Intuition The one core idea
Energy is never lost (that is the First Law), but energy does have a preferred direction of flow: heat slides from hot to cold on its own, and no machine can perfectly undo that for free. The Second Law is just the bookkeeping of that one-way street — and everything below is the vocabulary you need to state it precisely.
Before you can even read the Kelvin–Planck and Clausius statements, a whole toolbox of words and symbols must already mean something to you. This page builds each one from nothing, in the order they depend on each other. Nothing here is assumed — if the parent note used it, we define it.
This is the foundations note for the Second Law topic .
U (internal energy)
Plain words: the total hidden jiggling energy stored inside a lump of stuff — the kinetic energy of its wildly moving molecules, plus the energy locked in the springs between them.
The picture: a box full of tiny balls bouncing around. Fast balls = hot = large U . Slow balls = cold = small U .
Why the topic needs it: the Second Law is about what happens to energy as it moves. U is the reservoir of energy that sits inside a system.
Q
Plain words: energy that flows because of a temperature difference . It is energy in transit , not energy that a body "has."
The picture: two boxes touching — one with fast balls, one with slow. Fast box shares jiggle with slow box across the wall. That flowing jiggle is Q .
Why: both Second-Law statements are literally rules about which way Q may flow.
W
Plain words: energy transferred by a push over a distance — an ordered, useful, mechanical form. Turning a wheel, lifting a weight, driving a piston.
The picture: a gas pushing a piston outward. The piston moves; something outside gets lifted. That organised energy is W .
Sign convention (fix this now, keep it forever): throughout this page W means the work done by the system on its surroundings . So W > 0 when the system pushes outward (an engine delivering work), and W < 0 when the surroundings push in on the system (work being supplied to it, as in a fridge).
Why: an engine's whole job is to turn messy heat Q into tidy work W . The Second Law limits how well it can.
Figure s01 — Heat vs Work across a boundary. The teal arrow on the left is heat Q (disordered, driven by a temperature difference); the plum arrow on the right is work W done by the system on the piston. Notice how the plum arrow all points one way (ordered) while the molecular arrows inside scatter every direction (disordered).
Intuition Heat vs work — the key contrast
Both Q and W are energy crossing a boundary . The difference is order : work is coordinated (all the pushing points one way), heat is disordered (jiggle in every direction). The Second Law is really about the price of turning disorder into order.
Definition Thermal reservoir
Plain words: an object so enormous that you can pour heat in or scoop it out without changing its temperature at all.
The picture: the ocean. Drop a hot spoon in — the ocean does not warm up measurably.
Why: the statements say "a single reservoir," "hot reservoir," "cold reservoir." We need bodies whose temperature stays fixed so we can talk cleanly about heat flowing between two steady temperatures.
We write the hot reservoir temperature and heat with subscript H , the cold with subscript C :
Q H = heat exchanged with the hot reservoir.
Q C = heat exchanged with the cold reservoir.
Common mistake "The subscript tells me the sign."
No — H and C only say which reservoir . Whether that heat flows in or out depends on the machine. In this topic we adopt the convention that Q H , Q C (and W in the efficiency and COP formulas) are written as magnitudes — positive numbers — and the direction of each flow is stated in words or shown by the diagram's arrows.
Definition Cyclic process (a cycle)
Plain words: a process that ends in exactly the same state it started in — same pressure, same volume, same internal energy U . The machine is ready to repeat forever.
The picture: a closed loop drawn on a pressure–volume graph. Start at a point, wander around, return to the same point.
Why the topic needs it: every forbidden machine is a cyclic device. A one-shot trick that ends in a different state doesn't count. This single word defuses the "isothermal expansion converts all heat to work" objection.
Figure s02 — A cycle as a closed loop. The orange curve is the machine's path on a pressure–volume graph; the teal arrows show the direction of travel; the plum dot is the single point where the path starts and ends, so Δ U = 0 over one loop.
Intuition Why "cycle" is the secret hero
In one straight-line expansion a gas can turn all its absorbed heat into work — but it ends up bigger, and you cannot run it again without resetting it. Resetting costs work and dumps heat. Only over a closed loop is the accounting honest, and only then does full heat-to-work conversion become impossible.
Δ
Plain words: Δ X means "the final value of X minus the initial value" — how much X changed.
The picture: an arrow from the start-height to the end-height of a quantity.
Q net
Plain words: the total heat that ends up added to the system over a whole cycle — everything it absorbed minus everything it rejected.
In symbols (using magnitudes): Q net = Q H − Q C (heat taken from hot, minus heat dumped to cold).
Why we need a name for it: the cycle derivation below adds up all the heat crossings into this one bookkeeping number.
Intuition The magic simplification for a cycle
In a cycle the system returns to its start, so its internal energy returns too: Δ U = 0 . The First Law then collapses to
0 = Q net − W ⟹ W = Q net = Q H − Q C .
This one line — work equals heat-in minus heat-out — is used in every engine calculation in the parent note.
See First law of thermodynamics for the full construction of Δ U = Q − W .
