IB Chemistry on Entropy and Laws of Thermodynamics

29
E = sum kinetic energy/motion of molecule, and potential energy represented by chemical bond bet atom E = q + w E = Change internal energy q = heat transfer w = work done by/on system Thermodynamics Study of work, heat and energy on a system E universe = E sys + E surrounding = 0 1 st Law Thermodynamics Entropy - Measure of disorder ∆S uni = ∆S sys + ∆S surr > 0 (irreversible rxn) All spontaneous rxn produce increase in entropy of universe 2 nd Law Thermodynamics S uni = S sys + S surr Isolated system - Entropy change of universe always increase Click here thermodynamics entropy Entropy Measure molecular disorder/randomness More disorder - More dispersion of matter/energy More random - Rxn toward right- Entropy Increases Direction to right- Spontaneous to right 2 nd Law Thermodynamics Embrace the chaos Over time - Entropy increase Direction to left Never happen ! Click here thermodynamics Energy cannot be created or destroyed > 0

Transcript of IB Chemistry on Entropy and Laws of Thermodynamics

Page 1: IB Chemistry on Entropy and Laws of Thermodynamics

E = sum kinetic energy/motion of molecule, and potential energy represented by chemical bond bet atom

∆E = q + w

∆E = Change internal energy

q = heat transfer

w = work done by/on system

Thermodynamics Study of work, heat and energy on a system

∆E universe = ∆E sys + ∆E surrounding = 0

1st Law Thermodynamics

Entropy - Measure of disorder ↓

∆S uni = ∆S sys + ∆S surr > 0 (irreversible rxn) ↓

All spontaneous rxn produce increase in entropy of universe

2nd Law Thermodynamics

∆S uni = ∆S sys + ∆S surr

Isolated system - Entropy change of universe always increase

Click here thermodynamics entropy Entropy

Measure molecular disorder/randomness ↓

More disorder - More dispersion of matter/energy ↓

More random - Rxn toward right- Entropy Increases ↑

Direction to right- Spontaneous to right →

2nd Law Thermodynamics

Embrace the chaos

Over time - Entropy increase ↑

Direction to left ← Never happen !

Click here thermodynamics

Energy cannot be created or destroyed

> 0

Page 2: IB Chemistry on Entropy and Laws of Thermodynamics

∆S = Entropy change

Entropy

Dispersal/Distribution Matter Energy

Matter more disperse ↑

Entropy increases ↑

solid liquid gas

spontaneous - entropy ↑

Over time - Entropy increase ↑

Phase change - sol → liq → gas ↓

Entropy increase ↑

Every energy transfer - increase entropy universe Entropy universe can only go up - never go down Entropy increase - many ways energy spread out

Dispersion energy as heat - increase entropy

Stoichiometry- more gas/liq in product ↓

Entropy increase ↑

T

QS

Heat added ↑ Phase change Stoichiometry

Embrace the chaos

N2O4(g) → 2NO2(g)

1 2

2H2O(l) → 2H2 (g) + O2 (g)

1 2 3

3

More gas in product - Entropy ↑

Heat added ↑

Entropy

Measure molecular disorder/randomness ↓

More disorder - More dispersion of matter/energy ↓

More randon - Rxn towards right- Entropy Increases ↑

Liq more disorder than solid Gas more disorder than liq

kinetic energy distributed

over wide range

Q = heat transfer

T = Temp/K

Distribution matter in space Distribution energy bet particles

Direction to left ← Never happen ! Direction to right- Spontaneous to right →

Page 3: IB Chemistry on Entropy and Laws of Thermodynamics

Statistical Entropy

Entropy

Measure molecular disorder/randomness ↓

More disorder - More dispersion of matter/energy ↓

More random - Entropy Increases ↑

1st Law Thermodynamics - Doesn't help explain direction of rxn ∆S uni > 0 (+ve) → More disorder - spontaneous ∆S uni < 0 (-ve) → More order - non spontaneous

Change sol → liq → gas - Higher entropy Greater number particles in product - Higher entropy

More complex molecule - More atoms bonded - Higher entropy Higher temp - Vibrate faster - More random - Higher entropy

Why gas mixes and not unmix? Why heat flow from hot to cold?

