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				<title>NTU CEE Graduate Club : download</title>
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				<pubDate>Fri, 10 Sep 2010 20:55:58 -0600</pubDate>
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					<title>NTU CEE Graduate Club : download</title>
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						<title>Singapore Salary Survey year 2010</title>
<link>http://ntuceegrad.org/download.php?view.452</link>
<description></description>
<category domain='http://ntuceegrad.org/download.php?list.11'>Reports</category>
<pubDate>Wed, 10 Feb 2010 10:22:52 -0700</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.452</guid>
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						<title>PORE STRUCTURE AND DURABILITY OF CONCRETE CONTAINING GBFS</title>
<link>http://ntuceegrad.org/download.php?view.451</link>
<description><![CDATA[INTRODUCTION<br />The use of Granulated Blast Furnace Slag (GBFS) as<br />supplementary cementitious material for concrete production<br />is ecologically and economically very important[1]. High<br />quality and durable concrete is required to reduce the<br />rapid deterioration of concrete in severe conditions. It<br />has been proven that GBFS has perfect performance to<br />resist chloride induced corrosion[2]. Replacing Portland<br />Cement (PC) partially by GBFS can improve the fluidity<br />of fresh concrete, reduce its bleeding and postpone the<br />setting[3]. The quality of GBFS depends on the chemical<br />composition, glass phase content and fi neness of GBFS[4].<br />Using mineral admixtures will result in the consumption<br />of calcium hydroxide in concrete. In short curing period,<br />it may increase the carbonation rate of concrete[1]. In this<br />study, the effect of replacing PC with various percentages<br />of GBFS on different characteristics of concrete has been<br />studied. Replacing PC partially with GBFS improved the<br />characteristic of concrete significantly.<br /><br /><script type="text/javascript"><!--google_ad_client = "pub-3118306239017845";/* 468x60, created 5/1/09 */google_ad_slot = "7355621409";google_ad_width = 468;google_ad_height = 60;//--></script><script type="text/javascript"src="http://pagead2.googlesyndication.com/pagead/show_ads.js"></script><p>Authors:</p>Sabet Divsholi Bahador (Sabe0001@ntu.edu.sg)<br />Jong Herman Cahyadi (CHSjong@ntu.edu.sg)]]></description>
<category domain='http://ntuceegrad.org/download.php?list.9'>Research Bulletin</category>
<author>Sabe0001@nospam.com (Sabet Divsholi Bahador)</author>
<pubDate>Sun, 03 May 2009 06:31:46 -0600</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.451</guid>
</item>
						<item>
						<title>SUMATRAN MEGATHRUST EARTHQUAKES: WHAT HAS HAPPENED, AND WHAT’S NEXT?</title>
<link>http://ntuceegrad.org/download.php?view.450</link>
<description><![CDATA[Why does Sumatra keep sending earthquakes our way? And<br />what might be coming next? These are questions that many<br />Singaporeans are asking recently, as the shaking that began<br />in June 2000 continues.<br />The world’s biggest earthquakes and most of its volcanoes<br />occur where giant tectonic plates beneath the oceans are<br />diving down under neighbouring landmasses. Singapore is<br />fortunate to lie several hundred kilometres from the nearest<br />such “subduction” zone, in the middle of a tectonic plate<br />that includes all of its Southeast Asian neighbours. Still, the<br />western edge of that plate, on the other side of Sumatra,<br />generates such big earthquakes that gentle swaying is<br />commonly felt in Singapore.<br />All of the earthquakes we have felt in the past eight years<br />happened because the upper surface of the downgoing<br />oceanic plate (called the Sunda megathrust) is sticky. As the<br />oceanic plate descends northward at about 60 millimetres per<br />year beneath Sumatra, it clings to Sumatra’s underside along<br />the megathrust, until it reaches depths of 50 kilometres or<br />so, where it fi nally becomes hot and gooey enough to slip<br />steadily into the deep earth.<br /><br /><script type="text/javascript"><!--google_ad_client = "pub-3118306239017845";/* 468x60, created 5/1/09 */google_ad_slot = "7355621409";google_ad_width = 468;google_ad_height = 60;//--></script><script type="text/javascript"src="http://pagead2.googlesyndication.com/pagead/show_ads.js"></script><p>Authors:</p>Kusnowidjaja Megawati (kusno@ntu.edu.sg)<br />Kerry Sieh (sieh@ntu.edu.sg)<br />Tso-Chien Pan (cpan@ntu.edu.sg)]]></description>
