Chemistry · Thermodynamics

Enthalpies of Different Reactions

The enthalpy change of a reaction depends on the conditions under which it is carried out, so chemists fix a reference — the standard state — and then give specific names to the enthalpy change of specific processes. Following NCERT Class 11 Unit 5 (§5.4–5.5), this note builds the family of named enthalpies: formation, combustion, phase transition, atomisation, bond and lattice enthalpy, plus enthalpy of solution. For NEET, the most reliable marks come from the summation rule $\Delta_r H^\ominus = \sum \Delta_f H^\ominus(\text{products}) - \sum \Delta_f H^\ominus(\text{reactants})$ and the bond-enthalpy method — both reappear almost every year.

Standard Enthalpy of Reaction

The enthalpy of a reaction depends on the temperature and pressure at which it occurs, so to make values comparable we specify a standard state. The standard state of a substance at a given temperature is its pure form at 1 bar; for example, the standard state of liquid ethanol at 298 K is pure liquid ethanol at 1 bar, and that of solid iron at 500 K is pure iron at 1 bar. Data are usually tabulated at 298 K.

The standard enthalpy of reaction, written $\Delta_r H^\ominus$, is the enthalpy change for a reaction when every participating substance is in its standard state. The superscript $\ominus$ denotes standard conditions. The unit is $\text{kJ mol}^{-1}$, meaning "per mole of reaction" as written: once the equation is balanced in a particular way, that fixes one mole of reaction.

Because enthalpy is an extensive property, doubling the coefficients doubles $\Delta_r H^\ominus$, and reversing the equation reverses its sign. For ammonia synthesis $\ce{N2(g) + 3H2(g) -> 2NH3(g)}$ has $\Delta_r H^\ominus = -91.8~\text{kJ mol}^{-1}$, while the reverse decomposition $\ce{2NH3(g) -> N2(g) + 3H2(g)}$ has $\Delta_r H^\ominus = +91.8~\text{kJ mol}^{-1}$.

NEET Trap

"Per mole" is per mole of reaction, not per mole of any one species

When NCERT balances $\ce{Fe2O3(s) + 3H2(g) -> 2Fe(s) + 3H2O(l)}$ one way it gets $\Delta_r H^\ominus = -33.3~\text{kJ mol}^{-1}$; halving every coefficient gives exactly half, $-16.6~\text{kJ mol}^{-1}$. The number is tied to the equation, so always read the coefficients before plugging in.

Change the stoichiometric coefficients → scale $\Delta_r H^\ominus$ by the same factor. Reverse the equation → flip the sign.

Exothermic vs Endothermic Profiles

A reaction that releases heat to the surroundings is exothermic and carries a negative $\Delta_r H$; one that absorbs heat is endothermic with a positive $\Delta_r H$ (NIOS §9.2). Burning methane, $\ce{CH4(g) + 2O2(g) -> CO2(g) + 2H2O(l)}$ with $\Delta H = -891~\text{kJ}$, is exothermic, whereas $\ce{H2(g) + I2(g) -> 2HI(g)}$ with $\Delta H = +52.2~\text{kJ}$ is endothermic. The sign of $\Delta_r H$ is the single fact a profile diagram has to communicate.

Figure 1 Enthalpy H Reaction progress Reactants Products ΔH < 0 Exothermic Reaction progress Reactants Products ΔH > 0 Endothermic

Reaction enthalpy profiles. In an exothermic reaction the products sit lower on the enthalpy axis than the reactants, so heat is released ($\Delta H < 0$). In an endothermic reaction the products sit higher, so heat is absorbed ($\Delta H > 0$). The vertical gap between the reactant and product levels is $\Delta_r H$.

