Gen Chem II: Chapter 17
First Law of Thermodynamics
- You can’t win!
- Energy cannot be Created or Destroyed
- The total energy of the universe cannot change
- Energy can transfer from one place to another
- \Delta E{universe} = 0 = \Delta E{system} + \Delta E_{surroundings}
- For an exothermic reaction, “lost” heat from the system goes into the surrounds
- Converted to heat (q)
- Used to do work (w)
Spontaneous Processes
- Thermodynamics predicts whether a process will proceed under the given conditions
- Spontaneity is determined by comparing the free energy of the system before the reaction with the free energy of the system after the reaction
- If the system after reaction has less free energy than before the reaction, the reaction is thermodynamically favorable
- Processes that occur spontaneously in one direction cannot, under the same conditions, also occur spontaneously in the opposite direction
- Examples:
- A lump of sugar spontaneously dissolves in a cup of tea
- Spontaneity can be fast or slow, determined by kinetics
- Thermodynamics focuses on initial and final states to determine spontaneity
Two Factors Determining Spontaneity
- \Delta H (Enthalpy): comparison of the bond energy of the reactants to the products
- Bond energy = amount needed to break a bond.
- \Delta S (Entropy): relates to the randomness/orderliness of a system
- The enthalpy factor is generally more important than the entropy factor in determining spontaneity
Enthalpy
- Related to the internal energy
- Stronger bonds = more stable molecules
- If products are more stable than reactants, energy is released - Exothermic \Delta H = negative
- If reactants are more stable than products, energy is absorbed - Endothermic \Delta H = positive
Entropy
- Entropy (S) is a thermodynamic function that increases as the number of energetically equivalent ways of arranging the components increases
- S = k \ln W
- k = Boltzmann Constant = 1.38 x 10^{-23} J/K
- W is the number of energetically equivalent ways
- Random Systems require less energy than ordered systems
Entropy (W)
- Macrostate A and B can only be achieved through one possible arrangement of particles
- There are 6 possible arrangements that give State C
- Therefore State C has higher entropy than either State A or B
Changes in Entropy, \Delta S
- Entropy change is favorable when the result is a more random system
- \Delta S is positive
- Examples of increases in entropy
- Reactions whose products are in a more disordered state (solid < liquid < gas)
- Reactions which have larger numbers of products molecules than reactant molecules
- Solids dissociating into ions upon dissolving, although not always positive
- Increasing temperature
- When materials change state, the number of microstates it can have changes as well
- For entropy: solid < liquid < gas
- Because the degrees of freedom of motion increases
Changes in Entropy, \Delta S
- Molecules can rotate as well as vibrate and have translational energy.
- This increases with increasing temperature
Changes in Entropy
- Dissolution of a salt generally increases the entropy
- NaCl(s) \rightarrow NaCl(aq)
- Increasing entropy
Changes in Entropy
- More particles dissolved in solution leads to a greater number of possible arrangements (W).
- Also need to consider hydration of ions, which causes water molecules to become ordered around ions.
