<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJCM</journal-id><journal-title-group><journal-title>Open Journal of Composite Materials</journal-title></journal-title-group><issn pub-type="epub">2164-5612</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojcm.2014.44021</article-id><article-id pub-id-type="publisher-id">OJCM-50807</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Unsymmetrical Fibre-Reinforced Plastics for the Production of Curved Textile Reinforced Concrete Elements
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>enrik</surname><given-names>L. Funke</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Sandra</surname><given-names>Gelbrich</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>Andreas</surname><given-names>Ehrlich</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>Lars</surname><given-names>Ulke-Winter</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>Lothar</surname><given-names>Kroll</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Institute of Lightweight Structures, Technische Universit?t Chemnitz, Chemnitz, Germany </addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>henrik.funke@mb.tu-chemnitz.de(ELF)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>25</day><month>09</month><year>2014</year></pub-date><volume>04</volume><issue>04</issue><fpage>191</fpage><lpage>200</lpage><history><date date-type="received"><day>11</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>30</day>	<month>September</month>	<year>2014</year>	</date><date date-type="accepted"><day>11</day>	<month>October</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  A new constructive and technological approach was developed for the efficient production of large-
  dimensioned, curved freeform formworks, which allow the manufacturing of single and double-curved textile reinforced concrete elements. The approach is based on a flexible, multi-layered formwork system, which consists of glass-fibre reinforced plastic (GFRP). Using the unusual structural behavior caused by anisotropy, these GFRP formwork elements permit a specific adjustment of defined curvature. The system design of the developed GFRP formwork and the concrete-lightweight-elements with stabilized spacer fabric was examined exhaustively. Prototypical curved freeform surfaces with different curvature radii were designed, numerically computed and produced. Furthermore, the fabric’s contour accuracy of the fabric was verified, and its integration was adjusted to loads.
 
</p></abstract><kwd-group><kwd>Anisotropic Formworks</kwd><kwd> Textile-Reinforced Concrete</kwd><kwd> Fibre-Reinforced Plastics</kwd><kwd> Curved Concrete</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Research in the fields of innovative concrete structures with high potential for lightweight design, and of textile reinforcement for special applications has been object of intensive scientific and application-oriented efforts for a couple of years [<xref ref-type="bibr" rid="scirp.50807-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.50807-ref3">3</xref>] . There is a lack of appropriate formwork systems to implement light shell structures of this kind, with the need for flexibly moldable, reusable systems being particularly tense [<xref ref-type="bibr" rid="scirp.50807-ref4">4</xref>] . Textile reinforced concrete offers a high range of variation and thus facilitates a flexible adjustment of the form and textile reinforcement to the relevant conditions (cf. e.g. [<xref ref-type="bibr" rid="scirp.50807-ref5">5</xref>] ) and the citations listed there). Another advantage in comparison to ordinary reinforced concrete is that corrosion can be largely excluded. In this way, filigree constructions of minimal thickness can be realized [<xref ref-type="bibr" rid="scirp.50807-ref6">6</xref>] -[<xref ref-type="bibr" rid="scirp.50807-ref8">8</xref>] .</p><p>A crucial technological objective of textile reinforced concrete elements is the development of complex solid preform-structures. These are produced by processing flat structures through appropriate cutting [<xref ref-type="bibr" rid="scirp.50807-ref9">9</xref>] . The soft- elastic behavior of the 3D-textiles can be influenced to a large extent by modifying parameters such as stiffness, alignment and concentration of pile threads. In this way, it can be adjusted to the defined curvature. Although selectively deformable textile 3D-structures, for instance spacer fabric, for the reinforcement of concrete light- weight elements exist, the corresponding formwork elements are only in an early stage of development. These elements are essential for the realization of concrete shell structures that can be curved in any way.