STABILTY ASSESSMENT OF HEADRACE TUNNEL SYSTEM FOR PUNATSANGCHHU II HYDROPOWER PROJECT, BHUTAN_Estimation of seepage and water leakage in underground tunnels

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  • 7/28/2019 STABILTY ASSESSMENT OF HEADRACE TUNNEL SYSTEM FOR PUNATSANGCHHU II HYDROPOWER PROJECT, BHUTAN

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    6/12/13 12 STABILTY ASSESSMENT OF HEADRACE TUNNEL SYSTEM FOR PUNATSANGCHHU II HYDROPOWER PROJECT, BHUTAN Karma Tsheri

    www.orgsun.com/2/4/21175-12-stabilty-assessment-headrace-tunnel-system-for-punatsangchhu.php

    rock mass, the support material will be subjected to high stresses and sometimes when the

    support fails to sustain the large deformation caused by high tangential stresses, the tunnelssqueezes inward reducing the size of opening. In extreme cases, new equilibrium are reachedafter the complete closure of tunnel, eg Kovari in 1998 and Steiner 1996 (Panthi, 2006). Manyauthors have developed different approaches to predict tunnel squeezing. Hoek and Marinosapproach is discussed below.

    Hoek and Marinos (2000) Over burden alone is not responsible for squeezing. The changingstrength and deformability properties of the rock mass over time have far greater consequenceson squeezing (Kovari, 1998).

    In Hoek and Marinos approach, rock mass strength and over burden are the two parameters

    considered responsible for squeezing. With this view, Hoek and Brown (2000) have suggested arelation that gives total strain (ratio of tunnel closer to tunnel diameter), which is a function ofrock mass strength and in-situ overburden pressure. The criterion is based on iso-static circularstress condition.

    The support pressure can be calculated using different equations. The RMR method andUnal method are used here.

    The rock support pressure from the RMR relation.

    Norwegian University of Science and Technology, Trondheim Page Stability Analysis 100RMR P * * Dt.................................................................5(24) The support pressure can alsobe calculated using equation proposed by Unal (1983) as shown below.

    B Pi (100 RMR) * *.............................................................5(25) Where is rock density int/m3, and B is tunnel width in m. accordingly the deformation in the tunnels were calculated firstwithout support pressure and later with support pressure. The rock support pressure is tabulatedin table 5.13.

    Figure 5.11 Tunnel convergence and degree of difficulties associated with tunnel squeezing(Hoek & Marinos, 2000) Hoek and Marinos defined the plastic zone (R) and total tunnel strain (t)by following equations.

    ....5(26) 5(27) Where t is total inward deformation and t istotal inward strain. Pi is the support pressure in MPa. When the support pressure is taken aszero, the squeezing condition in the rock mass may be rewritten as.5(28) ..5(29)Norwegian University of Science and Technology, Trondheim Page Stability Analysis Hoek ansMarinos have assumed that weak rock mass are incapable of sustaining significant differentialstress and failure will occur till in-situ horizontal and vertical stresses are equalized.

    This justifies why they considered over burden instead of tangential stresses, which isalways greater than over burden pressure for estimating tunnel squeezing. For defining theapproximate degree of difficulty at different level of tunneling, the figure 5.11 right is used.

    The squeezing results from the Hoek and Marinos relations for the different reaches alongthe HRT alignment is given in table 5.13. The squeezing chart states that, degree of squeezingwill be with few support problems when strain is less than 1%. Minor squeezing problem whenstrain is between 1 %and 2.5%. When the strain exceeds 2.5% but less than 5% there can besevere squeezing problem in the rock mass. The tunnel will face extreme squeezing when thestrain exceeds 10%.

    Table 5-13Support pressure and deformation along the HRT alignment Description Ch.0 toAdit I Adit I to Adit II Adit II to S/shaft Support pressure MPa 6.23 6.68 7.Deformation withoutsupport 0.1 0.33 0.pressure % Deformation with support 0.003 0.06 0.pressure % From theresults, very less squeezing problems is expected along the HRT. All the possible squeezing canbe solved by adopting simple flexible support measures. However, since all these inputparameters are calculations based on rock mass parameters on the surface, it should not be areason to relax. There should be adequate readiness for any worsening squeezing problem

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    6/12/13 12 STABILTY ASSESSMENT OF HEADRACE TUNNEL SYSTEM FOR PUNATSANGCHHU II HYDROPOWER PROJECT, BHUTAN Karma Tsheri

    www.orgsun.com/2/4/21175-12-stabilty-assessment-headrace-tunnel-system-for-punatsangchhu.php

    Different types of support are adopted based on the nature of stability problems. Therecannot be a single standard support for any stability problem. It has to be customized dependingon rock mass parameters, technology, time and money available. The best support system canbe one which provides reasonably best stability within minimum time and cost. Some of thecommonly adopted support systems in tunnel stability problem are discussed below.

    6.1.1 Scaling Scaling involves removal of disintegrated loose hanging rock fragmentstriggered by vibration impact of blasting around the tunnel periphery. It is carried outimmediately after every cycle of blast at the face of the tunnel. Normally 20-30 minutes isrequired to remove the loose fragments rocks. Different methods of scaling are Manual scalingManual scaling is one of the oldest methods of scaling. The scaling is done from the piles of

    blasted material or from wheel loaders as a platform. It is risky and has poor safety standards. Itis not much in use these days except in small drifts and shafts where machines cannot be used.

    Figure 6.1 and 6.2 illustrates manual scaling.

    Figure 6.1 Mannual scaling from muck pile (L) & from scissor plateform (R) NorwegianUniversity of Science and Technology, Trondheim Page Rock Support Estimation Mechanicalscaling The scaling is done using the tunneling rig machines. This has improves safetystandards and consumes less time. In Bhutan, mechanical scaling is most widely practiced.Figure 5.2 illustrates how mechanical scaling is done.

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