Entropy

Notes on Entropy

1st Law Thermodynamics 2nd Law Thermodynamics

Energy cannot be created or destroyed Transfer from one form to another

∆E universe = ∆E sys + ∆E surrounding = 0

Isolated system ↓

∆S uni always increase

∆E = q + w

Method to calculate entropy

Number microstates

Thermodynamic Entropy

Heat + Temp involved

Gas mixes Solution diffuse Heat flow hot →cold

X X X

∆E = internal energy

q = heat transfer

w = work done ∆S = Entropy universe

∆S = Entropy system

∆S = Entropy surrounding

∆S uni = ∆S sys + ∆S surr

Law Thermodynamics

1 2

∆S = Entropy uni

WkS ln

∆S = Entropy change

k = boltzmann constant

W = Microstate

Click here statistical entropy Click here thermodynamics entropy

Why solution diffuse and not undiffuse?

Unit - J mol -1 K-1

surrsysuni SSS

∆S = Entropy sys and surr

Page 4: IB Chemistry on Entropy and Laws of Thermodynamics

1st Law Thermodynamics - Doesn't help explain direction of rxn ∆S uni > 0 (+ve) → More disorder - spontaneous ∆S uni < 0 (-ve) → More order - non spontaneous

Change sol → liq → gas - Higher entropy Greater number particles in product - Higher entropy

More complex molecule - More atoms bonded - Higher entropy Higher temp - Vibrate faster - More random - Higher entropy

Measure molecular disorder/randomness ↓

More disorder - More dispersion of matter/energy ↓

More random - Entropy Increases ↑

Isolated system ↓

∆S uni always increase

Entropy

Why gas mixes and not unmix? Why heat flow from hot to cold?

Notes on Entropy

1st Law Thermodynamics 2nd Law Thermodynamics

Energy cannot be created or destroyed Transfer from one form to another

∆E universe = ∆E sys + ∆E surrounding = 0

∆E = q + w

Gas mixes Solution diffuse Heat flow hot →cold

X X X

∆E = internal energy

q = heat transfer

w = work done ∆S = Entropy universe

∆S = Entropy system

∆S = Entropy surrounding

∆S uni = ∆S sys + ∆S surr

Law Thermodynamics

3rd Law Thermodynamics

Unit - J mol -1 K-1

Standard Molar Entropy, S0

Entropy perfectly crystal at 0K = 0 Std molar entropy, S0

↓ S0 when substance heated from 0K to 298K

Std state - 1 atm / 1M sol

Temp = 298K

Std Molar Entropy/S0 S0 at 298 /JK-1 mol-1

Fe (s) + 27

H2O (s) + 48

Na (s) + 52

H2O (l) + 69

CH3OH (l) + 127

H2 (g) + 130

H2O (g) + 188

CO2 (g) + 218

Solid - Order

Entropy Lowest

Liq - Less order

Entropy Higher

Gas - Disorder

Entropy Highest

Entropy highest

Why solution diffuse and not undiffuse?

Page 5: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mix and not unmix? Why solution diffuse and not undiffuse? Why heat flow from hot to cold?