Enthalpy of Formation

The standard molar enthalpy of formation, $\Delta_f H^\ominus$, is the standard enthalpy change when one mole of a compound is formed from its elements in their most stable reference states. The reference state of an element is its most stable state of aggregation at 25 °C and 1 bar — so the reference states of hydrogen, oxygen, carbon and sulphur are $\ce{H2(g)}$, $\ce{O2(g)}$, $\ce{C(graphite)}$ and $\ce{S(rhombic)}$ respectively. Three NCERT examples:

$\ce{H2(g) + 1/2 O2(g) -> H2O(l)}$;  $\Delta_f H^\ominus = -285.8~\text{kJ mol}^{-1}$
$\ce{C(graphite) + 2H2(g) -> CH4(g)}$;  $\Delta_f H^\ominus = -74.81~\text{kJ mol}^{-1}$
$\ce{2C(graphite) + 3H2(g) + 1/2 O2(g) -> C2H5OH(l)}$;  $\Delta_f H^\ominus = -277.7~\text{kJ mol}^{-1}$

A formation enthalpy is just a special case of a reaction enthalpy in which exactly one mole of a single compound is formed from elements. By convention, the $\Delta_f H^\ominus$ of any element in its reference state is taken as zero. Two reactions illustrate what does not qualify: $\ce{CaO(s) + CO2(g) -> CaCO3(s)}$ is not a formation reaction because the carbonate is built from compounds, and $\ce{H2(g) + Br2(l) -> 2HBr(g)}$ produces two moles, so its enthalpy equals $2\,\Delta_f H^\ominus(\ce{HBr})$ — to get the formation value we divide through to write $\ce{1/2 H2(g) + 1/2 Br2(l) -> HBr(g)}$ with $\Delta_f H^\ominus = -36.4~\text{kJ mol}^{-1}$.

NEET Trap

One mole of product, from elements, in reference states — all three must hold

Examiners disguise non-formation reactions by giving the right element but the wrong allotrope, or by forming two moles of product. If the equation makes more than one mole of the compound, or starts from a compound rather than an element, the listed $\Delta H$ is a reaction enthalpy, not $\Delta_f H^\ominus$.

Diamond is not the reference state of carbon — graphite is. So $\Delta_f H^\ominus(\ce{C, graphite}) = 0$ but $\Delta_f H^\ominus(\ce{C, diamond}) \neq 0$.

The ΔfH Summation Rule

Because enthalpy is a state function, the reaction enthalpy can be obtained from tabulated formation enthalpies through the central NEET formula:

$$\Delta_r H^\ominus = \sum_i a_i\,\Delta_f H^\ominus(\text{products}) - \sum_i b_i\,\Delta_f H^\ominus(\text{reactants})$$

where $a_i$ and $b_i$ are the stoichiometric coefficients of products and reactants. Applying it to the decomposition of limestone, $\ce{CaCO3(s) -> CaO(s) + CO2(g)}$, with $\Delta_f H^\ominus$ values of $-635.1$, $-393.5$ and $-1206.9~\text{kJ mol}^{-1}$ for $\ce{CaO}$, $\ce{CO2}$ and $\ce{CaCO3}$:

$$\Delta_r H^\ominus = [(-635.1) + (-393.5)] - (-1206.9) = +178.3~\text{kJ mol}^{-1}$$

The positive value confirms that decomposing calcium carbonate is endothermic — a chemical engineer must supply heat to drive it. This first worked example puts the rule to work on a multi-term reaction.

Worked Example 1 · ΔfH summation

For $\ce{Fe2O3(s) + 3H2(g) -> 2Fe(s) + 3H2O(l)}$, calculate $\Delta_r H^\ominus$ given $\Delta_f H^\ominus(\ce{H2O, l}) = -285.83$ and $\Delta_f H^\ominus(\ce{Fe2O3, s}) = -824.2~\text{kJ mol}^{-1}$.

Step 1 — set element baselines. By convention $\Delta_f H^\ominus(\ce{Fe, s}) = 0$ and $\Delta_f H^\ominus(\ce{H2, g}) = 0$, since both are elements in their reference states.

Step 2 — apply the rule with coefficients. Products give $2(0) + 3(-285.83)$; reactants give $1(-824.2) + 3(0)$.

$$\Delta_r H^\ominus = 3(-285.83) - (-824.2) = -857.5 + 824.2 = -33.3~\text{kJ mol}^{-1}$$

Result. $\Delta_r H^\ominus = -33.3~\text{kJ mol}^{-1}$ — exothermic. Had the equation been written with half-coefficients, the answer would halve to $-16.6~\text{kJ mol}^{-1}$, demonstrating that enthalpy is extensive.

