Method Article

Artificial Thermal Ageing of Polyester Reinforced and Polyvinyl Chloride Coated Technical Fabric

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DOI:

10.3791/60737

January 29th, 2020

In This Article

Summary

Here, we simulate accelerated thermal ageing of technical fabric and see how this ageing process influences the mechanical properties of the fabric.

Abstract

Architectural fabric AF9032 has been subjected to artificial thermal ageing to determine changes of the material parameters of the fabric. The proposed method is based on the accelerated ageing approach proposed by Arrhenius. 300 mm x 50 mm samples were cut in the warp and fill directions and placed in a thermal chamber at 80 °C for up to 12 weeks or at 90 °C for up to 6 weeks. Then after one week of conditioning at ambient temperature, the samples were uniaxially tensioned at a constant strain rate. Experimentally, the parameters were determined for the non-linear elastic (linear piecewise) and viscoplastic (Bodner–Partom) models. Changes in these parameters were studied with respect to the ageing temperature and ageing period. In both cases, the linear approximation function was successfully applied using the simplified methodology of Arrhenius. A correlation was obtained for the fill direction between experimental results and the results from the Arrhenius approach. For the warp direction, the extrapolation results exhibited some differences. Increasing and decreasing tendencies have been observed at both temperatures. The Arrhenius law was confirmed by the experimental results only for the fill direction. The proposed method makes it possible to predict real fabric behavior during long term exploitation, which is a critical issue in the design process.

Introduction

Polyester based architectural fabrics are commonly used for construction of hanging roofs1. Being relatively cheap with good mechanical properties, they can be employed in long-term exploitation (e.g., the hanging roof of the Forest Opera in Sopot - Poland). Unfortunately, weather conditions, ultraviolet radiation, biological reasons, and operational purposes (season pre-stressing and loosening2) can affect their mechanical properties. Hanging roofs made of AF9032 are typically seasonal structures subjected to high temperature (especially during sunny days in the summer), regular pre-tensioning and loosening. In order to properly design a hanging roof, fabric parameters must be determined not only at the beginning of exploitation, but also after several years of use.

Ageing analysis measures the ageing indicator and compares the initial and final values of the parameters to assess the impact of ageing. Cash et al.3 proposed one of the simplest methods by comparative analysis of 12 different types of roofing membranes. These membranes were exposed to outdoor weathering for 2 or 4 years. The authors used a rating system of several properties to assess fabric durability. In order to provide an analysis of polymer thermal ageing, the time-temperature superposition principle (TTSP) can be applied4. This principle states that the behavior of a material at low temperature and under low strain level resembles its behavior at high temperature and high strain level. The simple multiplicative factor can be used to relate the current temperature properties with the properties at the reference temperature. Graphically, it corresponds to the curve shift on the log time scale. Regarding the temperature, two methods are proposed to combine the shift factor and the ageing temperature: the Williams-Landel-Ferry (WLF) equations, and the Arrhenius law. Both methods are included in the Swedish standard ISO 113465 to estimate the lifetime and maximum operational temperature for rubber, or vulcanized and thermoplastic, materials. Recently, thermal ageing and Arrhenius methodology have been used in the cable lifetime prediction6,7, heating pipes8, and polymer glue PMMA4. An extension of the Arrhenius law is the Eyring law that takes into account other ageing factors (e.g., voltage, pressure, etc.)9. Alternatively, other studies propose and verify simple linear models for a description of ageing (e.g., biosensor ageing10). Although the Arrhenius method is commonly used, there is discussion on its relevance in the lifetime prediction of every material. Hence, the method must be used with care, especially in terms of initial assumptions and experimental conditions6.

Similar to most polymers, the polyester fabrics used in the current research exhibit two distinct transition phases defined by the melting temperature (Tm) and the glass transition temperature (Tg). The melting temperature (Tm) is the temperature when a material changes from its solid state to the liquid one, and the glass transition temperature (Tg) is the boundary between the glass and rubber states11. According to manufacturer's data, the AF9032 fabric is made from polyester threads (Tg = 100−180 °C12, Tm = 250−290 °C13) and PVC coating (Tg = 80−87 °C14,15, Tm = 160−260 °C16). The ageing temperature Tα should be selected below Tg. During sunny days, the temperature on the top surface of a hanging roof may even reach 90 °C; thus, two ageing temperatures (80 °C and 90 °C) are tested here. These temperatures are below the thread Tg and close to the coating Tg.