<category domain='http://ntuceegrad.org/download.php?list.9'>Research Bulletin</category>
<author>kusno@nospam.com (Kusnowidjaja Megawati)</author>
<pubDate>Sun, 03 May 2009 06:30:35 -0600</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.450</guid>
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						<title>STRAIN TRANSFER MODELS FOR STRAIN ACTUATORS</title>
<link>http://ntuceegrad.org/download.php?view.449</link>
<description><![CDATA[INTRODUCTION<br />One of the advantages of piezo-composite actuators is to<br />provide low cost and in-situ actuation with high fl exibility[1].<br />Actuators as patches made of bulk lead zirconate titanate<br />(PZT) material are widely used for vibration control of<br />mechanical structures. However, extremely brittle nature<br />of the PZT material requires extra attention during the<br />handling and bonding procedures[2]. Micro fi ber composite<br />(MFC) has shown its great potential for vibration and<br />noise control, health monitoring, morphing of structures<br />and energy harvesting[3]. To explore various applications<br />of MFC, a reasonable model accounting for the strain<br />transfer phenomenon between the MFC and the structure<br />is crucial[4]. There have been a few one dimensional (1-D)<br />models on strain transfer[5,6,7], but issues still remain on<br />how accurately these models predict the phenomenon and<br />how effectively they can be extended to two dimensional<br />(2-D) cases to increase the accuracy of prediction.<br />In this work, the existing 1-D Bernoulli-Euler formulation<br />for bending, coupled bending and extension of isotropic<br />beams/plates with induced strain actuators is extended to 2-D<br />cases. Further, it is improved to account for the reduction in<br />actuation as a result of strain distribution inside the actuator.<br />The improved 1-D and 2-D formulations are compared with<br />the uniform strain model which includes the shear lag effects<br />due to the adhesive layer. A fi nite element model is also<br />developed to study the strain transfer. Finally, an experimental<br />test is carried out to evaluate the accuracy and limitations<br />of the developed models. Results show that the models are<br />in good agreement with the experiment.<br /><br /><script type="text/javascript"><!--google_ad_client = "pub-3118306239017845";/* 468x60, created 5/1/09 */google_ad_slot = "7355621409";google_ad_width = 468;google_ad_height = 60;//--></script><script type="text/javascript"src="http://pagead2.googlesyndication.com/pagead/show_ads.js"></script><p>Authors:</p>Yang Yaowen (cywyang@ntu.edu.sg)<br />Sabet Divsholi Bahador (sabe0002@ntu.edu.sg)]]></description>
<category domain='http://ntuceegrad.org/download.php?list.9'>Research Bulletin</category>
<author>cywyang@nospam.com (Yang Yaowen)</author>
<pubDate>Sun, 03 May 2009 06:29:35 -0600</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.449</guid>
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						<title>STATIC ULTIMATE STRENGTH OF CRACKED SQUARE HOLLOW SECTION Y-JOINT</title>
<link>http://ntuceegrad.org/download.php?view.448</link>
<description><![CDATA[INTRODUCTION<br />To validate the fi nite element models of a cracked square<br />hollow section (SHS) Y-joint[1], a full-scale specimen was<br />tested under incremental loads up to failure. The Y-joint<br />was fi rst fatigue cracked using the “Orange Frame” test<br />rig available in the Construction Technology Laboratory.<br />The specimen contains a surface crack located at one of<br />the corners as shown in Figure 1. After completion of the<br />fatigue test, the crack dimensions were measured using the<br />Alternating Current Potential Drop (ACPD) technique[2].<br />The specimen was fabricated from BS4360 structural<br />steel of grade 50D[3]. The weld profi le and the specimen<br />preparation were carried out in accordance with the American<br />Welding Society (AWS) Structure Welding Code–Steel<br />D1.1/D.1.1M:2006[4] specifi cations. The specimen material<br />yield stress is 380.3 MPa.<br /><br /><script type="text/javascript"><!--google_ad_client = "pub-3118306239017845";/* 468x60, created 5/1/09 */google_ad_slot = "7355621409";google_ad_width = 468;google_ad_height = 60;//--></script><script type="text/javascript"src="http://pagead2.googlesyndication.com/pagead/show_ads.js"></script><p>Authors:</p>Lie Seng Tjhen (cstlie@ntu.edu.sg)<br />Yang Zhengmao (ZhengMao.Yang@dnv.com.sg)]]></description>
