Glasses and amorphous materials

In thermally tempered glass of thickness t = 10 mm, let y be the distance from the mid-plane; the stress follows the parabolic distribution σ(y) = σc(1 − 12y²/t²) (tension positive, σc is the tensile stress at the mid-plane). If the surface compressive stress is 120 MPa, which correctly pairs the mid-plane tensile stress σc with the depth from the surface to the end of the compressive layer?

  1. AAbout 120 MPa, about 2.1 mm
  2. BAbout 60 MPa, about 2.1 mm
  3. CAbout 60 MPa, about 2.9 mm
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Answer: B. About 60 MPa, about 2.1 mm

At the surface, y = t/2, σ = σc(1 − 3) = −2σc, so 2σc = 120 MPa gives σc = 60 MPa. The stress is zero where 12y²/t² = 1, that is, at y = t/√12 ≈ 2.89 mm, so the depth from the surface is 5.0 − 2.89 ≈ 2.1 mm (about 21% of the thickness). This distribution satisfies force balance: summed through the thickness, the stress is zero. About 2.9 mm takes the distance measured from the mid-plane as the depth from the surface. A pairing with the mid-plane tension equal to the 120 MPa surface compression does not satisfy force balance. A surface compression about twice the mid-plane tension and a compressive layer about one fifth of the thickness are the usual guidelines for thermal tempering.

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