The reaction that converts cis-1,2-difluoroethene to trans-1,2-difluoroethene provides a simple example for thinking about equilibrium on the molecular level.
This reaction does not occur at room temperature because it requires breaking the carbon-carbon π bond. But at 615 K (and assisted by a catalyst), 1 mole of cis-1,2-difluoroethene will transform into an equilibrium mixture of ⅔ mole cis isomer and ⅓ mole trans isomer. From a macroscopic point of view, it may appear that the reaction stops once equilibrium is attained, but on the microscopic level, such a statement is untrue.
As cis-1,2-difluoroethene molecules move around in a container at 615 K, energy is constantly being transferred from one molecule to another as they collide. This yields a distribution of kinetic energies, and at any single point in time, a small fraction of cis-1,2-difluoroethene molecules have sufficient energy to convert to the trans isomer. We can think about this pictorially using a reaction energy diagram, which is a diagram that shows energy as a function of reaction progress.
As one end of the molecule rotates relative to the other, energy increases because the π bond is partially broken. When the angle of rotation reaches 90°, the π bond is completely broken. Once the angle exceeds 90°, a new π bond begins to form and the molecule’s energy decreases. Finally, when the angle of rotation is 180°, the new π bond is completely formed and the molecule’s energy has decreased to almost the same value it was initially. (If a molecule does not have energy higher than the highest energy point in the reaction energy diagram, the reaction cannot occur.)
This cis to trans conversion process does not stop when equilibrium has been attained at 615 K. There are still plenty of cis-1,2-difluoroethene molecules present in the equilibrium mixture, and they have the same kinetic energy distribution. Hence, a fraction of them continues to convert to the trans isomer.
If this were the only reaction taking place, the eventual result would be that all the cis isomer would be converted to the trans isomer. This does not happen because the reverse reaction is also occurring at the same time. The trans-1,2-difluoroethene molecules, once formed, also have a distribution of kinetic energies, a fraction of which have sufficient energy to convert back into the cis form. Thus cis-1,2-difluoroethene molecules are not only being consumed but are also being produced.
Once equilibrium has been reached, the concentration of cis-1,2-difluoroethene remains constant because the rate at which they are being consumed is exactly balanced by the rate at which they are being produced. In other words, for every cis molecule that converts to the trans isomer, there will be, on average, a molecule of trans isomer converting back to the cis isomer. This constant reshuffle of molecules between reactant (cis-1,2-difluoroethene) and product (trans-1,2-difluoroethene) continues indefinitely without any net change in the concentration of either species.
In this dynamic chemical equilibrium, if you can follow one specific molecule over time, you will find the molecule bouncing around and colliding with other molecules quite a bit. More importantly, sometimes the molecule is in the trans form and other times the molecule is in the cis form.
If we follow this molecule for a while, we would find that, on average, it spends ⅓ of the time in trans form and ⅔ of the time in cis form. This is true for every molecules in the equilibrium mixture. Therefore, at any given moment in time, we will find a mixture in which ⅓ of the molecules are trans-1,2-difluoroethene while the other ⅔ are cis-1,2-difluoroethene. The ratio of product to reactant will be 1:2, as measured experimentally.
Why is this case? The reason is that the trans isomer is higher in energy than the cis isomer. The change in Gibbs free energy, ΔrG°, for the reaction is positive:
On average, a molecule will spend more time in the lower Gibbs free energy form (cis-1,2-difluoroethene) than the higher free energy form (trans-1,2-difluoroethene).
Looking at the Figure: Reaction Energy Diagram above, we see that it is the free energy difference between the reactant and product that dictates their ratio at equilibrium. The highest energy point in the reaction energy diagram dictates how much time it takes for equilibrium to establish, a topic that we will discuss in more detail in a later unit.
Let’s consider again the nitrogen dioxide reaction, which involves two reactant molecules:
The sign of ΔrG° tells us that the product of this reaction is lower in free energy than the reactant at 298 K.
At 298 K, a sizable fraction of NO2 molecules has sufficient energy to react. If two such NO2 molecules collide with the N atoms facing each other, allowing for the formation of a N-N bond, a N2O4 molecule will form. As the reaction proceeds toward equilibrium, the concentration of NO2 decreases while the concentration of N2O4 increases. A fraction of these newly formed N2O4 molecules will have sufficient energy for the reverse reaction to occur, thereby producing NO2 molecules. When the equilibrium is reached at 298 K, the reaction vessel contains 70% N2O4 and 30% NO2.
Both the forward and reverse reaction continues to occur after equilibrium has been established. If you can follow one specific NO2 molecule inside the equilibrium mixture over time, you will find it bouncing around and colliding constantly. A specific collision with another NO2 molecule would lead to the formation of a N2O4 molecule. This N2O4 molecule continues to move and collide, and a collision may impart sufficient energy for it to fall apart into two separate NO2 molecules, one of which is the original NO2 molecule we were following. If we follow the NO2 molecule for a while, we would find that, on the average, it spends 70% of the time as a part of a N2O4 molecule and 30% of the time as a free NO2 molecule.
By simply examining this reaction via the Lewis structures of reactant and product, we can see that this reaction has a negative ΔrH°: a N-N bond is formed and no bonds are broken (both the reactant and product molecules have important resonance structures):
This reaction also has a negative ΔrS° because two separate gaseous reactant molecules are combining to form a single gaseous product molecule. There is a loss of freedom of motion because a N2O4 molecule has to move as a whole while two separate NO2 molecules can move independently.
Therefore, compared to the cis–trans isomerization example, entropy plays a more important role in this reaction. In the forward direction, this is an exothermic reaction with a decrease in entropy. At temperatures above 52 °C, the magnitude of TΔrS° term becomes larger than the magnitude of the ΔrH° term, and the reaction becomes reactant-favored as the ΔrG° becomes positive (Gibbs free energy of the product becomes higher than Gibbs free energy of the reactant).
In other words, if the 2 NO2(g) ⇌ N2O4(g) reaction occurred at a higher temperature, for example at 75 °C, the equilibrium mixture would contain more NO2 molecules (~75%) than N2O4 molecules (~25%). On a molecular level, if we follow one NO2 molecule over time, we would find that as it goes back and forth between being part of a N2O4 molecule and being a free NO2 molecule, it now only spends ~25% of the time as part of a N2O4 molecule. Therefore, just like ΔrG°, the equilibrium state is temperature-dependent. This is true for all processes.
Even though the color stops changing once equilibrium is established at the three different temperatures, both the forward and reverse reactions are still continuously occurring inside each of the three reaction vessels.
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