strong>the</strong> second tunnel construction is with<strong>in</strong> <strong>the</strong> capacity of <strong>the</strong> l<strong>in</strong><strong>in</strong>g of<br />

<strong>the</strong> first tunnel.<br />

Additional analyses have been carried out <strong>in</strong> <strong>the</strong> design of CCL3 tunnel l<strong>in</strong><strong>in</strong>g to determ<strong>in</strong>e <strong>the</strong><br />

allowable additional diametrical distortion for construction. This allowable diametrical distortion is<br />

not only for <strong>the</strong> effect of second tunnel construction, but also for <strong>the</strong> effects of all o<strong>the</strong>r construction<br />

activities, for example cross passage construction. In <strong>the</strong> analyses, it has been assumed that <strong>the</strong> r<strong>in</strong>g<br />

has a reduced moment of <strong>in</strong>ertia as recommended by Muir Wood (1975). The follow<strong>in</strong>g steps are<br />

taken to determ<strong>in</strong>e <strong>the</strong> allowable diametrical distortion for construction:<br />

• The hoop thrust and moment under <strong>the</strong> ground load<strong>in</strong>g and surcharge are calculated based on <strong>the</strong><br />

method described by Muir Wood (1975) and modified by Curtis (1976);<br />

• The spare moment capacity is taken as <strong>the</strong> difference between <strong>the</strong> ultimate capacity based on <strong>the</strong><br />

re<strong>in</strong>forcement provided and <strong>the</strong> calculated moment due to <strong>the</strong> ground load<strong>in</strong>g and surcharge. Both<br />

ULS and SLS are checked and <strong>the</strong> lesser of <strong>the</strong> two is taken as <strong>the</strong> spare moment capacity that <strong>the</strong><br />

r<strong>in</strong>g has for construction.<br />

• This spare moment capacity is converted <strong>in</strong>to radial distortion with <strong>the</strong> use of Equation (10). This<br />

distortion multiplied by two is thus <strong>the</strong> allowable diametrical distortion for construction.<br />

Assum<strong>in</strong>g <strong>the</strong> allowable diametrical distortion will be fully developed dur<strong>in</strong>g construction, <strong>the</strong> r<strong>in</strong>g is<br />

checked for <strong>the</strong> capacity of 15mm distortion allowed for long term due to adjacent future unknown<br />

F19 6


development. Aga<strong>in</strong>, <strong>the</strong> additional moment that will be generated <strong>in</strong> <strong>the</strong> l<strong>in</strong><strong>in</strong>g due to <strong>the</strong> 15mm<br />

diametric distortion is computed by us<strong>in</strong>g Equation (10).<br />

The above procedures are illustrated by <strong>the</strong> N-M <strong>in</strong>teraction diagram <strong>in</strong> Figure 5 for <strong>the</strong> ultimate limit<br />

state. For serviceability limit state (crack width check<strong>in</strong>g), similar approach can be adopted.<br />

10000<br />

N (kN)<br />

9000<br />

8000<br />

7000<br />

6000<br />

5000<br />

4000<br />

3000<br />

2000<br />

1000<br />

0<br />

Ground<br />

Load<strong>in</strong>g<br />

Spare<br />

Capacity<br />

0 50 100 150 200 250 300 350 400<br />

M (kNm)<br />

f cu = 60 N/mm 2<br />

h = 275 mm<br />

b = 1000 mm<br />

Ground Load<strong>in</strong>g<br />

Ground Load<strong>in</strong>g +1%<br />

Volume Loss<br />

Figure 5. Moment – Hoop Thrust <strong>in</strong>teraction diagram for re<strong>in</strong>forcement ratio of 1.19%.<br />

4. MONITORING REQUIREMENTS<br />

The proposed monitor<strong>in</strong>g scheme is shown <strong>in</strong> Figure 6. The convergence monitor<strong>in</strong>g can be made by<br />

extensometers and <strong>the</strong> measurement should be able to determ<strong>in</strong>e <strong>the</strong> diametrical distortion of <strong>the</strong><br />

l<strong>in</strong><strong>in</strong>g. The required monitor<strong>in</strong>g frequency for each r<strong>in</strong>g <strong>in</strong> <strong>the</strong> first tunnel will depend on <strong>the</strong> position<br />

of <strong>the</strong> TBM of <strong>the</strong> second tunnel.<br />

Direction of advance<br />

TBM<br />

2nd Tunnel<br />

1st Tunnel<br />

1 D 1 D L 1 D 3 D<br />

Once daily<br />

Every 6 hours or every r<strong>in</strong>g<br />

progress whichever is<br />

Once daily<br />

Legend: L = length of TBM shield, D = Excavated tunnel diameter<br />

Figure 6. Convergence monitor<strong>in</strong>g scheme with read<strong>in</strong>g frequency<br />

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5. CONCLUSIONS<br />

The design methodology is presented for <strong>the</strong> design of <strong>the</strong> tunnel l<strong>in</strong><strong>in</strong>gs for CCL3 bored tunnels. A<br />

method has been proposed to make allowance <strong>in</strong> <strong>the</strong> tunnel l<strong>in</strong><strong>in</strong>g design to cater for <strong>the</strong> effect of <strong>the</strong><br />

second tunnel construction on <strong>the</strong> first tunnel if <strong>the</strong> two tunnels are aligned at closer than one tunnel<br />

diameter apart. Procedures are developed to derive <strong>the</strong> additional distortional capacity of tunnel<br />

l<strong>in</strong><strong>in</strong>gs. This capacity can be monitored dur<strong>in</strong>g construction by <strong>the</strong> conventional tunnel convergence<br />

monitor<strong>in</strong>g us<strong>in</strong>g taper extensometers. As <strong>the</strong> monitor<strong>in</strong>g is relatively simple and fast, <strong>the</strong> results will<br />

enable <strong>the</strong> eng<strong>in</strong>eer to assess whe<strong>the</strong>r <strong>the</strong> capacity of <strong>the</strong> l<strong>in</strong><strong>in</strong>g is exceeded dur<strong>in</strong>g construction.<br />

6. REFERENCES<br />

Curtis, D.J., 1976. Discussion, Geotechnique 26, 231 – 237<br />

Duddeck, H. and Erdmann, J., 1982. Structural design models for tunnels, Tunnell<strong>in</strong>g’82, International<br />

Symposium organised by Institution of M<strong>in</strong><strong>in</strong>g and Metallurgy.<br />

Morgan, H.D., 1961. A contribution to <strong>the</strong> analysis of stress <strong>in</strong> a circular tunnel, Geotechnique 11, 37<br />

– 46<br />

Muir Wood, A.M., 1975. The circular tunnel <strong>in</strong> elastic ground, Geotechnique 25, No. 1, 115 – 127.<br />

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