The viscosity \(\eta\) of a glass varies with temperature according to the
relationship
$$
\eta=A \exp \left(\frac{Q_{\mathrm{vis}}}{R T}\right)
$$
where \(Q_{\text {vis }}\) is the energy of activation for viscous flow, \(A\) is
a temperature-independent constant, and \(R\) and \(T\) are, respectively, the gas
constant and the absolute temperature. A plot of \(\ln \eta\) versus \(1 / T\)
should be nearly linear, and with a slope of \(Q_{\text {vis }} / R\). Using the
data in Figure 13.7, (a) make such a plot for the borosilicate glass, and (b)
determine the activation energy between temperatures of 500 and \(900^{\circ}
\mathrm{C}\).