Go Deeper

The summation rule is one face of a more general principle. See how indirect routes combine in Hess's Law of Constant Heat Summation.

Enthalpy of Combustion

The standard enthalpy of combustion, $\Delta_c H^\ominus$, is the enthalpy change per mole of a substance when it is completely burnt with all reactants and products in their standard states. Combustion reactions are always exothermic, which is why they dominate industry, rocketry and everyday fuels. The cooking gas in cylinders is mostly butane, and burning one mole releases 2658 kJ:

$\ce{C4H10(g) + 13/2 O2(g) -> 4CO2(g) + 5H2O(l)}$;  $\Delta_c H^\ominus = -2658.0~\text{kJ mol}^{-1}$

Glucose combustion releases 2802 kJ per mole via $\ce{C6H12O6(g) + 6O2(g) -> 6CO2(g) + 6H2O(l)}$, $\Delta_c H^\ominus = -2802.0~\text{kJ mol}^{-1}$ — and the body extracts energy from food by the same overall oxidation, though through a long chain of enzyme-mediated steps. Combustion data are valuable precisely because they let us reach formation enthalpies that cannot be measured directly, as the benzene problem below shows.

Worked Example 2 · combustion → formation

Combustion of one mole of benzene at 298 K and 1 atm liberates 3267.0 kJ, forming $\ce{CO2(g)}$ and $\ce{H2O(l)}$. Find $\Delta_f H^\ominus$ of benzene. Take $\Delta_f H^\ominus(\ce{CO2, g}) = -393.5$ and $\Delta_f H^\ominus(\ce{H2O, l}) = -285.83~\text{kJ mol}^{-1}$. (NCERT Problem 5.9)

Target. $\ce{6C(graphite) + 3H2(g) -> C6H6(l)}$, $\Delta_f H^\ominus = ?$

Combustion (given). $\ce{C6H6(l) + 15/2 O2(g) -> 6CO2(g) + 3H2O(l)}$, $\Delta_c H^\ominus = -3267~\text{kJ mol}^{-1}$.

Apply the summation rule to the combustion. The combustion enthalpy equals products minus reactants, where benzene's formation enthalpy is the only unknown:

$$\Delta_c H^\ominus = \big[6\,\Delta_f H^\ominus(\ce{CO2}) + 3\,\Delta_f H^\ominus(\ce{H2O})\big] - \Delta_f H^\ominus(\ce{C6H6})$$

$$-3267 = \big[6(-393.5) + 3(-285.83)\big] - \Delta_f H^\ominus(\ce{C6H6})$$

$$-3267 = (-2361 - 857.49) - \Delta_f H^\ominus(\ce{C6H6}) = -3218.49 - \Delta_f H^\ominus(\ce{C6H6})$$

Solve. $\Delta_f H^\ominus(\ce{C6H6, l}) = -3218.49 - (-3267) = +48.5~\text{kJ mol}^{-1}$. NCERT obtains the value via Hess addition as $\Delta_f H^\ominus = +48.51~\text{kJ mol}^{-1}$ — endothermic, signalling that benzene is energetically less stable than its elements.

Phase-Transition Enthalpies

Phase changes occur at constant pressure and constant temperature, yet still involve heat. The standard enthalpy of fusion ($\Delta_{fus}H^\ominus$) accompanies melting one mole of solid, vaporisation ($\Delta_{vap}H^\ominus$) accompanies boiling one mole of liquid, and sublimation ($\Delta_{sub}H^\ominus$) accompanies a solid passing directly to vapour. All three are endothermic and positive, because each must overcome intermolecular attraction.

