Chemical Thermodynamics deals with energy changes in chemical reactions and determines whether a reaction is spontaneous.
Overview
graph TD
A[Chemical Thermodynamics] --> B[First Law]
A --> C[Enthalpy]
A --> D[Second Law]
A --> E[Gibbs Energy]
C --> C1[Hess's Law]
C --> C2[Types of ΔH]
D --> D1[Entropy]
E --> E1[Spontaneity]System and Surroundings
Types of Systems
| Type | Matter Exchange | Energy Exchange |
|---|---|---|
| Open | Yes | Yes |
| Closed | No | Yes |
| Isolated | No | No |
State Functions
Properties that depend only on state, not path:
- Internal Energy (U)
- Enthalpy (H)
- Entropy (S)
- Gibbs Energy (G)
Path functions: Work (W), Heat (Q)
First Law of Thermodynamics
$$\boxed{\Delta U = q + w}$$For processes at constant volume:
$$\Delta U = q_V$$For processes at constant pressure:
$$\Delta H = q_P$$Work Done
Expansion work:
$$w = -P_{ext}\Delta V$$Reversible isothermal:
$$w = -nRT\ln\frac{V_2}{V_1} = -2.303nRT\log\frac{V_2}{V_1}$$Enthalpy (H)
$$H = U + PV$$At constant pressure:
$$\boxed{\Delta H = \Delta U + P\Delta V = \Delta U + \Delta n_g RT}$$where $\Delta n_g$ = (moles of gaseous products) - (moles of gaseous reactants)
Heat Capacity
At constant volume: $C_V = \frac{dU}{dT}$
At constant pressure: $C_P = \frac{dH}{dT}$
$$\boxed{C_P - C_V = R}$$(for ideal gas)
Types of Enthalpy Changes
| Type | Symbol | Definition |
|---|---|---|
| Formation | $\Delta_f H°$ | 1 mole of compound from elements |
| Combustion | $\Delta_c H°$ | Complete burning with O₂ |
| Atomization | $\Delta_a H°$ | Conversion to gaseous atoms |
| Sublimation | $\Delta_{sub} H°$ | Solid to gas |
| Ionization | $\Delta_{ion} H$ | Removal of electron |
| Bond dissociation | $\Delta_{bond} H°$ | Breaking one mole of bonds |
| Neutralization | $\Delta_{neut} H°$ | Acid + Base → Salt + Water |
Standard States
- Gases: 1 bar pressure
- Solutions: 1 M concentration
- Temperature: 298 K (unless specified)
Hess’s Law
Enthalpy change is independent of path:
$$\Delta H_{overall} = \sum \Delta H_{steps}$$Applications
- Calculate ΔH for reactions that can’t be measured directly
- Add equations to get desired equation
Bond Enthalpy
$$\Delta H_{rxn} = \sum(\text{Bond energies of reactants}) - \sum(\text{Bond energies of products})$$or
$$\Delta H_{rxn} = \sum\Delta H(\text{bonds broken}) - \sum\Delta H(\text{bonds formed})$$Entropy (S)
Measure of disorder or randomness.
$$\Delta S = \frac{q_{rev}}{T}$$Second Law of Thermodynamics
$$\boxed{\Delta S_{universe} = \Delta S_{system} + \Delta S_{surroundings} \geq 0}$$- Spontaneous: $\Delta S_{universe} > 0$
- Equilibrium: $\Delta S_{universe} = 0$
- Non-spontaneous: $\Delta S_{universe} < 0$
Factors Increasing Entropy
- Solid → Liquid → Gas
- Increase in temperature
- Increase in volume
- Increase in number of moles
- Dissolving (usually)
Gibbs Energy (G)
$$G = H - TS$$ $$\boxed{\Delta G = \Delta H - T\Delta S}$$Spontaneity Criterion
| ΔH | ΔS | ΔG | Spontaneity |
|---|---|---|---|
| - | + | Always - | Always spontaneous |
| + | - | Always + | Never spontaneous |
| - | - | - at low T | Spontaneous at low T |
| + | + | - at high T | Spontaneous at high T |
At Equilibrium
$$\Delta G = 0$$ $$T_{eq} = \frac{\Delta H}{\Delta S}$$Standard Gibbs Energy
$$\boxed{\Delta G° = -RT\ln K = -2.303RT\log K}$$ $$\Delta G = \Delta G° + RT\ln Q$$where Q = reaction quotient, K = equilibrium constant
At Equilibrium (Q = K)
$$\Delta G = 0$$ $$\Delta G° = -RT\ln K$$Practice Problems
Calculate ΔU when ΔH = -280 kJ and Δn_g = -2 at 300 K.
For a reaction, ΔH = -200 kJ/mol and ΔS = -50 J/mol·K. At what temperature will it become non-spontaneous?
Given: $\Delta G° = -30$ kJ/mol at 300 K. Calculate the equilibrium constant.
Calculate ΔS for the universe when 1 mol of ice melts at 273 K. (ΔH_fus = 6 kJ/mol)