General Chemistry I · Energy and Thermodynamics

Energy and Heat

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On this page 7 sections
  1. In 30 seconds
  2. Why this matters
  3. The college version
  4. Eli explains
  5. Worked example
  6. Key takeaway
  7. Study tools

In 30 seconds

is the capacity to do work or transfer heat, appearing as (motion) or (stored position or composition). Thermochemistry tracks energy exchanged between a defined and its . Internal energy E is a , so ΔE depends only on initial and final states, not the path. The first law states that energy is conserved: ΔE = q + w, where q is heat added to the system and w is work done on it.

Why this matters

The first law underlies human energy balance. Food "Calories" are really kilocalories (1 Cal = 4184 J); the body is an open system that takes in chemical potential energy and releases heat and work, with fever and shivering adjusting that rate. In the lab, the same principle lets insulated containers (calorimeters) trap a reaction's heat so its energy change can be measured — the subject of the next topic.

The college version

1. Kinetic vs. Potential Energy

Kinetic energy is the energy of motion, depending on mass and speed. Potential energy is stored energy of position or composition — a stretched spring, a ball on a shelf, or chemical bonds. In any chemical sample the molecules are always moving (kinetic energy), while electrostatic attractions between nuclei, electrons, and neighboring molecules store potential energy. Reactions are useful precisely because they convert bond potential energy into heat and work.

2. System and Surroundings

The system is the substance or reaction under study; the surroundings are everything else. An open system exchanges both matter and energy (a boiling pot); a closed system exchanges energy but not matter (a sealed bottle); an isolated system exchanges neither (an ideal thermos). Energy crosses the boundary in only two forms: heat (q) or work (w).

3. State Functions and the First Law

Internal energy E is the total kinetic plus potential energy of the particles in a system. We cannot measure E itself, only ΔE = Efinal - Einitial. Crucially, E is a state function: its value depends only on the current state, not on how the system got there. The is conservation of energy applied to a system: ΔE = q + w. Heat and work are path functions, but their sum equals the change in the state function E.

How it works

  1. Choose the system and draw a boundary around it; everything else is the surroundings.
  2. Identify each energy transfer across that boundary as heat q, work w, or both.
  3. Assign signs: energy entering the system is positive; energy leaving is negative.
  4. Sum them using ΔE = q + w.
  5. If a gas changes volume against constant pressure, compute w = -PΔV and convert units.
  6. Interpret the sign of ΔE: positive means the system gained energy, negative means it lost energy.

Common confusions

Do not confuseWithDifference
Heat (q)TemperatureHeat is energy transferred; temperature is average molecular kinetic energy
Internal energy (E)Heat or workE is a state function of the system; q and w are transfers across the boundary
Work done on systemWork done by system"On" is positive (energy in); "by" is negative (energy out)
SystemSurroundingsSystem is what you study; surroundings are everything else
Isolated systemClosed systemIsolated exchanges neither matter nor energy; closed exchanges energy only

Memory aids

"In is +, Out is −" — any energy (heat or work) entering the system carries a plus sign, and anything leaving carries a minus sign. Then ΔE = q + w always balances the ledger.

Quick review

Topic Recap

Energy is the capacity to do work or transfer heat, existing as kinetic or potential energy. We track it by defining a system and its surroundings; energy crosses the boundary only as heat q or work w. Internal energy is a state function, and the first law says energy is conserved: ΔE = q + w. Consistent signs — positive for energy in, negative for energy out — make every calculation reproducible, and w = -PΔV quantifies pressure–volume work.

Knowledge Check

  1. Which quantity is a state function? A) heat q B) work w C) internal energy E D) path length
  2. A system absorbs 40 J of heat and has 15 J of work done on it. ΔE is: A) 25 J B) 40 J C) 55 J D) −25 J
  3. A gas expands, doing work on its surroundings. The sign of w for the system is: A) positive B) negative C) zero D) depends on pressure only
  4. Which system exchanges energy but not matter with its surroundings? A) open B) closed C) isolated D) none of these
  5. A gas is compressed from 4.0 L to 2.0 L at a constant external pressure of 2.0 atm. The work (L·atm) is: A) −4.0 B) +4.0 C) −8.0 D) +8.0

Answers and Rationales

  1. C — Internal energy depends only on the state of the system; heat and work depend on the path.
  2. C — ΔE = q + w = (+40 J) + (+15 J) = 55 J. Both terms are positive because heat and work both entered the system.
  3. B — The system loses energy doing expansion work, so w is negative (w = -PΔV with ΔV > 0).
  4. B — A closed system exchanges energy but not matter; an isolated system exchanges neither.
  5. B — ΔV = 2.0 - 4.0 = -2.0 L, so w = -(2.0 atm)(-2.0 L) = +4.0 L · atm. Compression means work is done on the system (positive).
Eli, the EliExplains learning guide

Eli explains

The same idea, in plain words

Explain it like I’m 10

Think of a system's energy like money in a bank account. Kinetic energy is cash moving between your hands right now; potential energy is money parked in savings. Drop a ball and stored potential energy becomes kinetic energy as it falls. Gasoline works the same way: it stores chemical potential energy in bonds, and burning releases it as heat and work.

