Energy Conservation in Chemical Reactions: From Bond Energies to Thermodynamics


1. Core concepts

  • Law of Conservation of Energy: Energy cannot be created or destroyed; it can only be transformed from one form to another. In chemistry this principle appears as the conservation of total energy of the system plus its surroundings during a reaction.

  • Internal energy (U): The sum of kinetic and potential energies of particles in a system. Changes in internal energy, ΔU, reflect changes in molecular motion and interactions (e.g., bond energies, intermolecular forces).

  • Enthalpy (H): A state function defined as H = U + PV. For reactions at constant pressure, the change in enthalpy, ΔH, equals the heat exchanged with the surroundings (q_p). For most classroom reactions performed at constant atmospheric pressure, ΔH is the heat change observed.

  • Heat (q) and work (w): The first law of thermodynamics states ΔU = q + w. Heat is energy transferred due to temperature difference; work often refers to pressure–volume work, w = −PΔV, for expansions/compressions.

  • Exothermic vs. endothermic:

    • Exothermic reaction: releases heat to the surroundings, ΔH < 0.
    • Endothermic reaction: absorbs heat from the surroundings, ΔH > 0.
  • Bond energies and reaction energetics: Chemical bonds store potential energy. During a reaction, some bonds break (energy input required) and new bonds form (energy released). The net energy change depends on the balance between these processes.


2. Energetic bookkeeping — how to calculate heat and internal energy changes

At constant pressure (common in labs), the heat observed equals the enthalpy change: q_p = ΔH

For reactions where gases expand or compress noticeably, account for PV work: ΔU = ΔH − Δ(n_gas)RT where Δ(n_gas) is the change in moles of gaseous species (useful approximation for ideal gases at temperature T).

Use bond enthalpies for rough estimates of ΔH: ΔH ≈ Σ(bond energies of bonds broken) − Σ(bond energies of bonds formed) This gives a qualitative/approximate value because bond enthalpy tables are averages and neglect molecular environment differences.

Calorimetry: measure temperature change to determine heat: q = m·c·ΔT where m is mass of the sample (or solvent), c is specific heat capacity, and ΔT is temperature change. For solution calorimetry, assume heat lost by reaction equals heat gained by solution (with sign change).


3. Thermochemistry examples and step-by-step calculations

Example 1 — Combustion of methane (conceptual energy flow) CH4(g) + 2 O2(g) → CO2(g) + 2 H2O(l)

  • Breaking bonds: C–H and O=O bonds require energy.
  • Forming bonds: C=O and O–H bonds release energy. If released energy (forming) > required energy (breaking), net heat is released → exothermic. In practice, methane combustion is strongly exothermic (ΔH° ≈ −890 kJ/mol).

Example 2 — Using bond enthalpies (approximate) Calculate approximate ΔH for the hydrogenation of ethene: C2H4 + H2 → C2H6

Using average bond enthalpies (kJ/mol):

  • Break: C=C (614), H–H (436) → total broken = 1050
  • Form: 2 × C–H (412 each) → total formed = 824 ΔH ≈ 1050 − 824 = +226 kJ/mol (positive) Conclusion: Rough bond-enthalpy method predicts an endothermic process — note this contradicts accurate tabulated thermodynamic values because average bond enthalpies are crude; actual hydrogenation of ethene is exothermic (~ −136 kJ/mol) because product stabilization and specific molecular context matter.

Example 3 — Calorimetry: neutralization Consider mixing 50.0 mL of 1.00 M HCl with 50.0 mL of 1.00 M NaOH at 25.0 °C. The solution mass ≈ 100.0 g, specific heat c ≈ 4.184 J·g−1·°C−1. The measured temperature rises to 30.0 °C.

  • ΔT = 5.0 °C
  • q_solution = m·c·ΔT = 100.0 g × 4.184 J/g·°C × 5.0 °C = 2092 J Assuming no heat loss, q_reaction = −q_solution = −2092 J. Moles of limiting reactant (HCl) = 0.0500 L × 1.00 M = 0.0500 mol. ΔH per mole ≈ −2092 J / 0.0500 mol = −41,840 J/mol ≈ −41.8 kJ/mol (close to typical ΔH° for strong acid-base neutralization ≈ −57 kJ/mol when factoring real heat losses and solution assumptions).

4. Electrochemical and non-thermal energy transfers

Not all energy exchanged in reactions is heat. Reactions can transfer energy as:

  • Electrical work (in galvanic cells): chemical energy → electrical energy.
  • Light (photochemical reactions): absorbed photons drive reactions (e.g., photosynthesis), or excited species emit light (chemiluminescence).
  • Mechanical work (explosions do rapid expansion doing work on surroundings).

