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<front>
<journal-meta>
<journal-id journal-id-type="publisher">NHESS</journal-id>
<journal-title-group>
<journal-title>Natural Hazards and Earth System Sciences</journal-title>
<abbrev-journal-title abbrev-type="publisher">NHESS</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Nat. Hazards Earth Syst. Sci.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1684-9981</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/nhess-10-191-2010</article-id>
<title-group>
<article-title>Rockslide deformation monitoring with fiber optic strain sensors</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Moore</surname>
<given-names>J. R.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gischig</surname>
<given-names>V.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Button</surname>
<given-names>E.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Loew</surname>
<given-names>S.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Geological Institute, Swiss Federal Institute of Technology (ETH), Zurich, Switzerland</addr-line>
</aff>
<pub-date pub-type="epub">
<day>02</day>
<month>02</month>
<year>2010</year>
</pub-date>
<volume>10</volume>
<issue>2</issue>
<fpage>191</fpage>
<lpage>201</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2010 J. R. Moore et al.</copyright-statement>
<copyright-year>2010</copyright-year>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri"  xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions>
<self-uri xlink:href="https://nhess.copernicus.org/articles/10/191/2010/nhess-10-191-2010.html">This article is available from https://nhess.copernicus.org/articles/10/191/2010/nhess-10-191-2010.html</self-uri>
<self-uri xlink:href="https://nhess.copernicus.org/articles/10/191/2010/nhess-10-191-2010.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/10/191/2010/nhess-10-191-2010.pdf</self-uri>
<abstract>
<p>With micro-strain resolution and the capability to sample at rates of 100 Hz
and higher, fiber optic (FO) strain sensors offer exciting new possibilities
for in-situ landslide monitoring. Here we describe a new FO monitoring system
based on long-gauge fiber Bragg grating sensors installed at the Randa
Rockslide Laboratory in southern Switzerland. The new FO monitoring system
can detect sub-micrometer scale deformations in both triggered-dynamic and
continuous measurements. Two types of sensors have been installed: (1) fully
embedded borehole sensors and (2) surface extensometers. Dynamic measurements
are triggered by sensor deformation and recorded at 100 Hz, while continuous
data are logged every 5 min. Deformation time series for all sensors show
displacements consistent with previous monitoring. Accelerated shortening
following installation of the borehole sensors is likely related to long-term
shrinkage of the grout. A number of transient signals have been observed,
which in some cases were large enough to trigger rapid sampling. The
combination of short- and long-term observation offers new insight into the
deformation process. Accelerated surface crack opening in spring is shown to
have a diurnal trend, which we attribute to the effect of snowmelt seeping
into the crack void space and freezing at night to generate pressure on the
crack walls. Controlled-source tests investigated the sensor response to
dynamic inputs, which compared an independent measure of ground motion
against the strain measured across a surface crack. Low frequency signals
were comparable but the FO record suffered from aliasing, where undersampling
of higher frequency signals generated spectral peaks not related to ground
motion.</p>
</abstract>
<counts><page-count count="11"/></counts>
</article-meta>
</front>
<body/>
<back>
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</article>