The Freundlich Adsorption Isotherm
Welcome to the fascinating world of Surface Chemistry! When a gas comes into contact with a solid surface, the gas molecules tend to accumulate on the surface. This phenomenon is known as adsorption. To quantify this, we use the Freundlich adsorption isotherm, which provides an empirical relationship between the quantity of gas adsorbed by a unit mass of solid adsorbent and pressure at a particular temperature.
The mathematical expression for the Freundlich isotherm is:
Here, x is the mass of the gas adsorbed, m is the mass of the adsorbent, p is the pressure, and k and n are constants that depend on the nature of the adsorbent and the gas at a given temperature.
Analyzing the Shape of the Curve
If we plot mx against pressure p, we don't get a simple straight line. The behavior changes depending on the pressure range:
1. At low pressures: The value of n1 is approximately 1. The equation becomes mx∝p1. This means adsorption increases linearly with pressure, which corresponds to the initial steep part of the curve.
2. At high pressures: The surface of the adsorbent becomes completely covered with a unimolecular layer of gas. Further increase in pressure does not increase adsorption. Here, n1≈0, making mx∝p0. The curve flattens out and becomes parallel to the pressure axis.
Because the graph must be a curve that eventually flattens, we can immediately eliminate any options that show straight lines.
The Role of Temperature
Now, let's introduce temperature into the mix. What happens to the extent of adsorption when we heat the system?
To answer this, we must look at the thermodynamics of the process. When gas molecules (which are moving freely and randomly) get adsorbed onto a solid surface, their freedom of movement is restricted. This decrease in randomness means the entropy change (ΔS) is negative. For the adsorption process to be spontaneous, the Gibbs free energy change (ΔG=ΔH−TΔS) must be negative. This is only possible if the enthalpy change (ΔH) is highly negative.
Therefore, physical adsorption is an exothermic process:
Gas+Solid⇌Gas adsorbed+Heat
According to Le Chatelier's Principle, if we increase the temperature of an exothermic equilibrium system, the system will shift in the reverse direction to absorb the added heat. In our case, the reverse process is desorption.
As we increase the temperature, the adsorbed gas molecules gain kinetic energy, overcome the weak van der Waals forces holding them to the surface, and escape back into the gaseous phase. Consequently, the extent of adsorption (mx) decreases with an increase in temperature.
Final Conclusion
Armed with this knowledge, let's evaluate the curves. For any given pressure, the curve representing the highest temperature must show the lowest amount of adsorption (it should be the bottom-most curve). Conversely, the curve for the lowest temperature will show the highest adsorption (the top-most curve).
Looking at the correct option, we see three curves:
- The top curve is at 200 K (Lowest temperature, highest adsorption).
- The middle curve is at 250 K.
- The bottom curve is at 270 K (Highest temperature, lowest adsorption).
This perfectly aligns with the principles of thermodynamics and Le Chatelier's principle, making it the correct graphical representation of the Freundlich adsorption isotherm at varying temperatures.