The journey to mastering chemical equilibrium often involves navigating the subtle nuances of heterogeneous reactions. In this problem, we are presented with a classic scenario: the thermal decomposition of a solid into gaseous products. This is not just a mathematical exercise; it's a window into how matter behaves under closed conditions and how we can quantify that behavior using equilibrium constants.
Analyzing the Setup
Imagine a sturdy, evacuated flask with a precise volume of 2 L. The term "evacuated" is crucial here—it means the flask is completely empty, devoid of any air or other gases that could interfere with our reaction or contribute to the total pressure. The temperature is maintained at a constant 27∘C, which we immediately convert to the absolute Kelvin scale as 300 K.
Into this pristine environment, we introduce 5.1 g of solid ammonium bisulfide, NH4HS. Before we can even think about equilibrium, we must translate this mass into the language of chemistry: moles.
The molar mass of NH4HS is calculated by summing the atomic masses of its constituent elements: Nitrogen (14), four Hydrogens (4×1), Sulfur (32), and another Hydrogen (1).
With the molar mass in hand, finding the initial number of moles is straightforward:
ninitial=51 g/mol5.1 g=0.1 mol
So, our starting point is 0.1 mol of solid NH4HS resting at the bottom of the flask.
The Master Equation and ICE Table
The solid doesn't just sit there; it begins to decompose. The balanced chemical equation for this process is:
NH4HS(s)⇌NH3(g)+H2S(g)
Notice the phase states. We have a solid reactant and two gaseous products. This is a heterogeneous equilibrium.
The problem states that 20% of the solid decomposes. This percentage gives us our degree of dissociation, α=0.2. It tells us exactly how much of our initial stash reacts.
Let's set up an ICE (Initial, Change, Equilibrium) table to track the moles of each species.
Initially, we have 0.1 mol of the solid and 0 mol of the gases.
The change is dictated by the 20% decomposition. Twenty percent of 0.1 mol is 0.02 mol. Therefore, 0.02 mol of the solid will disappear.
Because the stoichiometry is 1:1:1, the decomposition of 0.02 mol of solid will produce exactly 0.02 mol of NH3 and 0.02 mol of H2S.
At equilibrium, the moles are:
- NH4HS(s)=0.1−0.02=0.08 mol
- NH3(g)=0+0.02=0.02 mol
- H2S(g)=0+0.02=0.02 mol
Calculating the Equilibrium Constant Kc
The equilibrium constant in terms of concentration, Kc, requires molarities, not just moles. Molarity is moles per unit volume. Since our flask has a volume of 2 L, we divide the equilibrium moles of our gases by 2.
[NH3]=2 L0.02 mol=0.01 M
[H2S]=2 L0.02 mol=0.01 M
Now, we write the expression for Kc. Here is a critical rule of heterogeneous equilibrium: the active mass (concentration) of a pure solid or pure liquid is considered to be constant and is conventionally taken as 1. Therefore, the solid NH4HS does not appear in our Kc expression.
The Bridge to Kp
The question ultimately asks for Kp, the equilibrium constant in terms of partial pressures. While we could calculate the partial pressures of the gases using the ideal gas law and then find Kp, there is a much more elegant route. We use the fundamental relationship between Kp and Kc:
Here, R is the universal gas constant, T is the absolute temperature, and Δng is the change in the number of moles of gas between products and reactants.
Looking at our balanced equation, we have 1 mole of NH3 gas and 1 mole of H2S gas on the product side, totaling 2 moles. On the reactant side, we only have a solid, so there are 0 moles of gas.
Final Calculation
Now, we substitute all our known values into the equation. The problem provides R=0.082 L atm K−1 mol−1 and we know T=300 K.
First, let's compute the term inside the parentheses:
Next, we square this value:
Finally, we multiply by Kc:
Kp=10−4×605.16=6.0516×10−2
The problem states that Kp is in the form x×10−2 and asks for the nearest integer value of x. Comparing our result, 6.0516×10−2, with the given format, we can clearly see that x=6.0516.
Rounding to the nearest integer, we arrive at our final destination:
x=6
This problem beautifully illustrates the interconnectedness of stoichiometry, gas laws, and equilibrium principles. By carefully tracking the physical states and applying the correct relationships, even seemingly complex heterogeneous systems can be unraveled with precision.