The beauty of thermodynamics lies in its ability to connect abstract mathematical equations with tangible physical realities. In this problem, we are exploring one of the most elegant processes in physics: the adiabatic expansion.
Imagine a perfectly insulated cylinder containing a monoatomic ideal gas. The gas is allowed to expand, pushing a piston outwards. Because the cylinder is insulated, no heat can enter or leave the system (Q=0). Yet, the gas is doing work on the piston. Where does the energy for this work come from? It must come from the gas's own internal energy! As a result, the gas cools down. Let's dive into the math to see exactly how much energy is spent.
The Master Equation
Adiabatic Expansion
To find the change in internal energy, our first mission is to determine the final temperature of the gas. For an adiabatic process, the pressure, volume, and temperature are locked in a strict mathematical dance. Since we are dealing with temperature and volume, we use the relation:
This means that the initial state and the final state are connected by:
But what is γ (gamma)? Gamma is the ratio of specific heats (Cp/CV). For a monoatomic gas (like Helium or Argon), the atoms only have 3 translational degrees of freedom. This gives us a specific γ value:
Therefore, the exponent in our equation becomes:
Calculating the Final Temperature
Now, let's substitute the known values into our master equation. We know the initial temperature T1=100 K, and the final volume is eight times the initial volume (V2=8V1).
Notice how beautifully the initial volume V1 is poised to cancel out. Let's rearrange the equation to isolate the final temperature T2:
To solve this without a calculator, we can take the cube root first, and then square the result. The cube root of 81 is 21, and squaring that gives 41.
The gas has cooled down from 100 K to a freezing 25 K! This massive temperature drop is the direct result of the gas expending its internal energy to expand.
The Final Calculation
Change in Internal Energy
Now for the final piece of the puzzle. The change in internal energy (ΔU) for any ideal gas depends only on the change in temperature, and is given by the formula:
For a monoatomic gas, the molar heat capacity at constant volume (CV) is 23R. Let's set up our final calculation with n=1 mole and R=8.0 J mol−1K−1:
The negative sign is crucial here. It mathematically confirms our physical intuition: the internal energy of the system has decreased.
Since the question specifically asks for the decrease in internal energy, we take the absolute value. The internal energy decreased by exactly 900 J.
According to the First Law of Thermodynamics (Q=ΔU+W), since Q=0, the work done by the gas is W=−ΔU=900 J. The gas performed 900 J of mechanical work, and it paid the exact price of 900 J from its own thermal bank account!