<category domain='http://ntuceegrad.org/download.php?list.9'>Research Bulletin</category>
<author>cstlie@nospam.com (Lie Seng Tjhen)</author>
<pubDate>Sun, 03 May 2009 06:28:12 -0600</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.448</guid>
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						<title>SCF PREDICTION OF COMPLEX TUBULAR JOINT USING INTERPOLATION APPROACH</title>
<link>http://ntuceegrad.org/download.php?view.446</link>
<description><![CDATA[INTRODUCTION<br />In the fatigue assessment of tubular joint, the stress<br />concentration factor (SCF) is one of the most important<br />indicators that determine the performance of the joint under<br />cyclic loading. The variation of the SCF with respect to the<br />geometrical and loading parameters is always a critical factor<br />that needed to be considered during tubular joint design. In<br />most design codes for tubular joints, the variations of the<br />SCF with respect to the geometrical and loading parameters<br />are described by some empirical equations. These equations<br />are normally obtained by applying multi-variable regression<br />analysis on the numerical modelling results obtained from<br />parametric studies on a set of identifi ed parameters. For<br />simple joint types under simple loading condition, these<br />empirical equations are often able to provide reasonable<br />predictions. However, for the cases of a more complicated<br />joint or a simple joint under complex loading, such an<br />approach would often result in lengthy equations [1].<br />Furthermore, due to the complexity of the joint and the<br />presence of many parameters, these lengthy equations would<br />not be able to give good predictions over the whole range<br />of parameters. To overcome this problem, a new approach<br />based on the interpolation method described below was<br />proposed [1-3].<br /><br /><script type="text/javascript"><!--google_ad_client = "pub-3118306239017845";/* 468x60, created 5/1/09 */google_ad_slot = "7355621409";google_ad_width = 468;google_ad_height = 60;//--></script><script type="text/javascript"src="http://pagead2.googlesyndication.com/pagead/show_ads.js"></script><p>Authors:</p>Lee Chi King (ccklee@ntu.edu.sg)<br />Chiew Sing Ping (cspchiew@ntu.edu.sg)<br />Lie Seng Tjhen (cstlie@ntu.edu.sg)<br />Sopha Thong (soph0001@ntu.edu.sg)]]></description>
<category domain='http://ntuceegrad.org/download.php?list.9'>Research Bulletin</category>
<author>ccklee@nospam.com (Lee Chi King)</author>
<pubDate>Sun, 03 May 2009 06:25:58 -0600</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.446</guid>
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						<title>DAMAGE DETECTION USING MULTIPLE PIEZO-IMPEDANCE TRANSDUCERS</title>
<link>http://ntuceegrad.org/download.php?view.445</link>
<description><![CDATA[INTRODUCTION<br />Smart materials based structural health monitoring (SHM)<br />has attracted extensive research attention in the past decade.<br />Lead zircornate titanate (PZT) impedance transducers,<br />working on the principle of electromechanical impedance<br />(EMI), are among the most widely used smart materials due<br />to their self actuation and sensing capabilities. One single<br />PZT is sensitive enough to detect incipient damage and<br />its propagation [1]. However, it is diffi cult to identify the<br />location of structural damage by a single PZT. Therefore,<br />in this article, an experimental investigation on damage<br />location using multiple PZTs is fi rstly presented, followed<br />by the numerical simulation for verifi cation.<br /><br /><script type="text/javascript"><!--google_ad_client = "pub-3118306239017845";/* 468x60, created 5/1/09 */google_ad_slot = "7355621409";google_ad_width = 468;google_ad_height = 60;//--></script><script type="text/javascript"src="http://pagead2.googlesyndication.com/pagead/show_ads.js"></script><p>Authors:</p>Yang Yaowen (cywyang@ntu.edu.sg)<br />Liu Hui (liuh0019@ntu.edu.sg)]]></description>
<category domain='http://ntuceegrad.org/download.php?list.9'>Research Bulletin</category>
<author>cywyang@nospam.com (Yang Yaowen)</author>
<pubDate>Sun, 03 May 2009 06:25:05 -0600</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.445</guid>
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						<title>MONITORING VIBRATING STRUCTURES USING PZT IMPEDANCE TRANSDUCERS</title>
