Enthalpy, Heat Capacity & Calorimetry
Most chemical laboratory experiments and industrial reactions occur in open vessels under constant atmospheric pressure. Under constant pressure, heat exchanged is not equal to the change in internal energy (ΔU). To quantify constant-pressure thermal changes, thermodynamics introduces the state function Enthalpy (H).
1. Enthalpy (H) & Constant Pressure Heat (qp)
Enthalpy is defined as the total heat content of a system, mathematically given by:
Since internal energy U, pressure P, and volume V are state functions, Enthalpy (H) is also an extensive state function.
For a process occurring at constant pressure (P = constant):
ΔH = ΔU + Δ(PV) = ΔU + PΔV
From the First Law (ΔU = qp − PΔV), substituting ΔU + PΔV gives:
Similarly, at constant volume (ΔV = 0, w = 0):
2. Fundamental Relation: ΔH = ΔU + ΔngRT
For chemical reactions involving gaseous species, the volume change is primarily governed by the change in the number of gaseous moles. For an ideal gas, PV = nRT. At constant temperature T:
Δ(PV) = Δ(ngRT) = ΔngRT
Where Δng = ∑ ng(products) − ∑ ng(reactants) (strictly count ONLY species in the gaseous state (g); ignore solids (s) and liquids (l)).
| Condition | Physical Meaning | Example Reaction |
|---|---|---|
| Δng = 0 | ΔH = ΔU (No expansion work) | H2(g) + I2(g) → 2HI(g) (Δng = 2 − 2 = 0) |
| Δng > 0 | ΔH > ΔU (System expands, work done by system) | PCl5(g) → PCl3(g) + Cl2(g) (Δng = 2 − 1 = +1) |
| Δng < 0 | ΔH < ΔU (System contracts, work done on system) | N2(g) + 3H2(g) → 2NH3(g) (Δng = 2 − 4 = −2) |
3. Heat Capacity & Mayer's Relation (Cp − Cv = R)
The Heat Capacity (C) of a system is the quantity of heat required to raise its temperature by 1 Kelvin (or 1 °C):
- Specific Heat Capacity (c): Heat capacity per unit mass (J g−1 K−1 or J kg−1 K−1).
- Molar Heat Capacity (Cm): Heat capacity per mole (J mol−1 K−1).
Heat Capacity at Constant Volume (Cv) & Constant Pressure (Cp)
At constant volume: qv = ΔU ⇒ Cv = (∂U / ∂T)v
At constant pressure: qp = ΔH ⇒ Cp = (∂H / ∂T)p
Derivation of Mayer's Relation (Cp − Cv = R) for Ideal Gas
From enthalpy definition for 1 mole of ideal gas: H = U + PV = U + RT.
Differentiating with respect to temperature T:
dH/dT = dU/dT + R
The ratio γ = Cp / Cv is the Poisson ratio (adiabatic exponent):
- Monatomic gas (He, Ne, Ar): Cv = (3/2)R, Cp = (5/2)R ⇒ γ = 5/3 ≈ 1.67
- Diatomic gas (N2, O2, CO): Cv = (5/2)R, Cp = (7/2)R ⇒ γ = 7/5 = 1.40
- Non-linear triatomic gas (H2O, SO2): Cv = 3R, Cp = 4R ⇒ γ = 4/3 ≈ 1.33
Calorimetry Apparatus: Bomb Calorimeter vs Coffee-Cup Calorimeter
BOMB CALORIMETER (Constant Volume, ΔV = 0) COFFEE-CUP CALORIMETER (Constant Pressure)
+------------------------------------------+ +------------------------------------------+
| [Thermometer] [Motor Stirrer] | | [Thermometer] [Stirrer] |
| | | | | | | |
| +--|----------------|--+ | | +--|---------------|--+ |
| | v v | (Water Bath)| | | v v | |
| | .................. | | | === Styrofoam Insulated Cup === |
| | . +------------+ . | | | | | |
| | . | Heavy Steel| . | | | | Reacting Aqueous Soln | |
| | . | Bomb Vessel| . | | | | q_rxn = -q_calorimeter | |
| | . | (Ignition) | . | | | | q_rxn = -(m * c * ΔT) | |
| | . +------------+ . | | | +---------------------------+ |
| +----------------------+ | +------------------------------------------+
| q_v = C_cal * ΔT = ΔU | q_p = (m_sol * c_sol + C_cal) * ΔT = ΔH |
+------------------------------------------+ +------------------------------------------+
4. Calorimetric Formulae for Bomb & Solution Calorimetry
Molar ΔU = (qv / msubstance) × Mmolar
Then calculate ΔH using: ΔH = ΔU + ΔngRT
5. Solved High-Yield Numerical Examples & Exam MCQs
1. Write the balanced combustion equation:
C6H6(l) + 7.5 O2(g) → 6 CO2(g) + 3 H2O(l)
2. Calculate Δng (gaseous species only):
Δng = ng(products) − ng(reactants) = 6 − 7.5 = −1.5 mol
3. Identify ΔU: Bomb calorimeter measures constant volume heat ⇒ ΔU = −3267.0 kJ mol−1
4. Apply ΔH = ΔU + ΔngRT:
ΔngRT = (−1.5 mol) × (8.314 × 10−3 kJ K−1 mol−1) × (298 K) = −3.716 kJ
ΔcH° = −3267.0 + (−3.716) = −3270.72 kJ mol−1.
Notice that ΔH is slightly more negative than ΔU because work is done on the system by the atmosphere as volume contracts (Δng < 0).
Show answer
Δng = moles of gaseous products − moles of gaseous reactants = 2 − (1 + 3) = −2.
Substituting into ΔH = ΔU + ΔngRT gives ΔH = ΔU + (−2)RT = ΔU − 2RT.
Show answer
By Mayer's relation, for any ideal gas regardless of atomicity, Cp,m − Cv,m = R. For monoatomic gas, Cv = 1.5 R and Cp = 2.5 R, whose difference is exactly R.
6. Frequently Asked Questions (FAQs)
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