Internal energy, often denoted by the symbol \( U \), is a fundamental concept in chemistry that represents the total energy contained within a chemical system. This energy manifests as the sum of potential energy, which is the energy due to the positions of the particles, and kinetic energy, the energy of motion of the particles. An easy way to understand internal energy is by picturing a balloon: the energy that the gas molecules possess inside the balloon, due to their motion and interactions, comprises the balloon's internal energy.
What's crucial about internal energy is that it's a state function, which means its value doesn't depend on how the system arrived at its current state. Whether the molecules gained energy through heating or were compressed, the final amount of internal energy is the same if the end conditions are identical.
The change in internal energy (\( \Delta U \)) is what chemists often focus on, especially in reactions and processes. It can be calculated using the first law of thermodynamics, which relates the change in internal energy to the heat added to the system (\( Q \)) and the work done by the system (\( W \)): \[ \Delta U = Q - W \]
- \( Q \) is positive if heat is added to the system, increasing its internal energy.
- \( W \) is positive if work is done by the system, which decreases its internal energy.
Understanding internal energy helps students predict how energy transfers will affect chemical reactions and the physical states of substances.