<link>http://ntuceegrad.org/download.php?view.444</link>
<description><![CDATA[INTRODUCTION<br />The electromechanical impedance (EMI) method has<br />emerged as a widely recognized technique for dynamic<br />identifi cation and health monitoring of structural systems.<br />The electromechanical admittance response of the smart<br />system is derived from the dynamic interaction relation<br />between the lead zirconate titanate (PZT) transducer and<br />the host structure. For structural health monitoring (SHM)<br />applications, these spectra may be compared at various times<br />during the service lifespan of the structure, in which any<br />change between the spectra is an indication of the presence of<br />damage or material deterioration. However, the existing EMI<br />method does not consider the structural vibration caused by<br />the external excitation other than the PZT actuation, which<br />means that the existing EMI method is only applicable to<br />the static structures [1-3]. Unfortunately, many structures<br />are subjected to vibrations in practice. The vibrations of the<br />structures will infl uence the results of SHM by causing the<br />changes in PZT signatures. The changes in PZT signatures<br />caused by the external excitation and the structural damage<br />must be differentiated such that the correct information of<br />structural health state can be obtained. Therefore, this paper<br />attempts to study the infl uence of the external excitation on<br />the PZT impedance signature.<br />For this purpose, a new EMI model is developed for a<br />simply supported beam structure with external excitations.<br />Furthermore, an experimental test is carried out to verify<br />the developed theoretical model.<br /><br /><script type="text/javascript"><!--google_ad_client = "pub-3118306239017845";/* 468x60, created 5/1/09 */google_ad_slot = "7355621409";google_ad_width = 468;google_ad_height = 60;//--></script><script type="text/javascript"src="http://pagead2.googlesyndication.com/pagead/show_ads.js"></script><p>Authors:</p>Yang Yaowen (cywyang@ntu.edu.sg)<br />Miao Aiwei (miao0009@ntu.edu.sg)]]></description>
<category domain='http://ntuceegrad.org/download.php?list.9'>Research Bulletin</category>
<author>cywyang@nospam.com (Yang Yaowen)</author>
<pubDate>Sun, 03 May 2009 06:23:47 -0600</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.444</guid>
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						<title>ENERGY HARVESTING USING MICRO-FIBER COMPOSITES</title>
<link>http://ntuceegrad.org/download.php?view.443</link>
<description><![CDATA[INTRODUCTION<br />The decreasing energy consumption of MEMS, wireless<br />sensors and portable electronics invokes the possibility<br />to harvest energy from ambient vibrations for self power<br />supply. One simple method for vibration energy harvesting<br />is utilizing the direct piezoelectric effect. The macro-fi ber<br />composites (MFC)[1] are featured in their fl exibility of large<br />deformation, which enables them to harvest energy from<br />vibrations with little brittle risk and to serve for an unlimited<br />lifespan. However, the effi ciency of MFC has not been well<br />investigated. This article focuses on the effi ciency of the<br />energy harvesting system using MFC attached on a cantilever<br />beam. The output voltage of the MFC harvester is tested<br />and estimated using the fi nite element method (FEM). The<br />procedures of energy storing to the capacitor are simulated<br />using electronic design automation (EDA) software. By<br />combining the FEM and EDA simulations, the effi ciency of<br />the MFC energy harvesting system is estimated.<br /><br /><script type="text/javascript"><!--google_ad_client = "pub-3118306239017845";/* 468x60, created 5/1/09 */google_ad_slot = "7355621409";google_ad_width = 468;google_ad_height = 60;//--></script><script type="text/javascript"src="http://pagead2.googlesyndication.com/pagead/show_ads.js"></script><p>Authors:</p>Yang Yaowen (cywyang@ntu.edu.sg)<br />Tang Lihua (c070073@ntu.edu.sg)]]></description>
<category domain='http://ntuceegrad.org/download.php?list.9'>Research Bulletin</category>
<author>cywyang@nospam.com (Yang Yaowen)</author>
<pubDate>Sun, 03 May 2009 06:22:51 -0600</pubDate>
<guid isPermaLink="true">http://ntuceegrad.org/download.php?view.443</guid>
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