TransitionSymbolExample reactionΔH° (kJ mol⁻¹)
Fusion (melting)$\Delta_{fus}H^\ominus$$\ce{H2O(s) -> H2O(l)}$+6.00
Vaporisation (boiling)$\Delta_{vap}H^\ominus$$\ce{H2O(l) -> H2O(g)}$+40.79
Sublimation (dry ice)$\Delta_{sub}H^\ominus$$\ce{CO2(s) -> CO2(g)}$+25.2 (at 195 K)
Sublimation (naphthalene)$\Delta_{sub}H^\ominus$$\ce{C10H8(s) -> C10H8(g)}$+73.0

The magnitude reflects intermolecular force strength. Strong hydrogen bonds hold water molecules tightly, so its $\Delta_{vap}H^\ominus$ is large; acetone, held only by weaker dipole–dipole interactions, vaporises with much less heat. Sublimation is conceptually fusion plus vaporisation in one step, which is why $\Delta_{sub}H^\ominus$ values are comparatively large.

Atomisation & Bond Enthalpy

The enthalpy of atomisation, $\Delta_a H^\ominus$, is the enthalpy change on breaking one mole of bonds completely to give atoms in the gas phase. For dihydrogen $\ce{H2(g) -> 2H(g)}$, $\Delta_a H^\ominus = 435.0~\text{kJ mol}^{-1}$; for methane $\ce{CH4(g) -> C(g) + 4H(g)}$, $\Delta_a H^\ominus = 1665~\text{kJ mol}^{-1}$. For a metal it equals the sublimation enthalpy: $\ce{Na(s) -> Na(g)}$, $\Delta_a H^\ominus = 108.4~\text{kJ mol}^{-1}$.

For a diatomic molecule the bond dissociation enthalpy equals the atomisation enthalpy — for instance $\ce{Cl2(g) -> 2Cl(g)}$, $\Delta_{Cl-Cl}H^\ominus = 242~\text{kJ mol}^{-1}$ and $\ce{O2(g) -> 2O(g)}$, $\Delta_{O=O}H^\ominus = 428~\text{kJ mol}^{-1}$. In polyatomic molecules, the four successive C–H dissociations in methane cost different amounts (427, 439, 452 and 347 kJ mol⁻¹), so we use the mean bond enthalpy: $\Delta_{C-H}H^\ominus = \tfrac{1}{4}(1665) = 416~\text{kJ mol}^{-1}$.

The reaction enthalpy in the gas phase then follows from a simple balance of bonds broken against bonds formed:

$$\Delta_r H^\ominus = \sum (\text{bond enthalpies})_{\text{reactants}} - \sum (\text{bond enthalpies})_{\text{products}}$$

In words, $\Delta_r H^\ominus$ equals the energy needed to break all reactant bonds minus the energy needed to break all product bonds. The relationship is approximate and holds only when every reactant and product is gaseous.

Worked Example 3 · bond-enthalpy method (NEET 2018)

The bond dissociation energies of $\ce{X2}$, $\ce{Y2}$ and $\ce{XY}$ are in the ratio $1 : 0.5 : 1$. $\Delta H$ for the formation of $\ce{XY}$ is $-200~\text{kJ mol}^{-1}$. Find the bond dissociation energy of $\ce{X2}$.

Set up. Let the bond enthalpies be $\ce{X2} = a$, $\ce{Y2} = 0.5a$, $\ce{XY} = a$. The formation reaction is $\ce{1/2 X2 + 1/2 Y2 -> XY}$.

Apply the bond balance. Bonds broken in reactants $= \tfrac{1}{2}a + \tfrac{1}{2}(0.5a)$; bond formed in product $= a$.

$$\Delta_f H^\ominus = \left(\tfrac{a}{2} + \tfrac{0.5a}{2}\right) - a = \frac{1.5a}{2} - a = 0.75a - a = -0.25a$$

Solve. $-200 = -0.25a \;\Rightarrow\; a = \dfrac{-200}{-0.25} = 800~\text{kJ mol}^{-1}$.

Result. The bond dissociation energy of $\ce{X2}$ is $800~\text{kJ mol}^{-1}$ — matching the official key, option (3).

