Introduction to Entropy : Introduction to Entropy by Mike Roller
Slide 2 : Entropy (S) = a measure of randomness or disorder
Slide 3 : Entropy: Time’s Arrow
Slide 4 :
Second Law of Thermodynamics : In any spontaneous process, the entropy of the universe increases.
?Suniverse > 0
Another version of the 2nd Law:
Energy spontaneously spreads out if it has no outside resistance
Entropy measures the spontaneous dispersal of energy as a function of temperature
How much energy is spread out
How widely spread out it becomes
Entropy change = “energy dispersed”/T Second Law of Thermodynamics occurs without outside intervention
?
Entropy of the Universe : Entropy of the Universe ?Suniverse = ?Ssystem + ?Ssurroundings Positional disorder Energetic disorder ?Suniverse > 0 ? spontaneous process
Both ?Ssys and ?Ssurr positive
Both ?Ssys and ?Ssurr negative
?Ssys negative, ?Ssurr positive
?Ssys positive, ?Ssurr negative spontaneous process. nonspontaneous process. depends depends
Entropy of the Surroundings(Energetic Disorder) : Entropy of the Surroundings(Energetic Disorder) System Heat Entropy Surroundings System Heat Entropy Surroundings Low T ? large entropy change (surroundings)
High T ? small entropy change (surroundings) ?Hsys < 0 ?Hsys > 0 ?Ssurr > 0 ?Ssurr < 0
Positional Disorder and Probability : Positional Disorder and Probability Probability of 1 particle in left bulb = ½
" 2 particles both in left bulb = (½)(½) = ¼
" 3 particles all in left bulb = (½)(½)(½) = 1/8
" 4 " all " = (½)(½)(½)(½) = 1/16
" 10 " all " = (½)10 = 1/1024
" 20 " all " = (½)20 = 1/1048576
" a mole of " all " = (½)6.02?1023
The arrangement with the greatest entropy is the one with the highest probability (most “spread out”).
Entropy of the System: Positional Disorder : Ssolid < Sliquid << Sgas Entropy of the System: Positional Disorder Ludwig Boltzmann Ordered
states Disordered
states Low probability
(few ways) High probability
(many ways) Low S High S Ssystem ? Positional disorder
S increases with increasing # of possible positions Ludwig Boltzmann
The Third Law of Thermodynamics : The Third Law:
The entropy of a perfect crystal at 0 K is zero.
Everything in its place
No molecular motion The Third Law of Thermodynamics
Entropy Curve : Entropy Curve Solid Gas Liquid S
(qrev/T)
(J/K) Temperature (K) 0 0 ? fusion ? vaporization S° (absolute entropy) can be calculated for any substance
Entropy Increases with... : Entropy Increases with... Melting (fusion) Sliquid > Ssolid
?Hfusion/Tfusion = ?Sfusion
Vaporization Sgas > Sliquid
?Hvaporization/Tvaporization = ?Svaporization
Increasing ngas in a reaction
Heating ST2 > ST1 if T2 > T1
Dissolving (usually) Ssolution > (Ssolvent + Ssolute)
Molecular complexity more bonds, more entropy
Atomic complexity more e-, protons, neutrons
Recap: Characteristics of Entropy : Recap: Characteristics of Entropy S is a state function
S is extensive (more stuff, more entropy)
At 0 K, S = 0 (we can know absolute entropy)
S > 0 for elements and compounds in their standard states
?S°rxn = ?nS°products - ?nS°reactants
Raise T ? increase S
Increase ngas ? increase S
More complex systems ? larger S
Entropy and Gibbs Free Energy : Entropy and Gibbs Free Energy by Mike Roller
Entropy (S) Review : Entropy (S) Review ?Suniverse > 0 for spontaneous processes
?Suniverse = ?Ssystem + ?Ssurroundings ?
positional ?