In electrochemistry, the maximum non-expansion work is related to the change in Gibbs free energy: ΔG = −nFE_max where n is number of electrons transferred, F is Faraday’s constant, and E_max is the cell potential under reversible conditions.


5. Connecting energy conservation with spontaneity: Gibbs free energy

Energy conservation (first law) tells you energy balance but not whether a reaction will occur spontaneously. Spontaneity at constant temperature and pressure is governed by Gibbs free energy: ΔG = ΔH − TΔS

  • If ΔG < 0, process is spontaneous as written.
  • If ΔG > 0, non-spontaneous.

Thus a reaction can be exothermic (ΔH < 0) but non-spontaneous if entropy decreases enough that TΔS outweighs ΔH.


6. Common student pitfalls

  • Confusing heat (q) and enthalpy (ΔH): at constant pressure they are equal, but they are conceptually different.
  • Treating bond enthalpy calculations as exact — they’re approximations.
  • Forgetting sign conventions: heat released is negative for system; heat absorbed is positive.
  • Ignoring work other than PV work (electrical work in batteries, light, etc.).

7. Practice problems with solutions

Problem A — Heat of reaction (calorimetry) You dissolve 0.500 mol of KNO3 in 250.0 g of water. The water’s temperature falls from 21.0 °C to 17.2 °C. Assume c_water = 4.184 J·g−1·°C−1 and that solution mass ≈ water mass. Calculate ΔH per mole for the dissolution (assume constant pressure, no heat loss).

Solution: ΔT = 17.2 − 21.0 = −3.8 °C q_solution = m·c·ΔT = 250.0 g × 4.184 J/g·°C × (−3.8 °C) = −3975 J q_reaction = −q_solution = +3975 J (reaction absorbed heat) ΔH per mole = 3975 J / 0.500 mol = +7950 J/mol ≈ +7.95 kJ/mol (endothermic dissolution).

Problem B — Using Hess’s law Given: C(s) + O2(g) → CO2(g) ΔH° = −393.5 kJ 2 CO(g) + O2(g) → 2 CO2(g) ΔH° = −566.0 kJ Find ΔH° for: C(s) + ⁄2 O2(g) → CO(g)

Solution sketch: Write known reactions so their combination yields target. From first: C + O2 → CO2 (−393.5). From second, divide by 2: CO(g) + ⁄2 O2 → CO2(g) (−283.0). Reverse the half-second equation to get CO2 → CO + ⁄2 O2, ΔH = +283.0 kJ. Add to first: (C + O2 → CO2) + (CO2 → CO + ⁄2 O2) gives C + ⁄2 O2 → CO. ΔH = −393.5 + 283.0 = −110.5 kJ.

Problem C — Bond enthalpy estimate Using average bond enthalpies (kJ/mol): C≡C 839, C–H 412, H–H 436, C–C 348. Estimate ΔH for: HC≡CH + H2 → H2C=CH2

Break: C≡C (839) + H–H (436) = 1275 Form: C=C (614) + 2·C–H (2·412 = 824) = 1438 ΔH ≈ 1275 − 1438 = −163 kJ/mol (approximate; real value may differ). Conclusion: approx exothermic.


8. Study tips and experiments to build intuition

  • Use calorimetry lab exercises (neutralization, dissolution) to relate measured temperature changes to ΔH.
  • Practice Hess’s law problems to become comfortable shifting and combining reactions.
  • Compare bond enthalpy estimates with tabulated ΔH° values to see limitations of approximations.
  • Visualize energy profiles (reaction coordinate diagrams): show reactants, products, activation energy, and ΔH. This links kinetic barriers with thermodynamic energy changes.
  • For electrochemistry, build simple Daniell cell and measure voltage; relate measured E to ΔG.

9. Quick reference (cheat-sheet)

  • First law: ΔU = q + w
  • At constant pressure: q_p = ΔH
  • Bond enthalpy estimate: ΔH ≈ Σ(bonds broken) − Σ(bonds formed)
  • Gibbs free energy: ΔG = ΔH − TΔS (spontaneity: ΔG < 0)
  • Exothermic: ΔH < 0 (heat released). Endothermic: ΔH > 0 (heat absorbed).

Energy conservation provides the arithmetic of chemical reactions; combining it with entropy and kinetics explains whether reactions occur, how fast, and how much energy changes form. Understanding both the quantitative calculations and the conceptual pictures (bond breaking/forming, energy diagrams, calorimetry) gives students a clear, practical grasp of reaction energetics.

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