</p><p>Currently, the only possible shapes of shell structures are that of domes, hyperbolic paraboloids and conoids. Their production furthermore entails a considerable amount of material and high costs [<xref ref-type="bibr" rid="scirp.50807-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.50807-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.50807-ref11">11</xref>] . Also the mathematical description of the predetermined complex freeform surfaces and the anisotropic material characteristic is difficult [<xref ref-type="bibr" rid="scirp.50807-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.50807-ref13">13</xref>] . In the field of computer-aided visualization, different methods have been developed for the shape optimization of surfaces and their static construction calculation and design. However, these technologies are until now not applied in formwork production [<xref ref-type="bibr" rid="scirp.50807-ref14">14</xref>] . Among the common formwork techniques are conventionally segmented steel and wood systems, pneumatically supported and modeled formworks and combinations of them [<xref ref-type="bibr" rid="scirp.50807-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.50807-ref16">16</xref>] .</p><p>Close examinations of the production of double-curved concrete-lightweight-elements based on flexible formwork systems made from GFRP are yet to come. The focus of this research work is on the numerical calculation and experimental verification of flexible, anisotropic GFRP formworks and the production of prototypical double-curved concrete-lightweight-elements with integrated stabilizing spacer fabric.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Components for Glass-Fibre Reinforced Plastic</title><p>The unidirectional (UD) reinforced fabric UT-E500 by GURIT Holding AG was used for the production of the GFRP formwork. UT-E500 consists of aluminoborosilicate (“E glass”) and has an area density of 500 g/sqm. For the thermosetting resin matrix, the epoxy resin Epilox&#174; T19-27 by LEUNA-Harze GmbH was used. By means of manual laminating, UD single layers were made from the UD fabric and the epoxy resin. They had a fibre volume content of 30%. Within this UD single layer, the independent parameters: longitudinal (E1) and transverse (E2) moduli of elasticity, Poisson’s ratio (v<sub>12</sub>), shear modulus (G<sub>12</sub>) and the coefficients of linear thermal expansion α<sub>1</sub> and α<sub>2</sub> between +20˚C and +120˚C were determined experimentally. <xref ref-type="table" rid="table1">Table 1</xref> shows the results of these tests.</p></sec><sec id="s2_2"><title>2.2. Adjustment and Determination of Defined Curvatures</title><p>The determined basic parameters of the unidirectional single layer (<xref ref-type="table" rid="table1">Table 1</xref>) were used for the analytical and numerical calculation of multi-layered formworks, which showed both a balanced symmetrical and an asymmetrical construction. The GFRP formwork with a plate size of 50 &#215; 50 cm<sup>2</sup> was made of 11 UD single layers with total thickness of 3.3 mm (<xref ref-type="fig" rid="fig1">Figure 1</xref>).</p><p>After the production of the GFRP bond, the thermosetting matrix was cured in a heating cabinet over a period of 6 hours at a constant temperature of 120˚C. After curing, the GFRP bond were cooled to room temperature (20˚C). Due to this difference in temperature of −100 K, residual stress caused a small curvature of the anisotropic layer structure. Afterwards, high curvatures were caused by external preloading (up to a material load of R = 0.95 after CUNTZE criterion), utilizing the coupling effects that result from the GFRP bond (<xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>The calculations of the coupling effects caused by anisotropy were conducted analytically with the Classical Laminate Theory (CLT) and the First Order Shear Deformation Theory (FSDT). For the experimental verifica-</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Parameters of the unidirectional single layer</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >E<sub>1</sub> GPa</th><th align="center" valign="middle" >E<sub>2</sub> GPa</th><th align="center" valign="middle" >ν<sub>12</sub> -</th><th align="center" valign="middle" >G<sub>12</sub> GPa</th><th align="center" valign="middle" >α<sub>1(20/120)</sub> 10<sup>−6</sup>&#183;K<sup>−1</sup></th><th align="center" valign="middle" >α<sub>2(20/120)</sub> 10<sup>−6</sup>&#183;K<sup>−1</sup></th></tr></thead><tr><td align="center" valign="middle" >23.7</td><td align="center" valign="middle" >6.4</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >130</td></tr></tbody></table></table-wrap><p>tion of the anisotropic coupling effects calculated beforehand, selected GFRP bonds segments were produced and tested in the institute’s own structural test bench with the ABD-testing device (<xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>The results were used during the further procedure for the determination of the functional relations of curvatures, process parameters and geometrical parameters. Based on that, the analysis and identification of single and double curved basic forms was conducted. Their combination resulted in a maximum of defined freeform surfaces.</p><p>The experimental analysis of the curves was conducted with the aid of the optical forming-analysis-systems ARGUS and ARAMIS by GOM (<xref ref-type="fig" rid="fig4">Figure 4</xref>).