Lattice & Solution Enthalpy

The lattice enthalpy of an ionic compound is the enthalpy change when one mole of the solid dissociates into its gaseous ions: $\ce{NaCl(s) -> Na+(g) + Cl^-(g)}$, $\Delta_{lattice}H^\ominus = +788~\text{kJ mol}^{-1}$. It cannot be measured directly, so it is found indirectly through a Born–Haber cycle, which assembles sublimation, ionisation, dissociation and electron-gain enthalpies. Because enthalpy is a state function, the sum of enthalpy changes around the closed cycle is zero (Hess's law), and the lattice enthalpy emerges as $788$ kJ from $411.2 + 108.4 + 121 + 496 - 348.6$ for NaCl.

Figure 2 Na(s) + ½Cl₂(g) Na(g) + Cl(g) Na⁺(g) + Cl⁻(g) NaCl(s) +ΔsubH, +½ΔbondH +Δ_iH, +Δ_egH −Δlattice H ΔfH° (direct route)

Born–Haber cycle for NaCl. The solid is built either directly (green) or via gaseous atoms and ions (purple, then lattice formation in red). Because enthalpy is a state function, the sum of changes around the closed cycle is zero — applying Hess's law gives $\Delta_{lattice}H^\ominus = 411.2 + 108.4 + 121 + 496 - 348.6 = +788~\text{kJ mol}^{-1}$ for the dissociation $\ce{NaCl(s) -> Na+(g) + Cl^-(g)}$.

When the solid dissolves, the lattice must break (endothermic) while the freed ions are hydrated (exothermic). The enthalpy of solution is the sum of these competing terms:

$$\Delta_{sol}H^\ominus = \Delta_{lattice}H^\ominus + \Delta_{hyd}H^\ominus$$

For sodium chloride, $\Delta_{lattice}H^\ominus = +788$ and $\Delta_{hyd}H^\ominus = -784~\text{kJ mol}^{-1}$, so $\Delta_{sol}H^\ominus = +4~\text{kJ mol}^{-1}$ — barely any heat change, which is why NaCl dissolves so readily. For most ionic salts $\Delta_{sol}H^\ominus$ is positive and dissolution is endothermic, so solubility usually rises with temperature; if the lattice enthalpy is very large, the salt may scarcely dissolve at all.

NEET Trap

Lattice enthalpy in NCERT is for dissociation, so it is positive

NCERT defines lattice enthalpy as the endothermic break-up $\ce{NaCl(s) -> Na+(g) + Cl^-(g)}$ with $\Delta_{lattice}H^\ominus = +788~\text{kJ mol}^{-1}$. Some other texts define it for the reverse (lattice formation), giving a negative number. Use the NCERT sign convention in $\Delta_{sol}H^\ominus = \Delta_{lattice}H^\ominus + \Delta_{hyd}H^\ominus$ or your solution enthalpy will come out wrong.

All Enthalpy Types at a Glance

Every named enthalpy is ultimately a labelled $\Delta_r H^\ominus$ for a specific kind of process. The table consolidates each type, its symbol, sign behaviour and a representative reaction drawn from NCERT Unit 5.

Enthalpy typeSymbolDefined forSignExample reaction
Reaction$\Delta_r H^\ominus$One mole of reaction as written±$\ce{CaCO3(s) -> CaO(s) + CO2(g)}$
Formation$\Delta_f H^\ominus$1 mol compound from elements±$\ce{C(graphite) + 2H2(g) -> CH4(g)}$
Combustion$\Delta_c H^\ominus$Complete burning of 1 mol− (always)$\ce{C4H10(g) + 13/2 O2(g) -> 4CO2(g) + 5H2O(l)}$
Fusion$\Delta_{fus}H^\ominus$Melting 1 mol solid+ (always)$\ce{H2O(s) -> H2O(l)}$
Vaporisation$\Delta_{vap}H^\ominus$Boiling 1 mol liquid+ (always)$\ce{H2O(l) -> H2O(g)}$
Sublimation$\Delta_{sub}H^\ominus$Solid → vapour, 1 mol+ (always)$\ce{CO2(s) -> CO2(g)}$
Atomisation$\Delta_a H^\ominus$1 mol bonds → gaseous atoms+ (always)$\ce{CH4(g) -> C(g) + 4H(g)}$
Bond enthalpy$\Delta_{bond}H^\ominus$Breaking 1 mol of a bond (gas)+ (always)$\ce{H2(g) -> 2H(g)}$
Lattice$\Delta_{lattice}H^\ominus$Ionic solid → gaseous ions+ (NCERT)$\ce{NaCl(s) -> Na+(g) + Cl^-(g)}$
Solution$\Delta_{sol}H^\ominus$1 mol solute dissolved± (usually +)$\ce{NaCl(s) ->[\text{aq}] Na+(aq) + Cl^-(aq)}$
Quick Recap