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Unit - J mol -1 K-1

Standard Molar Entropy, S0

Entropy perfectly crystal at 0K = 0 ↓

S0 when substance heated from 0K to 298K

Std state - 1 atm / 1M sol

Temp = 298K

Std Molar Entropy/S0 S0 at 298 /JK-1 mol-1

Fe (s) + 27

H2O (s) + 48

Na (s) + 52

H2O (l) + 69

CH3OH (l) + 127

H2 (g) + 130

H2O (g) + 188

CO2 (g) + 218

Solid - Order

Entropy Lowest

Liq - Less order

Entropy Higher

Gas - Disorder

Entropy Highest

Entropy

highest

Entropy

Standard Molar Entropy, S0

Depend on

Temp increase ↑ - Entropy increase ↑

Physical/phase state

Dissolving solid Molecular mass

Click here thermodynamics entropy Ba(OH)2

Temp

Temp/K 273 295 298

S0 for H2 + 31 + 32 + 33.2

Sol → Liq → Gas - Entropy increase ↑

State solid liquid gas

S0 for H2O + 48 + 69 + 188

entropy increase ↑ entropy increase ↑

Depend on

Substance NaCI NH4NO3

S0 for solid + 72 + 151

S0 for aq + 115 + 260

More motion - entropy increase ↑ Higher mass - entropy increase ↑

Substance HF HCI HBr

Molar mass 20 36 81

S0 + 173 + 186 + 198

S0 = 0 at 0K All sub > 0K, have +ve S0

Page 6: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy perfectly crystal at 0K = 0 ↓

S0 when substance heated from 0K to 298K

Entropy

Why gas mix and not unmix? Why solution diffuse and not undiffuse? Why heat flow from hot to cold?

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Unit - J mol -1 K-1

Standard Molar Entropy, S0

Std state - 1 atm / 1M sol

Temp = 298K

Std Molar Entropy/S0 S0 at 298 /JK-1 mol-1

H2O (s) + 48

Na (s) + 52

H2O (l) + 69

CH3OH (l) + 127

H2O (g) + 188

CO2 (g) + 218

Solid - Order

Entropy Lowest

Liq - Less order

Entropy Higher

Gas - Disorder

Entropy Highest

Entropy

highest

Entropy

Standard Molar Entropy, S0

Depend on

Temp increase ↑ - Entropy increase ↑

Physical/phase state

Dissolving solid Molecular mass

Temp

Temp/K 273 295 298

S0 for H2 + 31 + 32 + 33.2

Sol → Liq → Gas - Entropy increase ↑

State solid liquid gas

S0 for H2O + 48 + 69 + 188

entropy increase ↑ entropy increase ↑

Depend on

More motion - entropy increase ↑

Click here entropy notes

Click here entropy, enthalpy free energy data

Click here entropy CRC data booklet

Higher mass - entropy increase ↑

S0 = 0 at 0K All sub > 0K, have +ve S0

Substance NaCI NH4NO3

S0 for solid + 72 + 151

S0 for aq + 115 + 260

Substance HF HCI HBr

Molar mass 20 36 81

S0 + 173 + 186 + 198

Page 7: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order - Less number gas ↓

Entropy surr ↑ increase - Heat release increase ↑ motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr > ∆S sys (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Combustion at 298K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

C3H8(g) + 5O2 (g) → 3CO2(g) + 4H2O(l) ∆H = -2220 kJ at 298K

C3H8(g) + 5 O2 (g) → 3 CO2(g) + 4 H2O(l) S0 +270 +205 x 5 +213 x 3 +70 x 4

1295 919 Reactant Product

17450

298

)2220000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

376

1295919

JKS

S

SSS

sys

sys

treacproductsys

170747450376

JKS

SSS

uni

surrsysuni

∆H = -2220 kJ = -2220000J

surrsysuni SSS

S /JK-1

Assume Q = H at constant pressure

+ve

-ve

spontaneous ∆Ssys = - 376

∆Ssurr = +7450

= +

∆Suni = + 7074

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is Combustion at 298K spontaneous?

Page 8: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order - Less number gas ↓

Entropy surr ↑ increase - Heat released increase ↑ motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr > ∆S sys (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Combustion at 298K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

CH4(g) + 2O2 (g) → CO2(g) + 2H2O(g) ∆H = - 890 kJ at 298K

CH4(g) + 2 O2 (g) → CO2(g) + 2 H2O(g) S0 + 186 +205 x 2 +213 + 188 x 2

+ 596 + 589 Reactant Product

12986

298

)890000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

7

596589

JKS

S

SSS

sys

sys

treacproductsys

1297929867

JKS

SSS

uni

surrsysuni

∆H = - 890 kJ = - 890 000J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous ∆Ssys = - 7

∆Ssurr = + 2986

= +

∆Suni = + 2979

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Assume Q = H at constant pressure

Is Combustion at 298K spontaneous?

