The Setup
A Tale of Two Gases
Imagine you have a sturdy, closed vessel. Inside this vessel, you have a sample of a monatomic ideal gas—let's say it's Helium or Neon. You have exactly 0.1 moles of this gas, and it's sitting at a chilly 200 K.
Now, you decide to pump more of the exact same gas into this vessel. You add 0.05 moles, but this new batch is much hotter, at 400 K. The question is: once these two batches of gas mix and settle down, what will be their final equilibrium temperature?
The Master Principle
Conservation of Energy
Whenever you are dealing with a closed, insulated system where no heat is lost to the surroundings and no mechanical work is done, you have a powerful tool at your disposal: The Conservation of Internal Energy.
The total internal energy of the system before mixing must perfectly equal the total internal energy after mixing. We can write this mathematically as:
For an ideal gas, the internal energy U is purely a function of its temperature and is given by the formula U=nCVT, where n is the number of moles and CV is the molar heat capacity at constant volume.
The Mathematical Symphony
Let's substitute our internal energy formula into the conservation equation. Since both batches are the exact same monatomic gas, their CV values are identical.
n1CVT1+n2CVT2=(n1+n2)CVT
Do you notice something beautiful here? The term CV appears in every single part of the equation. Because it's a non-zero constant, we can divide the entire equation by CV, completely eliminating it from our math!
This simplified equation tells us that the final temperature is essentially a weighted average of the initial temperatures, weighted by the number of moles.
The Final Calculation
Now, it's just a matter of carefully plugging in our given values. We have n1=0.1 mol, T1=200 K, n2=0.05 mol, and T2=400 K.
(0.1)(200)+(0.05)(400)=(0.1+0.05)T
Let's compute the terms on the left side:
To find the final temperature T, we simply divide 40 by 0.15:
The problem asks for the answer rounded to the nearest integer. Rounding 266.66 gives us our final answer:
And there you have it! By trusting the conservation of energy, we easily found the equilibrium state of the mixture.