The performance of the accelerated ageing protocol on technical fabrics is presented in the current work. Artificial thermal ageing is used to predict changes of the material properties. The article illustrates appropriate laboratory testing routines and a way to extrapolate relatively short-term experimental results.

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Protocol

1. Accelerated thermal ageing experiments on technical fabric

  1. Overall preparation
    1. Prepare a testing machine with proper software (in order to provide constant strain rate tests) and a video extensometer.
    2. Prepare a thermal chamber providing constant temperature of 80 °C (± 1 °C) and 90 °C (±1 °C) for at least 12 weeks.
  2. Specimen preparation
    1. Unroll the technical fabric AF9032 bale. Draw the desired shapes (300 mm x 50 mm) with a soft pencil or marker on the fabric surface parallel to the warp or fill direction.
      NOTE: The distribution of specimens on the fabric surface is given elsewhere17.
    2. Indicate the warp direction on each specimen with a permanent marker. Cut the specimens with a sharp knife or scissors. Use the ruler if a knife is used for cutting.
      NOTE: The specimens should be rectangular17. The major load-caring elements of the fabric are threads. In the operational phase, the coating material usually exceeds its yield limit, thus not taking part in the stress distribution. The only elements to carry the load are threads spreading from one grip to another. Therefore, it is not reasonable to use sophisticated shapes of specimens (e.g., a dumbbell shape usually used for metals). On the other hand, such sample shapes result in the need for special grips when the ultimate load is investigated, or the use of an extensometer in order to assess material parameters.
    3. Measure the specimen's thickness with a slide caliper and count the number of threads at the short edge of the specimen.
      NOTE: For each specimen, take three thickness measurements, and compute the average value. Use the magnifying glass to assess the number of threads if necessary.
  3. Turn on the thermal chamber, leaving the door open. Using the buttons and the control display, select the temperature (80 °C). Close the thermal chamber door and observe the increase of temperature on the control panel.
  4. Specimen warming
    1. When the temperature is close to 80 °C, open the thermal chamber door. Insert at least 7 sets of specimens with each set consisting of 6 specimens cut in the warp direction and 6 in the fill direction. Close the door as soon as possible in order to avoid a temperature drop.
      NOTE: The experiments should be conducted for three strain rates. For each strain rate, experiments are performed on two specimens in the warp direction and two in the fill direction. Place excess specimens in the chamber in case the experiments are not successful or the results from both tests are highly divergent.
    2. After 1 h, don thermal gloves and remove the first set of specimens (the reference set; 6 specimens in the warp direction and 6 in the fill direction). After every 2 weeks, remove a succeeding set of specimens from the thermal chamber.
      NOTE: The entire warming process will take 12 weeks.
  5. Specimen conditioning
    1. Leave the specimens at room temperature for one week. Cool the specimens to room temperature (i.e., their properties should be stabilized).
    2. Before the test, draw two black marks (dots) using a permanent marker with a lengthwise separation of about 50 mm (L0) in the middle of each specimen.
      NOTE: The dots will be used by the video extensometer.
  6. Testing machine setup
    1. Install four 60 mm flat inserts into the testing machine, two inserts per one grip. The inserts show a fish scale surface type and are used to avoid slipping the specimens out of the grips.
    2. Switch on the machine. Start the software (e.g., TestXpert) that controls the machine. Choose the program dedicated to the tensile tests.
    3. Select the starting position with a 200 mm grip to grip separation in the software. Click the Starting Position button to execute the 200 mm grip to grip separation. This grip position is usually called the starting position for a test.
      NOTE: The 200 mm distance is required by the ISO standard17.
  7. Video extensometer setup
    1. Move the camera of the video extensometer along the supporting bar to situate the lens of the camera at the level of the middle part of the specimen. Check whether the lens of the camera provides a clear view of the specimen markers during the whole experiment.
      NOTE: Perform a similar test before the main test to establish the probable sample elongation range to ensure that the camera will follow the black markers during an entire test.
    2. Select the proper brightness and focus for the lens using the computer screen and the associated software.
  8. Video extensometer calibration
    NOTE: The calibration device is the standard equipment of the video extensometer.
    1. Put the calibration device in the front of the camera and clamp it with the grips.
    2. Using the video extensometer software (e.g., VideoXtens), select the proper type of markers in the Targets window (usually black and white).
    3. Select the calibration procedure in the video extensometer software using the Scale option and choose the calibration distance in the Scale window.
      NOTE: The distance should be similar to the separation of markers on the specimens. The calibration device offers three measuring distances: 10, 15 and 40 mm. Due to the 50 mm marker separation, the 40 mm distance is appropriate.
    4. After calibration, change the marker type to Pattern in the Targets window.
      NOTE: This enables the video extensometer to follow the markers indicated on the specimen.
  9. Test performance
    1. Prepare the test parameters in the TextXpert software.
      NOTE: The prepared program must enable a test with a selected strain rate in the uniaxial stress case. It must be correlated with the video extensometer. The recorded parameters are the initial distance of the extensometer markers (L0), and result functions of time, grip displacements, current extensometer's markers distance, and force. The pre-load force of 50 N17 is programmed and the L0 distance is adjusted after preloading.
    2. Put the specimen along the machine main vertical axis and close the grips using the tubular spanner.
      NOTE: The specimen must be located symmetrically to the grips in the vertical and horizontal directions.
    3. Perform the tests with the selected constant strain rate until the specimens break (use 0.005, 0.001, and 0.0001 s-1 strain rates). For each strain rate, test at least two specimens in the warp direction and fill direction. Save the test results.
      NOTE: The following data are necessary: the initial distance of the extensometer markers (L0), time functions of the extensometer's marker distance, and the force.
  10. Repeat steps 1.5−1.9 every two weeks using the other sets of samples (six times, up to 12 weeks).
  11. Repeat the entire procedure at 90 °C. The total number of specimens does not change. The ageing process lasts 6 weeks. Remove and test subsequent sets of specimens every week.