Page 9: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order - Liquid form ↓

Entropy surr ↑ increase - Heat released increase ↑ motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr > ∆S sys (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Condensation at 298K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

H2O (g) → H2O(l) ∆H = - 44.1 kJ at 298K

H2O (g) → H2O(l) S0 + 188 + 70

+ 188 + 70 Reactant Product

1148

298

)44100(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

118

18870

JKS

S

SSS

sys

sys

treacproductsys

130148118

JKS

SSS

uni

surrsysuni

∆H = -44.1 kJ = - 44 100J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous

∆Ssys = - 118

∆Ssurr = + 148

= +

∆Suni = + 30

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Condensation steam at 298K (25C) spontaneous?

Assume Q = H at constant pressure

Page 10: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↑ increase - More disorder - More gas atoms form ↓

Entropy surr ↓ decrease - Heat absorb decrease ↓ motion surr particles ↓

Heat absorb by sys from surr decrease ↓ entropy surr ↓

∆S surr < ∆S sys (More -ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni < 0 - Atomization at 298K - Non Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

H2(g) → 2 H(g) ∆H = + 436 kJ at 298K

H2 (g) → 2 H(g) S0 + 130 + 115 x 2

+ 130 + 230 Reactant Product

11463

298

)436000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

100

130230

JKS

S

SSS

sys

sys

treacproductsys

113631463100

JKS

SSS

uni

surrsysuni

∆H = + 436 kJ = + 436 000J

surrsysuni SSS

S /JK-1

+ve

-ve

non - spontaneous

∆Ssys = +100

∆Ssurr = - 1463

= +

∆Suni = - 1363

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is Atomization of H2 at 298K spontaneous?

Assume Q = H at constant pressure

Page 11: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order - Solid form ↓

Entropy surr ↑ increase - Heat released increase ↑ motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S sys > ∆S surr (More -ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni < 0 - Freezing at 298K - Non Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

H2O (l) → H2O(s) ∆H = - 6 kJ at 298K

H2O (l) → H2O(s) S0 + 70 + 48

+ 70 + 48 Reactant Product

120

298

)6000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

22

7048

JKS

S

SSS

sys

sys

treacproductsys

122022

JKS

SSS

uni

surrsysuni

∆H = -6 kJ = - 6000J

surrsysuni SSS

S /JK-1

+ve

-ve

non - spontaneous

∆Ssys = - 22

∆Ssurr = + 20

= + ∆Suni= - 2

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is Freezing water to ice at 298K (25C) spontaneous?

Assume Q = H at constant pressure

Page 12: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order - Solid form ↓

Entropy surr ↑ increase - Heat released increase ↑ motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr > ∆S sys (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Freezing at 263K (-10C) - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

H2O (l) → H2O(s) ∆H = - 6 kJ at 263K

H2O (l) → H2O(s) S0 + 70 + 48

+ 70 + 48 Reactant Product

18.22

263

)6000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

22

7048

JKS

S

SSS

sys

sys

treacproductsys

18.08.2222

JKS

SSS

uni

surrsysuni

∆H = -6 kJ = - 6000J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous

∆Ssys = - 22

∆Ssurr = + 22.8

= + ∆Suni= + 0.8

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is Freezing water to ice at 263K (-10C) spontaneous?

