enthalpy and entropy
/ EN-thal-pee / EN-troh-pee /
Behind Gibbs free energy stand two characters, each describing a different reason a reaction might be favored. Enthalpy is about heat — does the reaction release energy or soak it up? Entropy is about disorder — does the reaction spread things out into more arrangements, or pack them into fewer? Nature likes both releasing heat and spreading out, and a reaction's fate is the negotiation between these two pulls.
Enthalpy change, delta H, is essentially a bond-strength ledger. Breaking bonds costs energy; forming bonds pays it back. If the bonds in the products are stronger overall than the bonds in the reactants, energy is released and delta H is negative — the reaction is exothermic, giving off heat (a burning match, an exploding firework). If it costs more than it pays, delta H is positive and the reaction is endothermic, absorbing heat (an instant cold pack). Entropy change, delta S, counts how the number of available arrangements changes: turning one big molecule into two smaller ones, or a tidy solid into a freely tumbling gas, raises entropy (positive delta S), because there are now vastly more ways for the pieces and their energy to be arranged.
These two combine through delta G = delta H - T delta S, and they can cooperate or compete. A reaction can be favorable because it releases a lot of heat even though it lowers entropy, or favorable because it raises entropy enough to overcome an uphill enthalpy — and the temperature T decides how much entropy gets to weigh in. This is why a ring-opening that makes more, freer molecules becomes favorable on heating, and why entropy, easy to overlook, quietly drives many organic reactions that enthalpy alone would forbid.
Burning methane is exothermic (negative delta H: strong O-H and C=O bonds form) and also raises entropy (more gas molecules), so both terms make delta G very negative.
Enthalpy = the heat (bond-strength) ledger; entropy = the spread-out (disorder) ledger.
Entropy is not simply messiness; it is the number of ways energy and particles can be arranged. And neither delta H nor delta S alone decides spontaneity — only their combination in delta G, weighed by temperature, does.