2. Data preparation

  1. Knowing the cross section area of the samples, use graphing software (SigmaPlot18 or similar) to recalculate the registered force and elongation increments according to elementary strength of material equations to the stress-strain relations. Plot a graph of obtained data, separately, for the warp and fill samples and for each of the strain rates.
  2. Repeat for the 80 °C and 90 °C results.

3. Parameter identification of material models

  1. Piecewise linear model for non-linear elastic modeling
    NOTE: The application of the piecewise linear material model is possible when the stress-strain curve can be split into sections of linear (or approximately linear) shapes. Particular crossing points of the lines at neighboring sections correspond to applicability ranges of the related lines19.
    1. In the case of every curve obtained in step 2.1, find the strain ranges, detecting the linear or close to linear stress-strain relation.
    2. Using the fit regression option in the graphing software and the least square method, identify the best-fit line in the chosen region.
      NOTE: The tangent to this curve corresponds to the stiffness of the material in a particular range.
    3. Denote the tangent as Eij where the index i corresponds to the current direction of the material (W for the warp direction and F for the fill direction) and the index j is a consecutive number of the identified line.
    4. Having parameters of all the lines, find the intersection points between the lines; denote them as εk/l, where k and l mark the crossing lines.
      NOTE: These points (εk/l) constitute the strain ranges to apply the particular longitudinal stiffness values (Eij) (Figure 1).
  2. Bodner–Partom viscoplastic model
    NOTE: The Bodner–Partom constitutive law is used to reflect the elasto-viscoplastic behavior of various materials20,21. The basics and mathematical formulation of the model is given in detail elsewhere20,21,22,23,24,25. The elementary equations are presented in Table 1 only to model the uniaxial stress state. The Bodner–Partom model parameters are identified by means of the uniaxial tensile tests conducted with at least three different strain rates. The value of the strain rate must be constant at least in the inelastic part of the experiment. The complete Bodner–Partom model identification procedure modified for technical woven fabrics is widely presented24,25.
    1. Using the graphing software, identify Bodner–Partom model parameters following Klosowski et al.24.