The analogy stops being exact because a bank balance is one number, while internal energy is spread across many invisible accounts — molecular motion plus every bond and attraction. We cannot total those accounts; we measure only changes when energy crosses the boundary as heat or work.

Simple Example

A hot cup of coffee (the system) sits on a desk (the surroundings). Its molecules jiggle fast, carrying lots of kinetic energy, which is why it feels hot. Energy flows out of the coffee as heat into the cooler room until both reach the same temperature. Nothing is created or destroyed — energy is simply transferred.

Worked example

Kinetic energy of a moving object of mass m and speed v:

KE = 12mv2

First law of thermodynamics:

ΔE = q + w

where ΔE is the change in internal energy (J), q is heat added to the system (J), and w is work done on the system (J). Pressure–volume work at constant pressure P with volume change ΔV:

w = -PΔV

Sign conventions (used consistently throughout these notes):

QuantityPositive (+)Negative (−)
q (heat)absorbed by systemreleased by system
w (work)done on system (compression)done by system (expansion)
ΔEsystem gains energysystem loses energy

Conversion factor: 1 L · atm = 101.3 J.

Worked Example 1 — First law with heat and work

A gas absorbs 50.0 J of heat and does 30.0 J of work on its surroundings. Find ΔE.

Step 1. Assign signs: heat is absorbed by the system, so q = +50.0 J; work is done by the system, so w = -30.0 J.

Step 2. Apply the first law:

ΔE = q + w = (+50.0 J) + (-30.0 J) = +20.0 J

The system gains 20.0 J of internal energy.

Worked Example 2 — Pressure–volume work

A gas expands from 1.00 L to 2.50 L against a constant external pressure of 1.00 atm. How much work does the gas do, in joules?

Step 1. Compute the volume change: ΔV = 2.50 L - 1.00 L = 1.50 L.

Step 2. Use w = -PΔV:

w = -(1.00 atm)(1.50 L) = -1.50 L · atm

Step 3. Convert to joules:

w = -1.50 L · atm × 101.3 J1 L · atm = -152 J

The negative sign confirms the system lost energy by doing work on the surroundings (expansion).

Common setup errors: forgetting the minus sign in w = -PΔV; using Celsius instead of a consistent unit set; and flipping the sign of q or w (always ask "into or out of the system?").

Key takeaways

  • High yield: Energy crosses a system boundary only as heat (q) or work (w).
  • High yield: Heat absorbed and work done on the system are positive; heat released and work done by the system are negative.
  • Internal energy E is a state function; q and w are path functions whose sum equals ΔE.
  • ΔE = q + w is the first law (conservation of energy).
  • Expansion work is w = -PΔV; an expanding gas has w < 0.
  • 1 L · atm = 101.3 J.
  • Heat and temperature differ: heat is an energy transfer; temperature is average molecular kinetic energy.

Keep learning

Ready to build on this? Continue to the next lesson.

Practice General Chemistry I

This lesson has no separate scored set. Practice draws from the subject’s question bank.

Study tools & related lessonsYou’ll learn to · Key vocabulary · Related

You’ll learn to

  • Distinguish kinetic from potential energy and identify each in chemical systems.
  • Define the system and surroundings and classify systems as open, closed, or isolated.
  • Explain what a state function is and why internal energy is one.
  • Apply the first law of thermodynamics, ΔE = q + w, with consistent sign conventions for heat and work.

Key vocabulary

Energy
Capacity to do work or transfer heat
Kinetic energy
Energy of motion, KE = 12mv2
Potential energy
Stored energy of position or composition
System
The part of the universe under study
Surroundings
Everything outside the system
State function
A property that depends only on the current state, not the path
Internal energy (E)
Total kinetic + potential energy of all particles
Heat (q)
Energy transferred because of a temperature difference
Work (w)
Energy transferred when a force moves something
First law of thermodynamics
Energy is conserved: ΔE = q + w
Joule (J)
SI unit of energy

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