People | Locations | Statistics |
---|---|---|
Naji, M. |
| |
Motta, Antonella |
| |
Aletan, Dirar |
| |
Mohamed, Tarek |
| |
Ertürk, Emre |
| |
Taccardi, Nicola |
| |
Kononenko, Denys |
| |
Petrov, R. H. | Madrid |
|
Alshaaer, Mazen | Brussels |
|
Bih, L. |
| |
Casati, R. |
| |
Muller, Hermance |
| |
Kočí, Jan | Prague |
|
Šuljagić, Marija |
| |
Kalteremidou, Kalliopi-Artemi | Brussels |
|
Azam, Siraj |
| |
Ospanova, Alyiya |
| |
Blanpain, Bart |
| |
Ali, M. A. |
| |
Popa, V. |
| |
Rančić, M. |
| |
Ollier, Nadège |
| |
Azevedo, Nuno Monteiro |
| |
Landes, Michael |
| |
Rignanese, Gian-Marco |
|
Maoult, Yannick Le
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (37/37 displayed)
- 2022Numerical Simulation of Recycled PET Preforms Infrared Heating Including Force Convection Effect in the Industrial ISBM Ovens
- 2022Infrared heating modeling of recycled PET preforms in injection stretch blow molding processcitations
- 2021Effect of oxidation on spectral and integrated emissivity of Ti-6Al-4V alloy at high temperaturescitations
- 2018On the thermal sensitivity and resolution of a YSZ:Er 3+ /YSZ:Eu 3+ fluorescent thermal history sensorcitations
- 2018The role of microcrystalline structure on optical scattering characteristics of semi-crystalline thermoplastics and the accuracy of numerical input for IR-heating modelingcitations
- 2017A non-invasive experimental approach for surface temperature measurements on semi-crystalline thermoplasticscitations
- 2017Industrial applications of the superplastic forming by using Infra-Red heatercitations
- 2017Novel erbia-yttria co-doped zirconia fluorescent thermal history sensorcitations
- 2016Experimental analysis on the coupled effect between thermo-optical properties and microstructure of semi-crystalline thermoplasticscitations
- 2016Infrared welding process on composite: Effect of interdiffusion at the welding interfacecitations
- 2016Infrared radiation applied to polymer processescitations
- 2016Titanium Superplastic Forming by Aurock: A Complete Integrated Solution from CAD File to Final Part
- 2016Identification of the temperature dependent relation between thermo-optical properties and morphology of semi-crystalline thermoplastics for thermoforming process
- 2016Effect of the developed temperature field on the molecular interdiffusion at the interface in infrared welding of polycarbonate compositescitations
- 2016Infrared Radiation applied to Blow Molding and thermoforming
- 2014Optimized sol–gel thermal barrier coatings for long-term cyclic oxidation lifecitations
- 2014Feasibility of luminescent multilayer sol-gel thermal barrier coating manufacturing for future applications in through-thickness temperature gradient sensingcitations
- 2013Innovative Superplastic Forming Based on In-Situ Infra-Red Sheet Heatingcitations
- 2012Superplastic forming of AZ31 magnesium alloy with controlled microstructurecitations
- 2011Infrared heating stage simulation of semi-transparent media (PET) using ray tracing methodcitations
- 2011Simulations of an Infrared Composite Curing Processcitations
- 2011Infrared curing simulations of liquid composites moldingcitations
- 2010Oxidation and spallation of FeCrAl alloys and thermal barrier coatings: in situ investigation under controlled temperature gradientcitations
- 2010Evolution de la microstructure et influence de la pollution atmosphérique lors de la mise en oeuvre d'une résine thermodurcissable
- 2010Advances in the field of new smart thermal barrier coatings
- 2008Direct obervations and analysis of the spallation of alumina scales grown on PM2000 alloycitations
- 2008TOWARDS SUPERPLASTIC FORMING OF AZ31 MAGNESIUM ALLOY WITH CONTROLLED MICROSTRUCTURE
- 2007Measurement of thermal contact resistance between the mold and the polymer for the stretch-blow molding processcitations
- 2004Experimental and numerical infrared heating of thermoplastic sheet during thermoforming process
- 20043D finite element modeling of the blow molding process
- 2003Heat conditioning modelling of thermoforming process: comparison with experiments
- 2003Modelling of infrared heating of thermoplastic sheet used in thermoforming processcitations
- 2002Infrared Heating Modeling of Thermoplastic Sheets in Thermoforming Process
- 2001Comparison between a numerical model and an experimental approach of preform infrared radiative heating-recent results
- 2001Recent Issues In Preform Radiative Heating Modelling
- 2001Comparison Between a Numerical Model and an Experimental Approach of Preform Infrared Radiative Heating – Recent Results
- 2000Analysis of influent parameters during infrared radiative heating of PET preform
Places of action
Organizations | Location | People |
---|
document
3D finite element modeling of the blow molding process
Abstract
The stretch blow molding process of PET bottles is a two-step process. First, a cold tube-shape preform is heated using an infrared oven above PET glass transition temperature (about 80°C) in order to reach the forming temperature. The softened preform is then simultaneously stretched and inflated with a rod and air pressure. The final wall thickness of the bottle is both related to heating parameters as well as stretch blow molding ones. It leads to a complex thermo-mechanical problem for which specific numerical models must be developed. In this work, a complete 3D finite element modeling of the stretch blow molding process has been developed including both infrared heating and forming steps. The energy transfer between the infrared oven and the irradiative surface of the preform is modeled using a ray tracing method. In the same time, the amount of radiation intensity absorbed by the polymer is approximated with a Rosseland model. Owing to that, the radiation heat transfer results in a pure conductive heat transfer. All the thermal computations will be compared to the so-called PLASTIRAD control volume software [MON2001] and to a temperature analytical model. Considering the deformation step, a Mooney-Rivlin hyperelastic model has been implemented in Forge3® software in order to account for the PET rheological behavior. The numerical model is developed using a velocity pressure formulation and P1+/P1 tetrahedral finite elements. In order to validate the hyperelastic behavior, computations are compared to a Mooney-Rivlin analytical model of a free inflation tube. This model enables to obtain the tube internal radius versus a given pressure on the internal surface.