- For these cases, the entropy change is negative
Predicting the Sign of Entropy Change
- Predict the sign of \Delta S for each process
- a) CO2(g) \rightarrow CO2(l)
- b) Solid iodine sublimes
- c) 2 N2O(g) \rightarrow 2 N2(g) + O_2(g)
- d) dissolving sugar in water
- e) cooling nitrogen gas from 80oC to 20oC
The 2nd Law of Thermodynamics
- The total entropy change of the universe must be positive for a process to be spontaneous
- For a reversible process \Delta S_{universe} = 0
- For irreversible (spontaneous) process \Delta S_{universe} > 0
- \Delta S{universe} = \Delta S{system} + \Delta S_{surroundings}
- If the entropy of the system decreases, then the entropy of the surroundings must increase by a larger amount
- When \Delta S{system} is negative, \Delta S{surroundings} is positive
Heat Flow, Entropy, and the 2nd Law
- Heat must flow from water to ice in order for the entropy of the universe to increase
- The increase in \Delta S_{surroundings} often comes from the heat released in an exothermic reaction
Temperature Dependence of \Delta S_{surroundings}
- When a system process is exothermic (q_{system} negative) it adds heat to the surroundings, increasing the entropy of the surroundings
- When a system process is endothermic, it takes heat from the surroundings, decreasing the entropy of the surroundings
- The amount of the entropy of the surroundings changes is proportional to the magnitude of q_{system}
Temperature Dependence of \Delta S_{surroundings}
- Under conditions of constant pressure q{system} = \Delta H{system}
- Therefore: \Delta S{surroundings} = -\frac{\Delta H{sys}}{T}
- As temperature increases, a given negative enthalpy produces a smaller positive \Delta S_{surroundings}
Calculating Entropy Changes in Surroundings
- The reaction: C3H8(g) + 5 O2(g) \rightarrow 3 CO2(g) + 4 H_2O(g)
- Has \Delta H_{rxn} = -2044 kJ at 25oC. Calculate the entropy change of the surroundings 6860 J/K
Gibbs Free Energy
- G = maximum amount of energy from the system available to do work on the surroundings
- G = H – T(S)
- \Delta G{sys} = \Delta H{sys} - T \Delta S_{sys}
- \Delta G{sys} = \sum n\Delta G{products} - \sum n\Delta G_{reactants}
- When \Delta G < 0, there is a decrease in free energy of the system that is released into the surroundings; therefore a process will be spontaneous when \Delta G is negative
Free Energy Change and Spontaneity
- Free Energy Determines the Direction of Spontaneous Change
- N2(g) + 3H2(g) \rightleftharpoons 2 NH_3(g)
Gibbs Free Energy
- \Delta G will be negative when (reaction will be spontanteous when)
- \Delta H is negative and \Delta S is positive
- Exothermic and more random
- \Delta H is negative and large and \Delta S is negative and small
- \Delta H is positive and small and \Delta S is positive and large, or at high temperatures
- \Delta H is negative and \Delta S is positive
- \Delta G will be positive when endothermic and \Delta S is negative
- When \Delta G = 0 the reaction is at equilibrium
Gibbs Free Energy
| \Delta H | \Delta S | Low Temperature | High Temperature | Example | |||
|---|---|---|---|---|---|---|---|
| Case 1 | - | + | Spontaneous (\Delta G < 0) | Spontaneous (\Delta G < 0) | 2 N2O(g) \rightarrow 2N2(g) + O2(g) | Case 2 | - | - | Spontaneous (\Delta G < 0) | Nonspontaneous (\Delta G > 0) | H2O(l) \rightarrow H2O(s) | Case 3 | + | + | Nonspontaneous (\Delta G > 0) | Spontaneous (\Delta G < 0) | H2O(l) \rightarrow H2O(g) | Case 4 | + | - | Nonspontaneous (\Delta G > 0) | Nonspontaneous (\Delta G > 0) | 3O2(g) \rightarrow 2O_3(g) | ||
Gibbs Free Energy |
- The reaction: CCl4(g) \rightarrow C(s, graphite) + 2 Cl2(g)
- Has \Delta H = 95.7 kJ and \Delta S = 142.2 J/K at 25oC. Calculate \Delta G and determine if it is spontaneous 53.3 kJ
Gibbs Free Energy
- The reaction: CCl4(g) \rightarrow C(s, graphite) + 2 Cl2(g)
- Has \Delta H = 95.7 kJ and \Delta S = 142.2 J/K at 25oC. Calculate \Delta G and determine if it is spontaneous. Calculate the minimum temperature it will be spontaneous. 673K
The 3rd Law of Thermodynamics
- The absolute entropy of a substance is the amount of energy it has due to dispersion of energy through its particle
