Circumferentially Adhesive Bonded Glass Panes for Bracing Steel Frames in Façades Edwin M.P. Huveners Bouwstenen 135 ISBN 978-90-6814-621-9 Cover design by Ton van Gennip Printed by University Press Facilities, Eindhoven University of Technology, the Netherlands Copyright © 2009 Edwin M.P. Huveners Circumferentially Adhesive Bonded Glass Panes for Bracing Steel Frames in Façades PROEFSCHRIFT ter verkrijging van de graad van doctor aan de Technische Universiteit Eindhoven, op gezag van de rector magnificus, prof.dr.ir. C.J. van Duijn, voor een commissie aangewezen door het College voor Promoties in het openbaar te verdedigen op donderdag 3 december 2009 om 16.00 uur door Edwin Michel Pierre Huveners geboren te Maastricht Dit proefschrift is goedgekeurd door de promotoren: prof.ir. F. van Herwijnen en prof.ir. F. Soetens Copromotor: dr.ir. H. Hofmeyer Samenstelling promotiecommissie: prof.ir. J. Westra TU Eindhoven (voorzitter) prof.ir. F. van Herwijnen TU Eindhoven prof.ir. F. Soetens TU Eindhoven dr.ir. H. Hofmeyer TU Eindhoven univ.-prof.dr.-ing. G. Siebert Universität der Bundeswehr, Munich, Germany prof.dr.ir. J. Rots TU Delft dr.ir. L.J. Govaert TU Eindhoven dr.-ing. F. Wellershoff Permasteelisa Central Europe GmbH, Würzburg, Germany Acknowledgements This thesis is the product of seven years part-time research with the last year even full-time to complete the job. Many people supported, encouraged and stimulated me during these years and this is my opportunity to thank them all and in particular the following persons below. First of all, I would like to express my sincere gratitude to my promoters Frans van Herwijnen and Frans Soetens for supervising this research work and their support. I profoundly appreciate their comments, valuable remarks and suggestions throughout the duration of this project. I owe a special depth of gratitude to Herm Hofmeyer, my copromotor. He kept a bird- eye's view on the research project. He supported me by the design of the experiments and the finite element models, and he has advised me to clarify the mechanical models. The other members of the committee are also acknowledged for their comments, valuable remarks and suggestions on the draft version of this thesis. A lot of time was spent to carry out the experiments in the Pieter van Musschenbroeck Laboratory at Eindhoven University of Technology. I would like to thank Hans Lamers for also giving a short course about polymers, Theo van de Loo and in particular Martien Ceelen, he was my help and stay through out the years. In this research, there was also a need for assistance of other laboratories. I really appreciate the hospitality of Leon Govaert of the section Polymer Technology of the department of Mechanical Engineering for using their testing apparatus and Peter Cappon of the unit Building Physics and Systems of the department Architecture, Building and Planning for using their chemical laboratory. I thank all my colleagues at Eindhoven University of Technology, unit Structural Design and Construction Technology for having a great time. I would like to thank Johan van den Oever for helping me with all my computer problems and Mark Wolffe for adding books about structural glass to the collection in our library. Many students I guided with master and graduate projects related to my research project. I would like to thank them all and in particular Bas Koggel who graduated successfully in 2006. I would like to thank for supplying testing materials and guidance during my research in particular Theo Rögels of Scheuten Glasgroep in Venlo and Berrie Roelofs of Sika Netherlands in Utrecht. I would like to express my great gratitude to Anton Tapper of Façade Consulting & Engineering in Eindhoven for his advices. During the first 5 years I also worked part-time as structural designer at the engineering office Volantis in Maastricht. I returned to Volantis in May 2009. I would like to thank all my colleagues for their support and in particular Bert Schepers. Last, but not least, I would like to thank my parents Pierre Huveners and Corrie Huveners- Valkenhoff van Doorn, my uncle Michel Huveners and my partner Kristel Tijssens. Edwin Huveners Eindhoven, October 2009 i ii Circumferentially Adhesive Bonded Glass Panes for Bracing Steel Frames in Façades Summary Contemporary architecture desires large glass surfaces in the building envelop with a minimum of non transparent members such as steel braces needed for the stability of a building. Glass panes have the capacity to resist in-plane loads and can replace the steel braces of a one-storey building. The vertical stability system of a building is a primary structural component and has to comply with strength (safety) and building stiffness (serviceability). A circumferentially adhesive bonded joint is a suitable connection to introduce in-plane loads into the glass pane. For the research three joint types have been defined. Joint type 1 is a flexible adhesive bonded joint (polyurethane) across the full thickness of the glass pane. Joint type 2 is a two-sided stiff adhesive bonded joint (epoxy) along the edges of the glass pane. Joint type 3 is a one-sided stiff adhesive bonded joint (epoxy) along the edges of the glass pane. The steel