energetic We can know the absolute entropy value for a substance
S° values for elements & compounds in their standard states are tabulated (Appendix C, p. 1019)
For any chemical reaction, we can calculate ?S°rxn:
?S°rxn = ?S°(products) - ?S°(reactants)
?Suniverse and Chemical Reactions : ?Suniverse and Chemical Reactions ?Suniverse = ?Ssystem + ?Ssurroundings
For a system of reactants and products,
?Suniverse = ?Srxn – ?Hrxn/T
If ?Suniverse > 0, the reaction is spontaneous
If ?Suniverse < 0, the reaction is not spontaneous
The reverse reaction is spontaneous
If ?Suniverse = 0, the reaction is at equilibrium
Neither the forward nor the reverse reaction is favored
C6H12O6(s) + 6 O2(g) ? 6 CO2(g) + 6 H2O(g) : C6H12O6(s) + 6 O2(g) ? 6 CO2(g) + 6 H2O(g) Compound
C6H12O6(s)
O2(g)
CO2(g)
H2O(g) ?H°f (kJ/mol)
-1275
0
-393.5
-242 S° (J/mol K)
212
205
214
189 ?Suniverse = ?Srxn – ?Hrxn/T ?S°rxn = ?S°(products) - ?S°(reactants)
= [6 S°(CO2(g)) + 6 S°(H2O(g))] – [S°(C6H12O6(s)) + 6 S°(O2(g))]
= [6(214) + 6(189)] – [(212) + 6(205)] J/K
?S°rxn = 976 J/K
?H°rxn = ??H°f (products) - ??H°f(reactants)
= [6 ?H°f(CO2(g)) + 6 ?H°f(H2O(g))] – [?H°f(C6H12O6(s)) + 6 ?H°f(O2(g))]
= [6(-393.5) + 6(-242)] – [(-1275) + 6(0)] kJ
?H°rxn = -2538 kJ
C6H12O6(s) + 6 O2(g) ? 6 CO2(g) + 6 H2O(g) : C6H12O6(s) + 6 O2(g) ? 6 CO2(g) + 6 H2O(g) Compound
C6H12O6(s)
O2(g)
CO2(g)
H2O(g) ?H°f (kJ/mol)
-1275
0
-393.5
-242 S° (J/mol K)
212
205
214
189 ?Suniverse = ?Srxn – ?Hrxn/T ?S°rxn = 976 J/K (per mole of glucose)
?H°rxn = -2538 kJ (per mole of glucose)
At 298 K,
?S°universe = 0.976 kJ/K – (-2538 kJ/298 K)
?S°universe = 9.5 kJ/K
Gibbs Free Energy (G) : –?G means +?Suniv
A process (at constant T, P) is spontaneous if free energy decreases Gibbs Free Energy (G) Josiah Gibbs G = H – TS
At constant temperature,
?G = ?H – T?S
(system’s point of view) ?G = ?H – T?S
Divide both sides by –T
-?G/T = -?H/T + ?S
?G and Chemical Reactions : ?G and Chemical Reactions ?G = ?H – T?S
If ?G < 0, the reaction is spontaneous
If ?G > 0, the reaction is not spontaneous
The reverse reaction is spontaneous
If ?G = 0, the reaction is at equilibrium
Neither the forward nor the reverse reaction is favored
?G is an extensive state function
Ba(OH)2(s) + 2NH4Cl(s) ? BaCl2(s) + 2NH3(g) + 2 H2O(l) : Ba(OH)2(s) + 2NH4Cl(s) ? BaCl2(s) + 2NH3(g) + 2 H2O(l) ?H°rxn = 50.0 kJ (per mole Ba(OH)2)
?S°rxn = 328 J/K (per mole Ba(OH)2) ?G = ?H - T?S ?G° = 50.0 kJ – 298 K(0.328 kJ/K)
?G° = – 47.7 kJ Spontaneous At what T does the reaction stop being spontaneous?
The T where ?G = 0.
?G = 0 = 50.0 kJ – T(0.328 J/K)
50.0 kJ = T(0.328 J/K)
T = 152 K ?not spontaneous below 152 K
Effect of ?H and ?S on Spontaneity : Effect of ?H and ?S on Spontaneity ?H
–
+
–
+ ?S
+
+
–
– Spontaneous?
Spontaneous at all temps
Spontaneous at high temps
Reverse reaction spontaneous at low temps
Spontaneous at low temps
Reverse reaction spontaneous at high temps
Not spontaneous at any temp ?G = ?H – T?S
?G negative ? spontaneous reaction
Ways to Calculate ?G°rxn : 1. ?G° = ??G°f(products) - ??G°f(reactants)
?G°f = free energy change when forming 1 mole of compound from elements in their standard states
2. ?G° = ?H° - T?S°
3. ?G° can be calculated by combining ?G° values for several reactions
Just like with ?H° and Hess’s Law Ways to Calculate ?G°rxn
2H2(g) + O2(g) ? 2 H2O(g) : 2H2(g) + O2(g) ? 2 H2O(g) 1. ?G° = ??G°f(products) - ??G°f(reactants)
?G°f(O2(g)) = 0
?G°f(H2(g)) = 0
?G°f(H2O(g)) = -229 kJ/mol
?G° = (2(-229 kJ) – 2(0) – 0) kJ = -458 kJ
2. ?G° = ?H° - T?S°
?H° = -484 kJ
?S° = -89 J/K
?G° = -484 kJ – 298 K(-0.089 kJ/K) = -457 kJ
2H2(g) + O2(g) ? 2 H2O(g) : 2H2(g) + O2(g) ? 2 H2O(g) 3. ?G° = combination of ?G° from other reactions (like Hess’s Law)
2H2O(l) ? 2H2(g) + O2(g) ?G°1 = 475 kJ
H2O(l) ? H2O(g) ?G°2 = 8 kJ
?G° = - ?G°1 + 2(?G°2)
?G° = -475 kJ + 16 kJ = -459 kJ Method 1: -458 kJ
Method 2: -457 kJ
Method 3: -459 kJ
What is Free Energy, Really? : What is Free Energy, Really? NOT just “another form of energy”
Free Energy is the energy available to do useful work
If ?G is negative, the system can do work (wmax = ?G)
If ?G is positive, then ?G is the work required to make the process happen
Example: Photosynthesis
6 CO2 + 6 H2O ? C6H12O6 + 6 O2
?G = 2870 kJ/mol of glucose at 25°C
2870 kJ of work is required to photosynthesize 1 mole of glucose