Energy, Heat & Work
The vocabulary of energy — system, surroundings, and the crucial difference between heat and temperature.
Touch a metal railing and a wooden bench on the same cold morning: the metal feels far colder, yet a thermometer says they're the same temperature. That puzzle is the whole point of thermochemistry — heat and temperature are not the same thing, and once you separate them, energy bookkeeping suddenly makes sense.
System, surroundings, and the boundary
To study energy we first draw a line. The system is the part of the universe we're focused on — the reacting chemicals, say. Everything else — the beaker, the air, the bench, the rest of the cosmos — is the surroundings. The imaginary line between them is the boundary, and energy is tracked as it crosses that line.
Energy crosses in just two forms: heat (q), the flow driven by a temperature difference, and work (w), energy transferred by a force acting through a distance (for gases, usually pushing back the atmosphere as they expand). Everything in this module is careful bookkeeping of those two flows.
Heat always flows hot → cold
Here's a phrase to bury for good: "the cold from the freezer got into my hand." Cold is not a substance and it does not flow. What actually happens is the reverse — heat flows out of your warm hand into the cold air, and losing that energy is what your nerves register as "cold."
This is why the metal railing feels colder than the wooden bench at the same temperature: metal conducts heat away from your skin quickly, so heat leaves your hand faster. Same temperature, very different rate of heat flow.
The first law: energy is conserved
Internal energy (U) is the total energy stored in a system — the kinetic and potential energy of all its particles. We can't measure U directly, but we can measure how it changes. The first law of thermodynamics says the change equals the heat added plus the work done on the system:
- Heat is absorbed by the system, so q = +500 J.
- The system does work on the surroundings (it expands outward), so energy leaves: w = −200 J.
- Apply the first law: ΔU = q + w = (+500) + (−200).
- ΔU = +300 J.
- Heat is released by the system, so q = −350 J.
- Work is done on the system (it is compressed), so w = +120 J.
- ΔU = q + w = (−350) + (+120).
- ΔU = −230 J — the internal energy fell by 230 J.
Check your understanding
- The system is what we study; the surroundings are everything else; energy is tracked crossing the boundary.
- Temperature = average kinetic energy (intensity); heat = energy transferred because of a temperature difference.
- Heat flows from hot to cold — "cold flowing in" is just heat flowing out.
- Internal energy U is a state function; heat and work are path functions.
- First law: ΔU = q + w, with energy IN positive and energy OUT negative.