frame, the single annealed glass pane and one of the three joint types form the system which is only subjected to a horizontally concentrated in-plane load at the top of the system. The objective of the research is to get more insight in the structural behaviour of these systems and to set-up mechanical models and possibly design rules. The research methodology consisted of experiments, finite element simulations and parametric studies. The experiments were carried out with square glass pane sizes of 1.0 m with nominal glass pane thickness of 12 mm. Systems with joint type 1 had a very small in-plane stiffness of the system, a glass-steel contact at large horizontal in-plane displacements at the top of the system and a good residual capacity, namely large horizontal in-plane displacements at the top of the system with increasing horizontal in-plane load. Systems with joint type 2 had much larger in- plane stiffness of the system than systems with joint type 1. The residual capacity was very good, because the horizontal in-plane load kept increasing after the first and following glass cracks. Systems with joint type 3 had slightly smaller in-plane stiffness of the system than systems with joint type 2. The residual capacity after the first glass breakage was very poor. One finite element model for systems with joint types 1 to 3 was developed and calibrated with experiments. The results of the finite element simulations matched well with the results of experiments till the onset of the first crack in the glass pane or till the glass-steel contact for systems with joint type 1. The parametric studies only focused on the variation of the thickness, the width and the height of the glass pane. For systems with joint type 1, the in-plane stiffness of the system depends on the width-height ratio of the glass pane and the stiffness of the adhesive bonded joint. Systems with the rectangular glass panes have two glass-steel contacts at increasing horizontal in-plane displacements at the top of the system. Besides the stiffness criterion for vertical stability systems of buildings the normal strain rate and the shear strain rate can also be a criterion. For systems with joint type 2 and 3, the in-plane stiffness of the system is determined by the width- height ratio and the thickness of the glass pane. The maximum principle (tension) stress in the glass pane rapidly increases at the vicinity of the corners in which the ‘tension diagonal’ is iii anchored, caused by the difference in in-plane displacements between the stiff adhesive bonded joint and the bolted connection between the outside beam and the beadwork of the steel frame. Moreover, for systems with joint type 3, the eccentric load transfer between the steel frame and the glass pane results in bending of the glass pane. The mechanical models for systems with joint type 1 well predict the in-plane stiffness of the system, the largest maximum principle (tension) stress in the glass pane and the maximum normal and shear stresses in the adhesive bonded joint. The criteria were the limitation of the horizontal in-plane displacement at the top of the system or the limitation of the strain rates of the adhesive bonded joint. For the residual capacity, the mechanical models also predict well the horizontal in-plane load and the horizontal in-plane displacement at the top of the system at the first glass-steel contact. For systems with joint type 2 and 3, no mechanical models were developed, because the very stiff adhesive bonded joint and the very small in-plane displacements of the bolted connection between the outside beam and the beadwork of the steel frame resulted in a complex stress distribution along the edges of the glass pane as well as in the adhesive bonded joint. A range of several shear stiffnesses of the adhesive bonded joint has been presented which has a positive influence on the distribution of the principle stresses in the glass pane as well as the normal stresses and shear stresses in the adhesive bonded joint without losing of the in-plane stiffness of the system. Glass panes as bracing elements in steel frames have a great potential. For systems with joint type 1, all glass panes have to be structurally bonded to the steel frame of the façade to guarantee the stability of the building because of the small in-plane stiffness. The residual capacity is good, because the horizontal in-plane load increases at overloading. Furthermore, the large horizontal in-plane displacements of the building visually warn for overloading. For systems with joint types 2 and 3, few bays in the façade are sufficient to guarantee the stability of the building by the larger in-plane stiffness. However, systems with joint type 2 produced the best results for a transparent vertical stability system for buildings because of the residual capacity at overloading. The applied epoxy adhesive behaved too stiff and therefore, it is recommended a range of several shear stiffnesses for the adhesive bonded joint for systems with joint type 2 which more favourably loads the glass pane as well as the adhesive bonded joint without a reduction of the in-plane stiffness of the system. iv
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