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ISRN Optics
Volume 2014 (2014), Article ID 802369, 5 pages
http://dx.doi.org/10.1155/2014/802369
Research Article

Wavelength Dependent Haze of Transparent Glass-Particle Filled Poly(Methyl Methacrylate) Composites

Institute of Polymer Technology, Friedrich-Alexander-University Erlangen-Nürnberg, Am Weichselgarten 9, 91058 Erlangen, Germany

Received 13 January 2014; Accepted 19 February 2014; Published 12 March 2014

Academic Editors: X. Chen and V. Matejec

Copyright © 2014 Wolfgang Wildner and Dietmar Drummer. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

Glass particles as filler were incorporated in a poly(methyl methacrylate) matrix. The refractive indexes of both materials match at a wavelength of about 400 nm. The effect of particle volume fraction on the light transmittance and light scattering (haze) in dependence of the refractive index difference was studied. The curve shape of the haze in dependence of the wavelength is comparable to that of the refractive index difference, but the base line of the haze increases with the filling grade. This indicates that there are other scattering or absorbing mechanisms, like defects in the filler binding.

1. Introduction

Particle-filled polymers are normally nontransparent. By the use of a transparent polymer as a matrix and an optical glass with a matching refractive index as filler particles, transparency can be achieved for at least one temperature and wavelength of light. These transparent composites are expected to have, compared to the bulk material, increased mechanical properties (higher stiffness, increased strengths by the use of fibers) a lower expansion coefficient and an increased thermal conductivity. In the event the particle size is one order of magnitude greaterthan the wavelength in the visible range (), the light scattering theories of Rayleigh and Mie cannot be applied. [1] First experiments on this subject have been done by Breuer and Grzesitza [2]. They analyzed a mixture between two polymers to adapt the refractive index to that of the used glass fibers. Specimens show a wavelength- (because of the different dispersion) and temperature-dependent extinction curve of the indecent light. Significant work on this subject has been carried out in Japan by the group of Kagawa. They studied the influence on light transmittance, mechanical, and thermal properties of many parameters, such as refractive index difference, particle size, particle surface area, and filler content [38]. The materials that have been investigated are an epoxy resin as a matrix and different optical glasses as filler particles. The light transmittance clearly shows the dependence of the refractive index difference because of the different dispersions of the materials. Nevertheless, the light transmittance of the compound is always less than that of the pure matrix. Waver et al. [9] investigated glass-fiber reinforced PMMA. They used optical glass as fiber material and studied the optical properties in dependence of the temperature among others. Experiments show that the temperature dependence of the polymer changes with the filling grade due to the reduced thermal expansion of the compound.

To achieve a transparent composite, a matching refractive index of filler particles and polymer matrix is necessary. The refractive index of a specific material changes with the wavelength of the incident light (dispersion) and with the temperature of the material. These two dependencies are not the same for commercial available polymers and glasses. Therefore, selected plastics and glasses have a matching refractive index only at specific wavelengths and temperatures. Many publications report investigations about the effects of the refractive index difference between filler particles and the surrounding matrix on the transmission of the compound. Despite the fact that the transmission is very important to see through the specimen, it is also necessary that the light is not distracted by the compound for a clear view. Otherwise, objects behind will appear blurry. The amount of distracted light and the haze in dependence of the refractive index difference is analyzed in this paper.

2. Experimental Procedure

2.1. Materials

As a matrix, the polymer poly(methyl methacrylate) (PMMA, Plexiglas 7N by Evonik Industries AG), and as a filler the glass “N-PK52A” (Schott AG), was chosen. This glass was selected to obtain a matching refractive index with the polymer matrix for at least one wavelength in the visible range at room temperature. Table 1 shows relevant properties of the glass and polymer.

tab1
Table 1: Properties of the materials used.

2.2. Milling of Glass and Characterization of Particles

The bulk glass was crushed with a mortar and then thieved by a sieving machine with two laboratory sieves (mesh width between 63 and 180 μm). Afterwards, the glass was cleaned with acetone to remove the small particles (μm). The glass particles were characterized by SEM images (SEM Ultra Plus type, supplier: Zeiss), and the volumetric and numeric particle-distribution was determined by the measuring instrument “Morphology” of Malvern Instruments. For each measurement of the particle distribution, at least 42000 particles were photographed and analyzed.

