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  <titleInfo>
    <title>Modelling of pushing resistance on cohesionless soil using different scale model tests</title>
  </titleInfo>
  <name type="personal">
    <namePart>Nguyen Van Hoan</namePart>
    <role>
      <roleTerm authority="marcrelator" type="text">creator</roleTerm>
    </role>
  </name>
  <name type="personal">
    <namePart>Sugimoto, M.</namePart>
    <role>
      <roleTerm type="text">Chairperson</roleTerm>
    </role>
  </name>
  <name type="personal">
    <namePart>Balasubramaniam, A.S.</namePart>
    <role>
      <roleTerm type="text">Examination Committee</roleTerm>
    </role>
  </name>
  <name type="personal">
    <namePart>Ashford, Scott A.</namePart>
    <role>
      <roleTerm type="text">Examination Committee</roleTerm>
    </role>
  </name>
  <name type="corporate">
    <namePart>The Government of Japan</namePart>
    <role>
      <roleTerm type="text">Scholarship Donor</roleTerm>
    </role>
  </name>
  <typeOfResource>text</typeOfResource>
  <originInfo>
    <place>
      <placeTerm type="code" authority="marccountry">th</placeTerm>
    </place>
    <place>
      <placeTerm type="text">Bangkok</placeTerm>
    </place>
    <publisher>Asian Institute of Technology</publisher>
    <dateIssued>1996</dateIssued>
    <issuance>monographic</issuance>
  </originInfo>
  <language>
    <languageTerm authority="iso639-2b" type="code">eng</languageTerm>
  </language>
  <physicalDescription>
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    <extent>98 leaves</extent>
  </physicalDescription>
  <abstract>The capacity of cutting equipment depends on the acting load. Nevertheless, the acting  load on the cutter face of shield has not been clear. The last year research made clear that the  pushing resistance, which does not appear in the design of shield capacity, is an important  component of the acting load.  This study aims to make the model of pushing resistance on Cohesionless soil by  different scale model tests.  In this research study, Axial force and torque behavior exhibited in dry compact sand  (relative density of 100%) have been investigated. Pushing resistance, as a major component of  cutter torque, has been found to be the function of speed ratio (v/f), radius (R0 and Rj) and the  number of cutter path (P n), which is different from the theoretic equations. Based on the  experimental results the model equations for pushing resistance have been proposed. As the  stress concentration occurs at the tip of the cutter bits, the friction concept does not satisfy the  test model and two constants known as influencing factors At and b have been introduced to  describe the model. These parameters both are found to be the function of face angle (Uc) and  clearance angle (y c)·</abstract>
  <note>A thesis submitted in partial fulfillment of requirements for the degree of Master of  Engineering, School of Civil Engineering</note>
  <note>Thesis (M. Eng.) - Asian Institute of Technology, 1996</note>
  <subject authority="lcsh">
    <topic>Shields (Geology)</topic>
  </subject>
  <subject authority="lcsh">
    <topic>Tunnels</topic>
  </subject>
  <relatedItem type="series">
    <titleInfo>
      <title>Thesis ; no. GE-95-15</title>
    </titleInfo>
    <name type="corporate">
      <namePart>Asian Institute of Technology.</namePart>
      <namePart/>
    </name>
  </relatedItem>
  <identifier type="uri">http://203.159.5.9/ait-thesis/detail.php?q=B15105</identifier>
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    <url displayLabel="Full-Text">http://203.159.5.9/ait-thesis/detail.php?q=B15105</url>
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