Assume Q = H at constant pressure

Page 13: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↑ increase - More disorder - Gas form ↓

Entropy surr ↓ decrease - Heat absorb decrease ↓ motion surr particles ↓

Heat absorb by sys from surr decrease ↓ entropy surr ↓

∆S surr < ∆S sys (More -ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni < 0 - Decomposition at 298K - Non Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

CaCO3 (s) → CaO(s) + CO2(g) ∆H = + 178 kJ at 298K

CaCO3 (s) → CaO (s) + CO2(g) S0 + 93 + 40 + 213

+ 93 + 253 Reactant Product

1597

298

)178000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

160

93253

JKS

S

SSS

sys

sys

treacproductsys

1437597160

JKS

SSS

uni

surrsysuni

∆H = + 178 kJ =+ 178 000J

surrsysuni SSS

S /JK-1

+ve

-ve

non - spontaneous

∆Ssys = + 160

∆Ssurr = - 597

= +

∆Suni= - 437

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Decomposition CaCO3 at 298K (25C) spontaneous?

Assume Q = H at constant pressure

Page 14: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↑ increase - More disorder - Gas form ↓

Entropy surr ↓ decrease - Heat aborb decrease ↓ motion surr particles ↓

Heat absorb by sys from surr decrease ↓ entropy surr ↓

∆S sys > ∆S surr (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Decomposition at 1500K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

CaCO3 (s) → CaO(s) + CO2(g) ∆H = + 178 kJ at 1500K

CaCO3 (s) → CaO (s) + CO2(g) S0 + 93 + 40 + 213

+ 93 + 253 Reactant Product

1118

1500

)178000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

160

93253

JKS

S

SSS

sys

sys

treacproductsys

142118160

JKS

SSS

uni

surrsysuni

∆H = + 178 kJ =+ 178 000J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous

∆Ssys = + 160

∆Ssurr = - 118

= + ∆Suni = + 42

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Decomposition CaCO3 at 1500K (1227C) spontaneous?

Assume Q = H at constant pressure

Page 15: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order - Less gas form ↓

Entropy surr ↑ increase - Heat release increase ↑ motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr > ∆S sys (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Oxidation at 298K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

2NO(g) + O2(g) → 2NO2(g) ∆H = - 114 kJ at 298K

2 NO(g) + O2 (g) → 2NO2(g) S0 + 210 x 2 + 102 + 240 x 2

+ 522 + 480 Reactant Product

1382

298

)114000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

42

522480

JKS

S

SSS

sys

sys

treacproductsys

133938242

JKS

SSS

uni

surrsysuni

∆H = - 114 kJ = - 114 000J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous

∆Ssys = - 42

∆Ssurr = + 382

= +

∆Suni = + 339

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is Oxidation of NO at 298K (25C) spontaneous?

Assume Q = H at constant pressure

Page 16: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order - Less gas form ↓

Entropy surr ↑ increase - Heat release increase ↑ motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr > ∆S sys (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - NH3 production at 298K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

N2(g) + 3H2(g) → 2NH3(g) ∆H = - 92 kJ at 298K

N2(g) + 3H2 (g) → 2NH3(g) S0 + 192 + 131 x 3 + 192 x 2

+ 585 + 384 Reactant Product

1308

298

)92000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

201

585384

JKS

S

SSS

sys

sys

treacproductsys

1107308201

JKS

SSS

uni

surrsysuni

∆H = - 92 kJ = - 92 000J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous

∆Ssys = - 201

∆Ssurr = + 308

= +

∆Suni = + 107

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is Haber, NH3 production 298K (25C) spontaneous?

Assume Q = H at constant pressure

NH3

Page 17: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order ↓

Entropy surr ↑ increase - Heat release increase ↑ motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr > ∆S sys (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - AI production at 298K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

Fe2O3(s) + 2AI(s) → 2Fe(s) + AI2O3(s) ∆H = - 851 kJ at 298K

+ 143 + 105 Reactant Product

12855

298

)851000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

38

143105

JKS

S

SSS

sys

sys

treacproductsys

12817285538

JKS

SSS

uni

surrsysuni

∆H = - 851 kJ = - 851 000J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous

∆Ssys = - 38

∆Ssurr = + 2855

= +

∆Suni = + 2817

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is Thermite, AI production 298K (25C) spontaneous?