2.3. Fabrication of Composite

To incorporate the glass particles into the polymer matrix, the micro-compounder “HAAKE MiniLab” by Thermo Fisher Scientific Inc. was used. The processing temperature was set to 210°C. To distribute the particles evenlyin the melt, a circle mode was held up for at least 3 minutes. Subsequently, specimens (melt films) were pressed with a thickness about 250 μm and a diameter of 20 mm. The particle volume fraction was controlled by thermal gravimetric analysis (TGA) measurements.

2.4. Characterization of Optical Properties
2.4.1. Refractive Index

The refractive index of the polymer was determined with a refractometer (Abbemat WR MW by Anton Paar) which works by the total reflection method. To achieve an optical contact between the polymer and the measuring prism, the contact liquid diiodomethane with a refractive index was used. To determine whether the refractive index of the particles lies above or below the refractive index of the surrounding PMMA-matrix, the oblique illumination and the Becke line test were utilized at different wavelength under a microscope.

2.4.2. Haze

The haze of the specimens was analyzed with an UV/VIS spectrometer (Lambda 18 by Perkin Elmer Inc.). Therefore, the transmission and the light scattering of the specimens were measured in the visible range. Figure 1 shows the fundamental setup for these measurements. For transmission measurements, all the incoming light is collected by the sphere and measured by the detector (a). If a beam trap is installed at the opposite position to the opening of the sphere, only the scattered light is measured by the detector. The undistracted light beam is completely absorbed by the beam trap (b).

802369.fig.001
Figure 1: UV/VIS spectrometer with the setup for transmission measurements (a) and measurements of the scattered light (b).

The Haze was calculated using the following equation according to [10]: where is the total incoming light, is the transmission of the sample, is the scattered light of the instrument, and is the scattered light of the sample and the instrument.

To determine the haze which is only caused by the refractive index difference between matrix and particles and not by the surface of the specimen, the haze of a nonfilled specimen was subtracted from the haze of the filled specimen.

3. Results and Discussion

3.1. Particles

The numeric particle distribution is shown in Figure 2. The smallest particles which can be detected by the measuring instrument have a diameter of 2 μm. The volumetric particle distribution of the washed particles is characterized as follows: , , and . Figure 2 shows, despite sieving and washing the particles, a considerable amount of small particles (μm). Nevertheless, the volumetric amount of these particles is quite small so that they should have a minor impact on the light scattering in the specimens.

802369.fig.002
Figure 2: Numeric distribution of the unwashed and washed particles.

Figure 3 shows the appearance of the glass particles, observed by scanning electron microscopy. According to the production process, they have an irregular shape and vary in size.

802369.fig.003
Figure 3: SEM image of washed glass particles.
3.2. Specimens

Figure 4 shows a computed tomographic image (CT image) of two melt films with different filling grades. As it can be seen, the particles are uniformly dispersed in the analyzed area. According to the TGA measurements, the filler content of the specimens tested is 3.9 vol.-%, 9.4 vol.-%, and 17.3 vol.-%.

fig4
Figure 4: CT images of two specimens with a different filling grade.
3.3. Optical Properties

Figure 5 shows the measured refractive index for PMMA and the refractive index of the glass N-PK52A, according to the data sheet, depending on the wavelength. The modulus of the refractive index difference is represented by the dotted line. The refractive index of both materials is the same at a wavelength of about 400 nm. The curve progression of the polymer was calculated with the Cauchy equation (2). The constants of the polymer were calculated from the measured values: The curve progression of the glass was calculated with the Sellmeier equation (3) with constants according to the data sheet: Observations of the refractive index difference by the oblique illumination method at different wavelengths nearly confirm these measurements, Figure 6. At a wavelength of 400 nm, the particle is nearly invisible. At longer wavelengths, a shadow at the side of the particle, facing the less illuminated side of the picture, can be seen clearly. This indicates that the refractive index of the particle lies above the refractive index of the surrounding matrix.

802369.fig.005
Figure 5: Refractive index of PMMA Plexiglas 7N and glass N-PK52A at 23°C.
fig6
Figure 6: Oblique illumination in the microscope with a particle at different wavelengths.

The analysis of the transmission and the haze of the specimens were performed at a temperature of 23°C. To exclude the haze caused by the surface of the specimen, the haze of a pure PMMA sample was subtracted from the haze of the filled melt films. Figure 7 shows this calculated haze for the specimen with a filler content of 9.4 vol.-% depending on the wavelength. The relatively high scattering of the unfilled specimen is caused by its surface.

802369.fig.007
Figure 7: Intensity of transmission, scattering, and calculated haze of a specimen filled with 9.4 vol.-% glass and a thickness of 250 μm.