- The 3rd law states that for a perfect crystal at absolute zero, the absolute entropy = 0 J/mol-K
- Every substance that is not a perfect crystal at absolute zero has some energy from entropy
- Therefore the absolute entropy of substances is always positive
Standard Entropies
- S^o
- Extensive property
- Entropies for 1 mole at 298K for a particular state, a particular allotrope, particular molecular complexity, a particular molar mass, and a particular degree of dissolution
Standard Entropy Values
- For different substances in the same phase, molecular complexity determines which ones have higher entropies
Standard Entropy, Molar Mass
- Greater the molar mass the higher the standard entropy
- Available energy states are more closely spaced, allowing more dispersal of energy through the states
Standard Entropy, Allotropes
- The less constrained the structure of an allotrope is, the larger the entropy
| Allotrope | S^o (J/mol-K) | ||
|---|---|---|---|
| C(s, diamond) | 2.4 | ||
| C(s, graphite) | 5.7 | ||
Standard Entropy, Molecular Complexity |
- Larger, more complex molecules generally have larger standard entropy values
- There is more available energy states, allowing more dispersal of energy through the states
Standard Entropy, Dissolution
- Dissolved solids generally have larger entropy
- Distributing particles throughout the mixture
Standard Entropy Calculation
- Calculate \Delta S^o for the reaction: 4 NH3 (g) + 5 O2(g) \rightarrow 4 NO (g) + 6 H_2O(g)
- 178.8 J/K
Calculating \Delta G^o
- At 25oC: \Delta G^o{reaction} = \sum n\Delta G^o{f(products)} - \sum n\Delta G^o_{f(reactants)}
- At temperatures other than 25oC: assuming the change in \Delta H^o{reaction} and \Delta S^o{reaction} is neglible, \Delta G^o{reaction} = \Delta H^o{reaction} - T\Delta S^o_{reaction}
Calculating \Delta G^o
- Calculate the \Delta G^o reaction at 25oC for the reaction: CH4(g) + 8 O2(g) \rightarrow CO2(g) + 2 H2O(g) + 4 O_3 (g)
- -148.3 kJ
Calculating \Delta G^o
- Calculate the \Delta G^o reaction at 125oC for the reaction: SO2(g) + 0.5 O2(g) \rightarrow SO_2(g)
- \Delta H^o = -98.9 kJ, \Delta S^o = -94.0 J/K
- -65.1 kJ
Free Energy and Reversible Reactions
- The change in free energy is a theoretical limit as to the amount of work that can be done
- If the reaction achieves its theoretical limit, it is a reversible reaction
\Delta G under nonstandard Conditions
- \Delta G = \Delta G^o only when the reactants and products are in the standard states
- Their normal state at that temperature
- Partial pressure of gas = 1 atm
- Concentration = 1M
- Under nonstandard conditions \Delta G = \Delta G^o + RT\ln Q
- At equilibrium \Delta G = 0, \Delta G^o = -RT\ln K
\Delta G under nonstandard Conditions
- H2O(l) \rightleftharpoons H2O(g)
- Water evaporates when \\Delta G is negative
- Water condenses when \Delta G is positive
- Equilibrium is when \Delta G = 0
Calculating \Delta G under non-standard conditions
- Consider the following reaction at 25oC
- 2 NO (g) + O2 (g) \rightarrow 2 NO2(g)
- \Delta G^o_{rxn} = -71.2 kJ
- Calculate \Delta G under the following conditions
- P_{NO} = 0.100 atm
- P{O2} = 0.100 atm
- P{NO2} = 2.00 atm
- Is the reaction more or less spontaneous under these conditions under standard conditions?
Free Energy and Equilibrium Constant
- A(g) ⇌ B(g) K<1
- Standard conditions PA=PB=1 atm Q=1. Pure A to Pure B. Reverse reaction spontaneous
- A(g) ⇌ B(g) K=1
- Standard conditions PA=PB=1 atm Q=1. Pure A to Pure B. At equilibrium
- A(g) ⇌ B(g) K>1
- Standard conditions PA=PB=1 atm Q=1. Pure A to Pure B. Forward reaction spontaneous
Practice
- Estimate the equilibrium constant and position of the equilibrium for the following reaction at 427oC
- N2 (g) + 3 H2 (g) \rightarrow 2 NH_3 (g)
- \Delta H^of of NH3(g) = -46.19kJ
- \Delta S^o of NH_3(g) = 192.5 J/K
- \Delta S^o of N_2(g) = 191.5 J/K
- \Delta S^o of H_2(g) = 130.5 J/K
- 3.45 x 10^{-4}
Temperature Dependence of K
- For an exothermic reaction, increasing the temperature decreases the value of the equilibrium constant
- For an endothermic reaction, increasing the temperature increases the value of the equilibrium constant