Enthalpies of Different Reactions in one screen

  • $\Delta_r H^\ominus$ is the standard reaction enthalpy; standard state = pure substance at 1 bar. Scale it with coefficients; reverse the equation → reverse the sign.
  • $\Delta_f H^\ominus$ forms one mole of compound from elements in reference states; $\Delta_f H^\ominus$ of any element in its reference state is zero.
  • Master formula: $\Delta_r H^\ominus = \sum \Delta_f H^\ominus(\text{products}) - \sum \Delta_f H^\ominus(\text{reactants})$, weighted by coefficients.
  • $\Delta_c H^\ominus$ (combustion) is always negative; fusion, vaporisation, sublimation, atomisation and bond enthalpies are always positive.
  • Bond-enthalpy route (gas phase only): $\Delta_r H^\ominus = \sum \text{B.E.(reactants)} - \sum \text{B.E.(products)}$.
  • $\Delta_{sol}H^\ominus = \Delta_{lattice}H^\ominus + \Delta_{hyd}H^\ominus$; for NaCl, $+788 - 784 = +4~\text{kJ mol}^{-1}$.

NEET PYQ Snapshot — Enthalpies of Different Reactions

Bond-enthalpy and formation/combustion items recur across NEET; here are the cleanest from 2018–2025.

NEET 2018 · Q.80

The bond dissociation energies of $\ce{X2}$, $\ce{Y2}$ and $\ce{XY}$ are in the ratio $1 : 0.5 : 1$. $\Delta H$ for the formation of $\ce{XY}$ is $-200~\text{kJ mol}^{-1}$. The bond dissociation energy of $\ce{X2}$ will be —

  1. 200 kJ mol⁻¹
  2. 100 kJ mol⁻¹
  3. 800 kJ mol⁻¹
  4. 400 kJ mol⁻¹
Answer: (3) 800 kJ mol⁻¹

Let $\ce{X2}=a$, $\ce{Y2}=0.5a$, $\ce{XY}=a$. For $\ce{1/2 X2 + 1/2 Y2 -> XY}$: $\Delta H = (\tfrac{a}{2} + \tfrac{0.5a}{2}) - a = -0.25a$. So $-200 = -0.25a \Rightarrow a = 800~\text{kJ mol}^{-1}$.

NEET 2025 · Q.85

For $\ce{C(s) + 2H2(g) -> CH4(g)}$, $\Delta H = -74.8~\text{kJ mol}^{-1}$. Which energy-profile diagram correctly represents the reaction? [R → reactants; P → products]

Answer: (2)

$\Delta H = -74.8~\text{kJ mol}^{-1}$ is negative, so the reaction is exothermic: the products (P) must lie below the reactants (R) on the enthalpy axis. Only the diagram showing P lower than R fits.

NEET 2023 · Q.91

Which is the correct relation between change in enthalpy and change in internal energy?

  1. $\Delta H + \Delta U = \Delta n_g R$
  2. $\Delta H = \Delta U - \Delta n_g RT$
  3. $\Delta H = \Delta U + \Delta n_g RT$
  4. $\Delta H - \Delta U = -\Delta n_g RT$
Answer: (3)

At constant pressure $\Delta H = \Delta U + p\Delta V$, and for gaseous reactions $p\Delta V = \Delta n_g RT$, giving $\Delta H = \Delta U + \Delta n_g RT$ — the bridge used when converting tabulated $\Delta_r H$ to $\Delta_r U$.