Figure 8 shows the haze caused by particlesfor different filling grades. It shows that the haze of the glass-filled specimens changes with the wavelength and the filler content. At the wavelength with a matching refractive index, the value of haze is lowest for all specimens. The curve shape of the haze in dependence of the wavelength is comparable to the curve shape of the refractive index difference. The absolute change of haze in dependence of the wavelength increases with higher filling grades. Nevertheless, the particle-caused haze approaches zero only for the low filler content of 3.9 vol.-%, even if the refractive indexes of the glass and the polymer match totally. The amount of scattered light at 400 nm is nearly the same for all specimens, whereas the transmission decreases with higher filling grades, in particular at short wavelengths. This leads to higher haze, according to (1). This decrease in transmission also can be seen as a slight yellow appearance of the specimens with higher filling grade. Measurements of the solution viscosity do not show an indication for aging of the material during the production process. The higher base line of the haze at higher filling grades also indicates that there are more scattering mechanisms, like defects in the filler binding. These may occur because no bonding agent is used by the making of the specimens. Further investigations will deal with this scattering and the decrease in transmission of the specimens.

802369.fig.008
Figure 8: Particle caused haze of specimens with different filling grades and a thickness of 250 μm.

4. Conclusion

The effect of the refractive index difference between a polymer matrix and glass particles as filler on the haze has been studied. The haze shows a minimum at the wavelength with matching refractive indexes and the change of haze increases with higher filling grade. However, the minimum haze is about 10% and 5% for the filling grades of 10 vol.-% and 15 vol.-%. Further work will deal with the high haze for higher filling grades and set up a relation between refractive index difference, haze, and clear view through the specimens.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

The authors gratefully acknowledge the German Research Foundation (DFG) for funding the work, the Institute of Polymer Materials for allowing the use of their micro-compounder, and the industrial partner Evonik Industries AG for providing material.

References

  1. H. C. van de Hulst, Light Scattering by Samall Particles, Dover, New York, NY, USA, 1981.
  2. H. Breuer and J. Grzesitza, “Trübungserscheinungen in zweiphasigen Polymersystemen (glasfaserverstärkte Polymere),” Die Angewandte Makromolekulare Chemie, vol. 45, no. 1, pp. 1–19, 1975. View at Publisher · View at Google Scholar
  3. Y. Kagawa, H. Iba, M. Tanaka, H. Sato, and T. Chang, “Fabrication and optical/thermal properties of glass particle-epoxy optically transparent composites,” Acta Materialia, vol. 46, no. 1, pp. 265–271, 1998. View at Scopus
  4. T. Naganuma and Y. Kagawa, “Effect of particle size on light transmittance of glass particle dispersed epoxy matrix optical composites,” Acta Materialia, vol. 47, no. 17, pp. 4321–4327, 1999. View at Scopus
  5. T. Naganuma, H. Iba, and Y. Kagawa, “Optothermal properties of glass particle-dispersed epoxy matrix composite,” Journal of Materials Science Letters, vol. 18, no. 19, pp. 1587–1589, 1999. View at Publisher · View at Google Scholar · View at Scopus
  6. H. Iba, T. Chang, and Y. Kagawa, “Optically transparent continuous glass fibre-reinforced epoxy matrix composite: fabriction, optical and mechanical properties,” Composites Science and Technology, vol. 62, no. 15, pp. 2043–2052, 2002. View at Publisher · View at Google Scholar · View at Scopus
  7. T. Naganuma and Y. Kagawa, “Effect of total particle surface area on the light transmittance of glass particle-dispersed epoxy matrix optical composites,” Journal of Materials Research, vol. 17, no. 12, pp. 3237–3241, 2002. View at Scopus
  8. H. Sato, H. Iba, T. Naganuma, and Y. Kagawa, “Effects of the difference between the refractive indices of constituent materials on the light transmittance of glass-particle-dispersed epoxy-matrix optical composites,” Philosophical Magazine B: Physics of Condensed Matter; Statistical Mechanics, Electronic, Optical and Magnetic Properties, vol. 82, no. 13, pp. 1369–1386, 2002. View at Publisher · View at Google Scholar · View at Scopus
  9. K. D. Waver, J. O. Stoffer, and D. E. Day, “Preparation and properties of optically transparent, pressure-cured poly (methyl methacrylate) composites,” Polymer Composites, vol. 14, no. 6, pp. 515–523, 1993. View at Scopus
  10. N.N., “DIN EN, 2155-9: Prüfverfahren für transparente Werkstoffe zur Verglasung von Luftfahrzeugen, Teil 9: Bestimmung der Trübung, ”, CEN, 1989.