4. Arrhenius extrapolation

NOTE: The Arrhenius law is based on an empirical observation that ambient temperature increase results in acceleration of a number of chemical reactions that may speed up the ageing process as well. The complete mathematical representation of the Arrhenius chemical reaction concept can be found elsewhere11,26. The Arrhenius law in a simplified form is called "the 10 degree rule"27. According to this rule, a surrounding temperature increase of about 10 °C theoretically doubles the rate of the aging process. Hence, the reaction rate f is defined as follows17:

Formula for frequency change, f=2ΔT/10, described in a mathematical context.

where ΔT = T - Tref is the difference between the ageing temperature T and the service temperature Tref of a material.

  1. Assume the temperature Tref according to the average value based on the results of the local meteorological station (here, Tref = 8 °C28). Assume the thermal chamber temperature T to be used in the ageing test (here, 80 °C and 90 °C).
    NOTE: The temperature level should be registered for a longer time period, at least one year, and then calculated as the mean value of that period, bringing a time average of this period taken as Tref.
  2. Calculate the reaction rate constant f from equation 1 and then extrapolate the ageing time (expressed in weeks) to years (Table 2).
    NOTE: The extrapolation effects of different ageing time periods conducted within the current research are presented in Table 3. For instance, thermal ageing of a specimen in 4 weeks at 90 °C is equal to its ageing in 8 weeks at 80 °C and corresponds to a natural ageing of approximately 23 years.

5. Data representation

  1. Present the obtained parameter values in the normalized form of X/X0, where X denotes a current value of the certain parameter and X0 corresponds to the initial value of this parameter, with regard to a specimen aged 1 hour only.
    NOTE: The time of artificial thermal ageing is set up in hours.
  2. Plot X/X0 values on the Y axis versus the ageing time plotted on the X axis to show the evolution of the parameters. Prepare plots for the warp and fill directions of the tested material separately.
  3. Describe the parameter values plotted over time by linear functions (or different best-fit functions) using the least square method and report R2 values.
  4. To evaluate whether the Arrhenius simplified relation is correct for AF9032 fabric, redraw the results obtained for 90 °C with respect to the ageing time recalculated into "real" time according to the Arrhenius law.

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Results

Figure 2 juxtaposes the stress-strain curves for the warp and fill directions of AF9032 fabric obtained at different ageing times, in the 80 °C temperature level for a strain rate of 0.001 s-1. The difference between the 1 h ageing period (reference test) and the rest of the ageing periods is clear. The ageing time does not seem to substantially affect the material response in the warp direction, as the stress–strain curves are highly repetitive, showing no important differences i...

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Discussion

This article incudes a detailed experimental protocol to simulate the laboratory accelerated experiments on polyester reinforced and PVC coated fabrics for civil engineering applications. The protocol describes the case of artificial thermal ageing only by the means of raising the ambient temperature. This is an obvious simplification of real weather conditions, as UV radiation and water influence play an additional role in material service ageing.

Generally, the conditions of accelerated agei...

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Disclosures

The authors have nothing to disclose.

Acknowledgements

The publication of this work was supported by the Faculty of Civil and Environmental Engineering at Gdansk University of Technology.

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Materials

List of materials used in this article
NameCompanyCatalog NumberComments
AF 9032 technical fabricShelter-Rite Seaman Corporation
knife of scisors
markerpernament
ruler
Sigma PlotSystat Software Inc.v. 12.5
Testing machine Z020Zwick RoellBT1-FR020TN.A50
TestXpert II programZwick Roellv. 3.50
Thermal chamberEurotherm Controls2408
tubular spanner13 mm
Video extensometerZwick RoellBTC-EXVIDEO.PAC.3.2.ENInstead of video extensometer, a mechanical one can be used
VideoXtensZwick Roell5.28.0.0 SP2

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Accelerated AgeingArrhenius MethodTensile TestingVideo ExtensometerBodner Partom ModelStress Strain AnalysisThermal ChamberConstant Strain Rate

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