</p></sec><sec id="s2_3"><title>2.3. Polymer-Bound Stabilization of 3D Spacer Fabrics for the Integration into Concrete</title><p>For the production of the textile reinforced concrete elements, the textile 3D-fabric “SITgrid” by V. Fraas Solutions in Textile GmbH was used. It is made from alkali-resistant glass (AR glass), with 2400 tex in warp and weft (<xref ref-type="fig" rid="fig5">Figure 5</xref>), which had a tensile strength of 978 MPa. The fabric was placed on the formwork elements to show and stabilize the curvatures accurately. Thermosetting and thermoplastic resin systems were used for the stabilization. The resin systems were applied by spraying, rolling or by using of capillary effect of the pile thread on the pre-curved 3D-fabric. By means of the Fourier transform infrared spectroscopy with attenuated total reflection (ATR-FTIR), the impact of the pile thread on capillary suction with the epoxy resin Indufloor-IB1240 of the company SCHOMBURG GmbH could be studied. For this purpose the ATR-FTIR testing apparatus ALPHA-P by BRUKER DALTONIK GmbH was used.</p></sec><sec id="s2_4"><title>2.4. Textile Reinforced Concrete</title><p>The development of the fine grained concrete was focused on the workability of the fresh concrete as well as the</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Process chain of anisotropic GFRP layered bond structures</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x5.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Temperature and tensile load of anisotropic GFRP layered bond structures for the adjustment of curvature states</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x6.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> ABD-testing device</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x7.png"/></fig><p>durability and good bonding between concrete matrix and textile reinforcement. <xref ref-type="table" rid="table2">Table 2</xref> shows the qualitative and quantitative composition of the fine grained concrete mix. Apart from white Portland cement type 52.5 R, the fine concrete contained an amorphous aluminosilicate as puzzolanic binder (<xref ref-type="table" rid="table2">Table 2</xref>). Dolomite sand with a grain size of 0.5 to 1.0 mm was used as aggregate and dolomite powder with an average grain size of 70 &#181;m was used as filler. The alkali-resistant (AR) short glass fibres (16 M.-% ZrO2) were 12 mm long and had a length mass of 45 tex. The high-performance superplasticizers had a polycarboxylate ether (PCE) contentof 30 M.-%. The water-cement-ratio was 0.37.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Curved GFRP layered bond structure plate with coded reference mark (picture on the left) and test set-up of the optical forming-analysis-system ARGUS (picture on the right)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x8.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> 3D-fabrics “SITGrid” by V. Fraas Solutions in Textile GmbH</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x9.png"/></fig><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Composition of the fine grained concrete mix</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Component</th><th align="center" valign="middle" >Content in kg/m<sup>3</sup></th><th align="center" valign="middle" >Mass fraction in %</th></tr></thead><tr><td align="center" valign="middle" >White cement CEM I 52.5 R</td><td align="center" valign="middle" >500</td><td align="center" valign="middle" >21.39</td></tr><tr><td align="center" valign="middle" >Amorphous aluminosilicate</td><td align="center" valign="middle" >150</td><td align="center" valign="middle" >6.42</td></tr><tr><td align="center" valign="middle" >Dolomite sand 0.5/1.0 (&#215;50 = 0.71 mm)</td><td align="center" valign="middle" >1270</td><td align="center" valign="middle" >54.32</td></tr><tr><td align="center" valign="middle" >Dolomite filler (&#215;50 = 70 &#181;m)</td><td align="center" valign="middle" >150</td><td align="center" valign="middle" >6.42</td></tr><tr><td align="center" valign="middle" >Water</td><td align="center" valign="middle" >240</td><td align="center" valign="middle" >10.27</td></tr><tr><td align="center" valign="middle" >AR-glass fibres (12 mm, integral)</td><td align="center" valign="middle" >18</td><td align="center" valign="middle" >0.77</td></tr><tr><td align="center" valign="middle" >superplasticizers</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.43</td></tr></tbody></table></table-wrap></sec><sec id="s2_5"><title>2.5. Production Tests GFRP Formworks/Concrete-Lightweight-Elements</title><p>Selected representative freeform surfaces, double-curved with different radii of curvature, were produced in the production tests for the system structure GFRP formworks/concrete-lightweight-elements. The adjustment of the curves is carried out via the new flexible GFRP formwork elements. The basic proceeding when conducting the production tests comprised the production of the flexible formwork with reference curvature or preload curvature. After the production of the formwork, the spacer (<xref ref-type="fig" rid="fig6">Figure 6</xref>—left) of the reinforcement was positioned and the spacer fabric was installed, fixed and stabilized (<xref ref-type="fig" rid="fig6">Figure 6</xref>—middle ). After positioning and stabilizing the textile 3D reinforcement structure from <xref ref-type="fig" rid="fig5">Figure 5</xref>, the fine concrete was laminated (<xref ref-type="fig" rid="fig6">Figure 6</xref>—right), using the adapted concrete composition displayed in <xref ref-type="table" rid="table2">Table 2</xref>.