Hollow glass microsphere composites: preparation and properties Citation for published version (APA): Verweij, H., With, de, G., & Veeneman, D. (1985). Hollow glass microsphere composites: preparation and properties. Journal of Materials Science, 20(3), 1069-1078. https://doi.org/10.1007/BF00585751 DOI: 10.1007/BF00585751 Document status and date: Published: 01/01/1985 Document Version: Publisher’s PDF, also known as Version of Record (includes final page, issue and volume numbers) Please check the document version of this publication: • A submitted manuscript is the version of the article upon submission and before peer-review. There can be important differences between the submitted version and the official published version of record. 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If the publication is distributed under the terms of Article 25fa of the Dutch Copyright Act, indicated by the “Taverne” license above, please follow below link for the End User Agreement: www.tue.nl/taverne Take down policy If you believe that this document breaches copyright please contact us at: [email protected] providing details and we will investigate your claim. Download date: 02. Oct. 2021 JOURNAL OF MATERIALS SCIENCE 20 (1985) 1069-1078 Hollow glass microsphere composites: preparation and properties H. VERWEIJ, G. DE WITH, D. VEENEMAN Philips Research Laboratories, P.O. Box 80000, 5600 JA Eindhoven, The Nether~ands Composites consisting of bonded hollow glass m icrospheres are promising for construc- tions in which materials are needed that combine a high Young's modulus with a low density. The elastic,properties of ideally bonded hollow glass microsphere composites are predicted theoretically. Heat-treated castings of quartz glass microspheres approach the theoretical Young's modulus from below. The best result achieved was a Young's modulus of about 1 GPa with a strength of about 0.8 MPa at a density of about 180 kg m -3 . This was obtained with a casting of quartz glass microspheres, bonded with mono-aluminium phosphate. Composites made by pressing of appropriate microsphere/ binder mixtures, followed by heating, had a density that was lower than for castings but had a Young's modulus far below the theoretical value. 1. Introduction 2. Theory The present investigations were initiated by a In microsphere composites two kinds of porosity request for new construction materials with a low may be present: an intergranular porosity P1 and density and a high Yotmg's modulus. The require- an intragranular porosity P2. The total porosity is ments for the density pointed towards highly given by: porous materials. These materials can be subdivided P = PI+P2. (1) into simple foams and more complex composites such as hollow glass microsphere composites. A reasonable estimate for the intergranular Organic materials generally have a Young's porosity, P1, given random sphere packing is P1 "~ modulus that is an order of magnitude below that 0.4. This estimate is based on both experimental of inorganic materials, which makes them less and theoretical data; see for example [2]. suitable for the applications in mind. A well The intragranular porosity, P2, can be estimated known inorganic foam is the so-called foam glass from the average relative density of a thin-walled [1 ] with a Young's modulus of typically 1 GPa at a single hollow sphere, Ps, given by; density of 130kgm -a. This material has a large 4rr 3/[ 4rr 3} average bubble size of up to 2 mm and must be Ps = ~[ R3-(R-d) ] --~R ~3d/R (2) machined to make complex shapes. This may be a disadvantage for mass production applications. where R is the (outer) radius of the sphere and d is Microsphere composites of complex shape can be the wall thickness. The single sphere porosity, Ps, prepared by casting or pressing microsphere/binder is given by: mixtures followed by heat treatment. This can be accomplished with relatively cheap techniques. e~ = 1 -- 3a/R. (3) The present paper reports on the theory of elas- In a microsphere composite only a fraction f= tic properties of hollow microsphere composites (1 --P~) is occupied by spheres so that the intra- and on the preparation and mechanical properties granular porosity, P2, becomes: of some specific hollow glass microsphere compo sites. P2 = fPs = (1 --Px) (1--3d/R). (4) 0022-2461/85 $03.00 + .12 1985 Chapman and Hall Ltd. 1069 The Young's modulus, E, of a porous material e/e0 = exp (- ble,) {1 - exp [- b2(1 --Ps)]} can be estimated using various models. The discussion of this subject as given below is necess- = exp(-blP1){l--exp [-b~ (1-P)]}(I-P1)] arily brief. An extensive review of the micro- structure dependence of mechanical properties can (8) be found in [3]. using Equations 1,4, 6 and 7. A simple expression for E, based on load- Expression 8 satisfies the boundary condition bearing section arguments for a cubic pore sym- for P = 1. Disadvantages of the model behind metrically positioned inside a cube of solid expressions 6, 7 and 8 are that it is semi-analytical material, reads: and that some parameters have to be estimated. These problems can be avoided by using a model --- (1 (5) E/Eo --P2/3)/(1 _p2/3 + p), for calculating elastic properties without approxi- where Eo is the Young's modulus of the cube mations. One of the most sophisticated models for material. Expression 5 satisfies the boundary quasi-homogeneous, isotropic materials is the conditions E = Eo for P = 0 and E = 0 for P = 1 three-phase model [5, 6]. This model uses two but generally leads to values for E that are too concentric spheres of materials 1 and 2 with high. respective radii b and a, embedded in an infinite Another well-known expression, based on load- matrix of unknown effective properties. The bearing section arguments for a packing of solid radii are chosen such that (a/b)3 equals the volume spheres, is given by: fraction of material 2. An expression for the bulk modulus K and the shear modulus G is derived on = exp (- (6) E/Eo blP), the assumption that the infinite matrix possesses where b x is a characteristic exponent that depends the same average conditions of stress and strain on the way the spheres are stacked. For a simple and that all continuity conditions at the interfaces cubic packing with a coordination number of 6, are fulfilled. the value of bl is about 6. In that case the It can be proved that the solution for K is also dependence of E on P is reasonably described for the solution for a material consisting of a composite 0<~P<0.5. sphere as mentioned above, surrounded by other In a random sphere stacking a coordination composite spheres that completely fill the entire number of 6 is also present [2]. This means that a space. This is probably true for G as well, but has value of 6 for b 1 could also be used for random- not been proved. In our case material 2 is the pore stacked microsphere composites, but it should be phase. The Young's modulus, E, can be calculated noted that Expression 6 is strictly valid only for from K and G in the usual way. The full intergranular porosity. Expression 6 does not hold expression~ for K and especially G are rather for high porosities, but Rice [3, 4] has shown that lengthy, but have been described several times in a complementary relationship can be used based the literature so that we omit them here. An on a model with spherical pores in a solid matrix: interesting feature of the three-phase model is that it also yields correct estimates for E if the 1 -- exp [-- b2(1 -- P)], (7) E/Eo= pores are not spherical as long as the material where b2 is again a characteristic exponent with a remains (quasi) isotropic [6]. value of about 0.5 for a simple cubic pore distri- Hollow glass microspheres can be obtained with bution. The validity range for Equation 7 is 0.5 ~< different compositions and in various sizes. As an P~<I. example vitreous silica glass microspheres are Following Rice [4] one may combine the based on a bulk material with a relatively high models of Expression 6 and 7 to obtain an Young's modulus of 73 GPa [7] and a low density expression for hollow sphere composites. In that of 2200kgm -3 [8]. The estimated Young's case the E value of a material with intergranular modulus and density for a number of vitreous porosity P1 is predicted by Expression 6 with P = silica microsphere composites, based on the P1 while Eo in this expression is calculated from various expressions discussed, are given in Table I.
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