The Beauty of Chemical Equilibrium
Imagine you are standing inside a microscopic reaction vessel heated to a scorching 1990 K. All around you, diatomic chlorine molecules (Cl2) are absorbing intense thermal energy and violently splitting apart into individual chlorine atoms (Cl). Simultaneously, these atoms are colliding and recombining back into molecules. This beautiful, dynamic dance is what we call chemical equilibrium.
Analyzing the Setup
The problem gives us a fascinating constraint: at equilibrium, the number of Cl2 molecules exactly equals the number of Cl atoms.
Why is this piece of information so powerful? Because in chemistry, the number of molecules is directly proportional to the number of moles (thanks to Avogadro's principle). If the molecules are equal in number, their moles must also be equal. Let's say we have n moles of Cl2 and n moles of Cl.
The Power of Mole Fractions
Here is where the magic happens. The total number of moles in our container is simply n+n=2n.
The mole fraction (χ) of any gas is its own moles divided by the total moles. For both our chlorine molecules and chlorine atoms, the math is identical:
They each make up exactly 50% of the gas mixture!
Dalton's Law in Action
Now that we have the mole fractions, we can find the partial pressures. Dalton's Law of Partial Pressures states that the partial pressure of a gas (pi) is equal to its mole fraction multiplied by the total pressure (Ptotal).
We are given that the total pressure is 1 atm. Let's calculate the partial pressures:
The Master Equation
With our partial pressures in hand, we are ready to tackle the equilibrium constant, Kp. For the reaction Cl2(g)⇌2Cl(g), the expression for Kp is the partial pressure of the products raised to their stoichiometric coefficients, divided by the partial pressure of the reactants.
Notice the squared term in the numerator! That comes directly from the '2' in front of the Cl atom in our balanced equation. This is a common place where students make silly mistakes, so always double-check your exponents.
Final Calculation
Let's substitute our calculated partial pressures into the Kp expression:
One of the 0.5 terms in the numerator beautifully cancels out with the 0.5 in the denominator, leaving us with:
The problem asks us to express this in the format x×10−1. We can easily rewrite 0.5 as 5×10−1.
Comparing this to the given expression, it is crystal clear that our unknown value x is exactly 5.