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Theoretical Verification of Major Curves</title><p>The theoretical major curves (for calculation approach cf. [<xref ref-type="bibr" rid="scirp.50807-ref12">12</xref>] ) of an asymmetrical layer structure with 0˚- and 90˚-layer content (90<sub>n</sub>/0<sub>m</sub>) are exemplarily depicted for two loading cases in <xref ref-type="fig" rid="fig8">Figure 8</xref>, dependent on the 0˚-layer content. The curves increased with increasing layer content accompanied by increasing anisotropy, both in the 1- and in the 2-axis (<xref ref-type="fig" rid="fig7">Figure 7</xref>).</p><p>The highest anisotropy was found with a relative 0˚-layer content of about 50 percent. This caused the largest</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Production test of the curved textile reinforced concrete elements: textile spacer (picture on the left), spacer fabric with textile spacer (picture on the middle), application of fine grained concrete (picture on the right)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x10.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Theoretical major curve of an asymmetrical layer structure (90<sub>n</sub>/0<sub>m</sub>), depending on the portion of 0˚-layer, with pure temperature load (ΔT = −100 K) and superimposed temperature and tensile load</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x11.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Theoretical major curve of the asymmetrical layer structure 905/06 depending on the portion of 0˚-layer, with pure temperature load (ΔT = −100 K) and superimposed temperature and tensile load</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x12.png"/></fig><p>curvature around both axes (<xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="fig" rid="fig8">Figure 8</xref>). A further increase of the 0˚-layer content caused a decrease of curvature, because the anisotropy of the GFRP layered bond structure decreased.</p><p>Due to external preload forces, the tensile load caused an increase of curvature around the 2-axis. At the same time, curvature around the 1-axis decreased, due to traction.</p></sec><sec id="s3_2"><title>3.2. Experimental Verification of Major Curves</title><p><xref ref-type="fig" rid="fig9">Figure 9</xref> displays the theoretical and experimentally verified major curves of the asymmetrical layer structure (90<sub>n</sub>/0<sub>m</sub>), depending on 0˚-layer content with a pure temperature load of (ΔT = −100 K). The major curves around the 1-axis that were determined experimentally agreed qualitatively and approximately also quantitatively with the major curve that was calculated previously (<xref ref-type="fig" rid="fig9">Figure 9</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref>0). The minor quantitative differences between the calculated and the experimentally verified major curves around the 1-axis were caused by physico-chemical reactions of the thermosetting matrices. In the calculations, these matrices could be included only insufficiently. Apart from chemical shrinkage, they included residual stress caused by swelling after increased water absorption in or among the molecular chains of the thermosetting matrices [<xref ref-type="bibr" rid="scirp.50807-ref17">17</xref>] .</p><p>In contrast to that, there are greater differences between the calculated and experimentally verified major curves around the 2-axis (<xref ref-type="fig" rid="fig9">Figure 9</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref>0). In reality however, only one of the major curves prevails, due to stability problems (problems with the transmission/distribution of forces). In this case, this is the curvature around the 1-axis.</p></sec><sec id="s3_3"><title>3.3. Polymer-Bound Stabilization of 3D-Fabric</title><p>Technique and technology from textile manufacturing had an influence on shape through coating with a thermosetting resin system. Mechanical characteristics were adapted to the variety of shapes and drapery. This resulted in an exact contour adapting (<xref ref-type="fig" rid="fig1">Figure 1</xref>1—left). Reverse deformation was less than 5 percent one day after the stabilization (<xref ref-type="fig" rid="fig1">Figure 1</xref>1—right). Thus, an exact depiction of the curvature state could be ensured.</p><p>Further production studies aimed on an additional stabilization with the cold-setting epoxy resin Indufloor-IB1240 by using of the capillary effect of the pile threads. However, it was not possible to prove an increase in stiffness of the 3D-fabric, due to the insufficient capillary effect of the spacer threads (<xref ref-type="fig" rid="fig1">Figure 1</xref>2). That</p><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Comparison between calculated and experimentally verified major curvatures at ΔT = −100 K</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x13.png"/></fig><fig-group id="fig10"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Experimentell curvature of the asymmetrical layer structure 905/06 after temperature load (ΔT = −100 K).