The First Law of Thermodynamics
Balancing Heat and Work
Imagine a gas trapped inside a cylinder with a movable piston. This gas is our thermodynamic system. The universe is constantly exchanging energy with this system in two primary ways: through heat and through work.
In this problem, we are told that the system absorbs 150 J of heat. According to the IUPAC sign convention used in chemistry, any energy entering the system is considered positive. Therefore, the heat exchanged is q=+150 J.
At the exact same time, the system does 200 J of work. When a system does work (like expanding and pushing a piston upward), it expends its own energy. Because energy is leaving the system, we assign a negative sign to this work. Thus, W=−200 J.
The Master Equation
To find out what happens to the system's overall energy, we invoke the First Law of Thermodynamics. This law is essentially the principle of conservation of energy applied to thermodynamic systems. It states that the change in internal energy (ΔU) is the sum of the heat added to the system and the work done on the system.
Mathematically, it is expressed as:
Final Calculation
Now, we carefully substitute our values into the master equation. It is crucial to carry the signs along to avoid silly mistakes!
The negative sign indicates that the system's internal energy has decreased by 50 J overall. It spent more energy doing work than it gained from the heat it absorbed.
However, the question specifically asks for the magnitude of the change in internal energy. The magnitude is simply the absolute value, stripping away the sign to just look at the 'size' of the change.
And there we have it! The magnitude of the change in internal energy is 50 J.