Assume Q = H at constant pressure

Fe2O3(s) + 2AI(s) → 2Fe(s) + AI2O3(s) S0 + 87 + 28 x 2 + 27 x 2 + 51

Page 18: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↓ decrease - More order ↓

Entropy surr ↑ increase - Heat release increase motion surr particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr > ∆S sys (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Decomposition KCIO3 at 298K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

4KCIO3(s) → 3KCIO4(s) + KCI(s) ∆H = - 144 kJ at 298K

+ 572 + 535 Reactant Product

1483

298

)144000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

37

572535

JKS

S

SSS

sys

sys

treacproductsys

144648337

JKS

SSS

uni

surrsysuni

∆H = - 144 kJ = - 144 000J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous

∆Ssys = - 37

∆Ssurr = + 483

= +

∆Suni = + 446

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is decomposition KCIO3

298K (25C) spontaneous?

Assume Q = H at constant pressure

∆S/∆H constant over range of temp

4KCIO3(s) → 3KCIO4(s) + KCI(s) S0 + 143 x 4 + 151 x 3 + 82

Page 19: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Entropy

Thermodynamic Entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

1 Quatitatively

T

H

T

QSsurr

Quatitatively

Entropy sys ↑ increase - More disorder ↓

Entropy surr ↑ increase - Heat release increase ↑ motion particles ↓

Heat release by sys to surr increase ↑ entropy surr ↓

∆S surr + ∆S sys > 0 (More +ve) ↓

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 Combustion sugar at 298K - Spontaneous

surrsysuni SSS

)tan()( treacprosys SSS

C6H12O6(s) + 6O2 (g) → 6CO2(g) + 6H2O(l) ∆H = - 2810 kJ at 298K

+ 821 + 1698 Reactant Product

19430

298

)2810000(

JKS

S

T

HS

surr

surr

surr

1

)tan()(

877

8211698

JKS

S

SSS

sys

sys

treacproductsys

1103079430877

JKS

SSS

uni

surrsysuni

∆H = - 2810 kJ = - 2810 000J

surrsysuni SSS

S /JK-1

+ve

-ve

spontaneous

∆Ssys = + 877

∆Ssurr = + 9430

= +

∆Suni = + 10307

∆S uni > 0 (+ve) → Spontaneous ∆S uni < 0 (-ve) → Non spontaneous

Is combustion sugar

298K (25C) spontaneous?

Assume Q = H at constant pressure

∆S/∆H constant over range of temp

C6H12O6 (s) + 6O2(g) → 6CO2(g) + 6H2O(l) S0 + 209 +102 x 6 + 213 x 6 + 70 x 6

Page 20: IB Chemistry on Entropy and Laws of Thermodynamics

∆S uni = ∆S sys + ∆S surr

↓ ∆S uni > 0

∆S uni = ∆S sys + ∆S surr

↓ ∆S uni > 0

q = heat transfer

Isolated system ∆S uni always increase

1st Law Thermodynamics 2nd Law Thermodynamics

Energy cannot be created or destroyed Transfer from one form to another

∆E universe = ∆E sys + ∆E surrounding = 0

∆E = q + w

∆E = internal energy

w = work done ∆S = Entropy universe

∆S = Entropy system

∆S = Entropy surrounding

∆S uni = ∆S sys + ∆S surr

Law Thermodynamics

3rd Law Thermodynamics

Unit - J mol -1 K-1

Standard Molar Entropy, S0

Entropy perfectly crystal at 0K = 0 Std molar entropy, S0

S0 when substance heated from 0K to 298K

Std state - 1 atm / 1M sol

Temp = 298K

spontaneous

+ve

-ve

=

S /JK-1

Exothermic - Heat released

∆Ssys = + ve

∆Ssurr = + ve

∆Suni = + ve

+

∆S sys + ve , ∆S surr +ve ↓

Suni > 0 (Rxn always spontaneous)