η (Greek letter "eta")
Plain words: the fraction of the heat you paid for (Q H ) that actually came out as useful work (W ). All three symbols here are positive magnitudes .
The picture: a pie of size Q H ; the slice you keep as work is W , the wasted slice is Q C .
Why: the Kelvin–Planck statement is exactly the claim "η can never reach 1 ."
Figure s03 — The efficiency pie. The teal bar is the paid heat Q H = 800 J. It splits into a plum slice W = 500 J (kept as work) and an orange slice Q C = 300 J (dumped cold). The ratio of plum to the whole teal bar is η = 0.625 .
Worked example Reading the pie
If Q H = 800 J and Q C = 300 J, then W = 500 J and η = 500/800 = 0.625 . So 62.5% of the input heat became work; the rest was dumped cold. (This is Example 3 in the parent note.)
Definition Coefficient of performance (COP)
Plain words: for a refrigerator, the ratio of the heat you pulled out of the cold room (Q C ) to the work you paid (W ) to do it. Bigger = better. As in the efficiency formula, Q C and W here are positive magnitudes .
The picture: you spend a small W (electricity) to move a large Q C out of the cold box — leverage.
Why: the Clausius statement is the claim "you can never get Q C for W = 0 " — a fridge with infinite COP is forbidden.
Common mistake "Which sign does
W take in the First Law for a fridge?"
In the signed First Law Δ U = Q − W , a fridge has work supplied to it, so there W is negative . But in the magnitude COP formula COP = Q C / W we use the size of that work, a positive number. Same physical work, two bookkeeping styles: signed for the First Law, magnitudes for the engine/fridge scorecards. Always ask: am I in signed mode or magnitude mode?
Absorbs Q H from hot, does work W (output, so signed W > 0 ), rejects Q C to cold. Runs "downhill" and skims work off the flow.
Definition Refrigerator / heat pump
Uses work W (input, so signed W < 0 in the First Law but written as a positive magnitude in COP) to drag Q C from cold and dump Q H = Q C + W into hot. Runs "uphill" and needs pushing.
Mnemonic Engine vs fridge arrows
Engine: heat falls hot→cold, work drips out.
Fridge: work drives heat cold→hot, uphill.
The related machines and their limits are studied in Carnot engine and Carnot theorem .
Definition Spontaneous process
Plain words: something that happens on its own , with no outside push. Heat flowing hot→cold is spontaneous; cold→hot is not.
Why: Clausius forbids the cold→hot transfer as a sole effect — i.e. spontaneously.
Definition Reversible vs irreversible
Reversible: a process you could run backward and leave no trace — the film looks fine played in reverse. Irreversible: running it backward would need a Second-Law-violating miracle.
Why: the whole Second Law is the statement that the real world is irreversible; time has a direction. See Reversible and irreversible processes and Arrow of time .
The deeper measure of this one-way-ness — entropy — is built in Entropy and the Clausius inequality .
Read the map below bottom-up as a dependency chain : the three raw quantities (U , Q , W ) plus the idea of a cycle combine into the First Law; the First Law plus the reservoir–engine picture gives efficiency η , and plus the reservoir–fridge picture gives COP; η becomes the language of Kelvin–Planck, COP becomes the language of Clausius, and (together with spontaneous flow) both feed the single Second Law. Every arrow means "you need the tail box before the head box makes sense."
Clausius no free cold to hot
Test yourself — cover the right side and answer before revealing.
What does internal energy U physically measure? The total hidden kinetic-plus-potential energy of a system's jiggling molecules.
What makes heat Q different from work W ? Q is disordered energy flowing due to a temperature difference; W is ordered energy transferred by a push over a distance.
What is the sign convention for W on this page? W is the work done by the system; W > 0 when the system pushes out (engine), W < 0 when work is supplied in (fridge).
What is a thermal reservoir? A body so large its temperature stays fixed even as heat is added or removed.
What do the subscripts H and C mean? They label the hot and cold reservoirs; Q H , Q C (and W in the scorecards) are magnitudes, with direction stated separately.
What is Q net for a cycle? The total heat added over the loop, Q net = Q H − Q C .
What defines a cyclic process, and why does it matter here? The system returns to its exact starting state (Δ U = 0 ); "cyclic" is what makes η = 1 genuinely impossible.
State the First Law and its cycle form. Δ U = Q − W (signed); for a cycle Δ U = 0 so W = Q net = Q H − Q C .
Write efficiency η three equivalent ways. η = W / Q H = ( Q H − Q C ) / Q H = 1 − Q C / Q H .
What is COP and which machine uses it? COP = Q C / W , the score of a refrigerator — heat pulled from cold per unit work paid.
How does W 's sign differ between the First Law and the COP formula for a fridge? In the signed First Law W < 0 (work supplied in); in the magnitude COP formula W is the positive size of that same work.
Why is a spontaneous cold→hot transfer forbidden? Because it would move heat uphill with no other effect — a Clausius violation; only work-driven uphill flow is allowed.