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Defining Gibbs Free Energy, G
Whether or not a chemical reaction or a physical change is spontaneous depends on the total entropy change of the entire system.
The total entropy change of the entire system includes both the entropy of the chemical system under investigation AND also the entropy of the surroundings.
That is:
total entropy change |
= |
entropy change change for the chemical system |
+ |
entropy change of the surroundings
|
ΔStotal |
= |
ΔSchemical system |
+ |
ΔSsurroundings
|
While it is often possible to estimate the entropy change for a chemical system, ΔSchemical system, it is almost impossible to determine the entropy change for the surroundings, ΔSsurroundings, given that the surroundings are actually the entire universe!
The problem of estimating the entropy change for the entire universe can be overcome by restricting ourselves to a consideration of chemical processes that occur only at constant temperature and constant pressure.
At constant temperature, the entropy change of the surroundings (ΔSsurroundings) depends on the:
- amount of heat energy absorbed by the surroundings when there is a change in the chemical system being investigated
- temperature (T) at which heat is transferred to the surroundings from the chemical system being investigated
We can write an equation to represent this entropy change in the surroundings at constant temperature as shown below:
ΔSsurroundings = |
heat absorbed by surroundings T |
At constant pressure, the amount of heat absorbed by the surroundings equals -q where q equals the amount of heat absorbed by the chemical system.
qsystem = heat absorbed by chemical system
-qsystem = heat absorbed by surroundings (that is, heat is transferred from surroundings to be absorbed by the chemical system)
Therefore, we can write:
ΔSsurroundings = |
heat absorbed by surroundings T |
ΔSsurroundings = |
-qsystem T |
Note that if the chemical system:
- gains heat (absorbs heat), q is a positive number, so -q is a negative number
- loses heat (releases heat), q is a negative number, so -q is a positive number
At constant pressure, q equals the enthalpy change for the system:
qsystem = ΔHsystem
At constant pressure, the amount of heat absorbed by the surroundings = -qsystem
So, the amount of heat absorbed by the surroundings = -ΔHsystem
At constant temperature AND pressure, we can write the following equation to represent the change in entropy for the surroundings:
ΔSsurroundings = |
-ΔHsystem T |
Note that if the chemical process is:
- exothermic, ΔHsystem is negative, -ΔHsystem is positive, and ΔSsurroundings is positive, entropy of the surroundings increase
- endothermic, ΔHsystem is positive, -ΔHsystem is negative, and ΔSsurroundings is negative, entropy of the surroundings decrease
Now we can substitute our expression for ΔSsurroundings into our original equation for determining the change in total entropy:
change in total entropy |
= |
change in entropy for the chemical system |
+ |
change in entropy of the surroundings
|
ΔStotal |
= |
ΔSchemical system |
+ |
ΔSsurroundings
|
ΔStotal |
= |
ΔSchemical system |
+ |
-ΔHchemical system T
|
ΔStotal |
= |
ΔSchemical system |
- |
ΔHchemical system T
|
Multiply throughout by -T
-T × ΔStotal |
= |
-T × ΔSchemical system |
- |
-T × ΔHchemical system T
|
-TΔStotal |
= |
-TΔSchemical system |
- |
-ΔHchemical system
|
-TΔStotal |
= |
-TΔSchemical system |
+ |
ΔHchemical system
|
Which can be rearranged in give:
-TΔStotal = ΔHchemical system - TΔSchemical system
We define the Gibbs free energy of a chemical system, or free energy of a chemical system, Gsystem, as:
Gsystem = Hsystem - TSsystem
where:
Hsystem = enthalpy of the chemical system
Tsystem = temperature of the chemical system
Ssystem = entropy of the chemical system
Gsystem, Hsystem, and Ssystem depend only on the state of a system.
If there is a change of state, say from state 1 to state 2, then:
Gstate 2 - Gstate 1 = Hstate 2 -Hstate 1 - (Tstate 2Sstate 2 - Tstate 1Sstate 1)
That is:
ΔGsystem = ΔHsystem - (Tstate 2Sstate 2 - Tstate 1Sstate 1)
At constant temperature, Tsystem = Tstate 2 = Tstate 1
So we can write the equation for the change in Gibbs free energy of the system (Gsystem) as:
ΔGsystem = ΔHsystem - (TsystemSstate 2 - TsystemSstate 1)
ΔGsystem = ΔHsystem - Tsystem(Sstate 2 - Sstate 1)
ΔGsystem = ΔHsystem - TsystemΔSsystem
Compare this with our equation for determining the total entropy change (ΔStotal) for a chemical process occurring at constant temperature and pressure:
-TΔStotal = ΔHchemical system - -TΔSchemical system
The change in Gibbs free energy for the system (ΔGsystem) can be equated with the total entropy change multiplied by -temperature:
ΔGsystem = -TΔStotal
Using Gibbs Free Energy (G) to Determine if a Chemical Reaction is Spontaneous or Nonspontaneous
According to the Second Law of Thermodynamics, the entropy of the universe increases, that is, the total entropy (ΔStotal) increases.
For a spontaneous change going from state 1 to state 2 the entropy of state 2 (Sstate 2) must be greater than the entropy of state 1 (Sstate 1)
Sstate 2 > Sstate 1
So the change in total entropy (ΔStotal) going from state 1 to state 2 spontaneously must be positive:
ΔStotal = Sstate 2 - Sstate 1
ΔStotal > 0
For a chemical process occurring at constant temperature and pressure, this means that the change in the Gibbs free energy of the system (ΔGsystem) must be negative for a spontaneous reaction:
ΔGsystem = -TΔStotal
ΔStotal is positive for a spontaneous reaction
ΔGsystem = negative
ΔGsystem < 0
A process in which the total entropy decreases (ΔStotal < 0) would be nonspontaneous.
At constant temperature and pressure, the change in Gibbs free energy for this nonspontaneous process would be positive:
ΔGsystem = -TΔStotal
ΔStotal is negative for a nonspontaneous reaction
ΔGsystem = positive
ΔGsystem > 0
For a system at equilibrium there is no change in total entropy (ΔStotal = 0)
At constant temperature and pressure, the change in Gibbs free energy for this process at equilibrium would be 0:
ΔGsystem = -TΔStotal
ΔStotal = 0 for a system at equilibrium
ΔGsystem = -T × 0
ΔGsystem = 0
The table below summarises the values for the change in Gibbs free energy for spontaneous reactions, nonspontaneous reactions and systems at equilibrium at constant temperature and pressure:
ΔG (constant T, P) |
Change |
ΔG < 0 (ΔG negative) |
spontaneous |
ΔG = 0 |
equilibrium (no net change) |
ΔG > 0 (ΔG positive) |
nonspontaneous |