</title></caption><fig id ="fig10_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x15.png"/></fig><fig id ="fig10_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x14.png"/></fig></fig-group><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Polymer-bound stabilization of 3D-fabrics with a thermosetting resin system: flexible 3D-fabric in curved GFRP formwork (picture on the left), stabilized 3D-fabric (picture on the right)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x16.png"/></fig><p>can be recognized on the sample “pile thread without epoxy resin contact”, which had no common quantitative characteristic peaks with the sample “epoxy resin”. As opposed to this, the sample “pile thread with epoxy resin contact” had a high quantitative and qualitative peak alignment with the sample “epoxy resin” (<xref ref-type="fig" rid="fig1">Figure 1</xref>2).</p></sec><sec id="s3_4"><title>3.4. Properties and Production Tests of Concrete Lightweight Elements</title><p><xref ref-type="table" rid="table3">Table 3</xref> shows the characteristics of fresh concrete and hardened concrete after 28 days. In the fresh concrete, an air content of 2.5% by volume and a geometrical density of 2.32 g/cm<sup>3</sup> were found by the use of an air entrainment meter. The total shrinkage deformation, measured with a shrinkage drain, was 0.71 mm/m. The compressive strength and 3-point bending tensile strength were 109.3 MPa respectively 14.74 MPa. For the textile reinforced concrete, a 3-point bending tensile strength of 41.51 MPa was measured.</p><p>Of special importance during the production tests was to ensure the evenness of the concrete layer thickness, consistently good surface quality, sufficient stability of the GFRP formwork and to avoid critical cracks both in the concrete and in the formwork system. Also essential were good sheeting qualities (<xref ref-type="fig" rid="fig1">Figure 1</xref>3).</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>The aim of this research project was to develop a flexible, multi-layered formwork system made from glass-fibre reinforced plastic, which allows for a specific adjustment of defined curvature states, utilizing the structural behavior influenced by anisotropy. The adjustment of the coupling effects, which are induced by anisotropy, was calculated in advance analytically by means of the extended laminate theory and numerically by means of the Finite Element Method. A good correspondence of the respective results for the representative shell structures was proved. An experimental verification of these intrinsic coupling phenomena has been conducted with specifically produced textile reinforced concrete-lightweight-elements. Based on the yielded results, ideal layer</p><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> Fourier transform infrared spectroscopy with attenuated total reflection for the validation of polymer-bound stabilization of 3D-fabric</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x17.png"/></fig><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Characteristics of fresh and hardened fine grained concrete after 28 days</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Characteristic</th><th align="center" valign="middle" >Fresh concrete</th><th align="center" valign="middle" >Hardened concrete</th></tr></thead><tr><td align="center" valign="middle" >geometric bulk density</td><td align="center" valign="middle" >2.32 g/cm&#179;</td><td align="center" valign="middle" >2.24 g/cm&#179;</td></tr><tr><td align="center" valign="middle" >air content</td><td align="center" valign="middle" >2.5 Vol.-%</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >linear shrinkage</td><td align="center" valign="middle"  colspan="2"  >0.71 mm/m</td></tr><tr><td align="center" valign="middle" >compressive strength</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >109.3 MPa</td></tr><tr><td align="center" valign="middle" >3-point bending tensile strength</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >14.74 MPa</td></tr><tr><td align="center" valign="middle" >CDF-Test</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >M 28 = 1172 g/m&#178; Ru, 28 = 100%</td></tr></tbody></table></table-wrap><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> Production tests of concrete lightweight elements</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810136x18.png"/></fig><p>constructions for the key curvature states and their variation range could be set. Beyond the efficient production of curved concrete-lightweight-elements, GFRP formworks employ excellent concrete qualities on highest classes of face concrete. This contributes to the generation of new forms of architecture and buildings. The intensively conducted numerical, technological and experimental tests show that combinations of concrete and stabilizing spacer fabrics permit the implementation of single and double curved, multi-axially loaded surface structures. Furthermore, the flexible GFRP formwork design allows not only a location-independent implementation of freeform surfaces following the principle “form follows form” but also results in thin-walled and thus extremely light concrete shell structures.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work was supported by the Priority Program SPP 1542 of the German Research Foundation (DFG). 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