Adsorption of a gas on a solid adsorbent follows the Freundlich adsorption isotherm. If \(x\) is the mass of the gas adsorbed on mass \(m\) of the adsorbent at pressure \(p\), and from the graph of \(\log\left(\frac{x}{m}\right)\) vs. \(\log p\) we obtain a slope of \(\tfrac{1}{2}\), then the extent of adsorption is proportional to:
Step 1: Freundlich Adsorption Isotherm \[ \frac{x}{m} = k\, p^{\,\frac{1}{n}}. \]
Step 2: Taking Logarithms \[ \log\left(\frac{x}{m}\right) = \log(k) + \frac{1}{n}\,\log(p). \] A plot of \(\log\left(\frac{x}{m}\right)\) vs. \(\log(p)\) is a straight line with slope \(\frac{1}{n}\).
Step 3: Slope Equals \(\frac{1}{2}\) If the slope is \(\frac{1}{2}\), then \[ \frac{1}{n} = \frac{1}{2} \quad \Longrightarrow \quad n = 2. \] Hence, \[ \frac{x}{m} \propto p^{\frac{1}{2}}, \] or \(\frac{x}{m} = k\, p^{1/2}\).
Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity)
Match the following: