Analyzing the Setup
Imagine you have a mysterious gas trapped in a container. We are given a fascinating scenario where we observe this gas in two different theoretical states. First, it behaves as a real gas with a compressibility factor (Z) of 0.5. Then, we are asked to imagine it behaving ideally at the exact same temperature and pressure.
Before we dive into the equations, let's clear up a small unit detail. The volume is given in dm3 mol−1. It is crucial to remember that 1 dm3 is exactly equal to 1 L. Therefore, our real molar volume is simply 0.4 L mol−1.
The Master Equation
To find the unknown pressure x, we need our master tool: the compressibility factor equation. This formula acts as the bridge between real and ideal behavior.
Let's carefully substitute our known values into this equation. We know Z=0.5, the molar volume Vm=0.4 L mol−1, and the temperature T=800 K. For the gas constant R, the problem explicitly tells us to use 8×10−2, which is 0.08 L atm K−1 mol−1.
Now, let's do the math. Multiplying the denominator, 0.08×800 gives us 64.
Multiplying 64 by 0.5 gives 32. Dividing 32 by 0.4, we get our pressure x:
The Ideal Shortcut
Next, we need to find the ideal molar volume, y. For an ideal gas, the volume is simply RT divided by P. We could plug our newly found pressure of 80 atm back into the ideal gas equation.
y=800.08×800=8064=0.8 L mol−1
But wait, there's a beautiful shortcut! The compressibility factor Z is also exactly equal to the ratio of real volume to ideal volume at the same temperature and pressure.
Using our shortcut, 0.5=y0.4. Solving this, we instantly get y=0.8 L mol−1. Both methods yield the exact same result, but the shortcut is a powerful tool to save time during an exam!
Final Calculation
We are almost at the finish line. The question asks for the ratio of x to y. We simply divide our pressure, 80, by our ideal volume, 0.8.
And there we have it! Our final answer is 100. As a quick conceptual check, since Z<1, it means the real gas is more compressible than an ideal gas, indicating that attractive intermolecular forces are dominating in this state.