NEET 2020 · Q.144

For the reaction $\ce{2Cl(g) -> Cl2(g)}$, the correct option is —

  1. $\Delta_r H > 0$ and $\Delta_r S < 0$
  2. $\Delta_r H < 0$ and $\Delta_r S > 0$
  3. $\Delta_r H < 0$ and $\Delta_r S < 0$
  4. $\Delta_r H > 0$ and $\Delta_r S > 0$
Answer: (3)

Forming a $\ce{Cl-Cl}$ bond releases energy (bond formation is exothermic), so $\Delta_r H < 0$; two gaseous atoms collapse into one molecule, lowering disorder, so $\Delta_r S < 0$.

FAQs — Enthalpies of Different Reactions

The conceptual distinctions NEET examiners test most often.

What is the difference between standard enthalpy of formation and standard enthalpy of reaction?

Standard enthalpy of formation (ΔfH°) is a special case of the standard enthalpy of reaction (ΔrH°) in which exactly one mole of a compound is formed from its constituent elements in their most stable reference states at 1 bar. Every ΔfH° is a ΔrH°, but not every ΔrH° is a ΔfH°. For example, CaO(s) + CO2(g) → CaCO3(s) is a reaction enthalpy, not a formation enthalpy, because the carbonate is built from compounds rather than from Ca, C and O2 directly.

Why is the standard enthalpy of formation of an element zero?

By convention, the standard enthalpy of formation of an element in its reference state — its most stable state of aggregation at 25 °C and 1 bar — is taken as zero. So ΔfH° of H2(g), O2(g), C(graphite) and S(rhombic) are all zero. This convention sets the baseline against which all compound formation enthalpies are measured, which is why ΔrH° can be computed as the sum of product formation enthalpies minus reactant formation enthalpies.

How do you calculate enthalpy of reaction from bond enthalpies?

For gas-phase reactions, ΔrH° equals the sum of bond enthalpies of all bonds broken in the reactants minus the sum of bond enthalpies of all bonds formed in the products. Breaking bonds absorbs energy and forming bonds releases it, so a reaction is exothermic when stronger or more numerous bonds form in the products. This relationship is approximate and is valid only when every reactant and product is in the gaseous state.

Why are all enthalpies of fusion and vaporisation positive?

Melting a solid and vaporising a liquid both require heat to overcome intermolecular attractions, so they are endothermic and their standard enthalpy changes (ΔfusH° and ΔvapH°) are positive. The magnitude depends on the strength of intermolecular forces: water, held by strong hydrogen bonds, has a larger ΔvapH° than acetone, whose dipole-dipole interactions are weaker. The reverse processes — freezing and condensation — release the same magnitude of heat and are therefore exothermic.

What is lattice enthalpy and why can it not be measured directly?

Lattice enthalpy is the enthalpy change when one mole of an ionic solid dissociates completely into its gaseous ions, for example NaCl(s) → Na+(g) + Cl−(g), ΔlatticeH° = +788 kJ mol−1. It cannot be measured directly because the process is experimentally inaccessible, so it is obtained indirectly through a Born–Haber cycle. Hess's law is applied around the cycle, where the sum of all enthalpy changes is zero, allowing the lattice enthalpy to be found from sublimation, ionisation, dissociation and electron-gain enthalpies.

How is enthalpy of solution related to lattice enthalpy and hydration enthalpy?

When an ionic compound dissolves, the lattice must break apart (endothermic, +ΔlatticeH°) while the freed ions are hydrated (exothermic, −ΔhydH°). The enthalpy of solution is their sum: ΔsolH° = ΔlatticeH° + ΔhydH°. For NaCl, ΔlatticeH° = +788 kJ mol−1 and ΔhydH° = −784 kJ mol−1, giving ΔsolH° = +4 kJ mol−1, so dissolving NaCl involves very little heat change. When lattice enthalpy greatly exceeds hydration enthalpy, the salt may barely dissolve at all.