Exothermic - Heat released

+ve

-ve ∆Ssys = - ve

+

∆Ssurr = + ve

∆Suni = + ve

= spontaneous

∆S sys - ve and ∆S surr + ve ↓

Suni > 0 (Rxn spontaneous)

Endothermic - Heat absorb

S /JK-1 S /JK-1

∆Ssys = + ve

+

∆Ssurr = - ve

=

∆Suni = + ve

∆S sys + ve and ∆S surr - ve ↓

Suni > 0 (Rxn spontaneous)

spontaneous

∆S uni = ∆S sys + ∆S surr

↓ ∆S uni > 0

C6H12O6(s) + 6O2 (g) → 6CO2(g) + 6H2O(l) ∆H = - 2810 kJ

Spontaneous / non spontaneous ∆Hsys and ∆Suni

2NO(g) + O2(g) → 2NO2(g) ∆H = - 114 kJ CaCO3 (s) → CaO(s) + CO2(g) ∆H = + 178 kJ

∆H = -ve ∆H = -ve ∆H = +ve

Page 21: IB Chemistry on Entropy and Laws of Thermodynamics

∆S uni = ∆S sys + ∆S surr

↓ ∆S uni< 0

∆S uni = ∆S sys + ∆S surr

↓ ∆S uni < 0

∆S uni = ∆S sys + ∆S surr

↓ ∆S uni < 0

q = heat transfer

Isolated system ∆S uni always increase

1st Law Thermodynamics 2nd Law Thermodynamics

Energy cannot be created or destroyed Transfer from one form to another

∆E universe = ∆E sys + ∆E surrounding = 0

∆E = q + w

∆E = internal energy

w = work done ∆S = Entropy universe

∆S = Entropy system

∆S = Entropy surrounding

∆S uni = ∆S sys + ∆S surr

Law Thermodynamics

3rd Law Thermodynamics

Unit - J mol -1 K-1

Standard Molar Entropy, S0

Entropy perfectly crystal at 0K = 0 Std molar entropy, S0

S0 when substance heated from 0K to 298K

Std state - 1 atm / 1M sol

Temp = 298K

Non spontaneous

+ve

-ve

=

S /JK-1

Endothermic - Heat absorb

∆Ssys = + ve

∆Ssurr = - ve

∆Suni = - ve

+

∆S sys + ve , ∆S surr - ve ↓

Suni < 0 (Rxn always Non spontaneous)

Exothermic - Heat released

+ve

-ve

∆Ssys = - ve

+

∆Ssurr = + ve

∆Suni = - ve

=

∆S sys - ve, ∆S surr + ve ↓

Suni < 0 (Rxn Non spontaneous)

Endothermic - Heat absorb

S /JK-1 S /JK-1

∆Ssys = + ve

+

∆Ssurr = - ve

=

∆Suni = - ve

∆S sys + ve and ∆S surr - ve ↓

Suni < 0 (Rxn Non spontaneous)

Spontaneous / non spontaneous ∆Hsys and ∆Suni

∆H = + ve ∆H = + ve ∆H = - ve

CaCO3 (s) → CaO(s) + CO2(g) ∆H = + 178 kJ H2O (l) → H2O(s) ∆H = - 6 kJ

Non spontaneous

H2(g) → 2 H(g) ∆H = + 436 kJ

Non spontaneous

Page 22: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Predict entropy change - quatitatively

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Reactant Product

CH4(g) + 2O2 (g) → CO2(g) + 2H2O(l)

CH4(g) + 2 O2 (g) → CO2(g) + 2 H2O(l) ∆Hf

0 - 74 0 - 393 - 286 x 2

S0 + 186 +205 x 2 + 213 + 70 x 2

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

1

)tan()(

243

596353

JKS

S

SSS

sys

sys

treacproductsys

12990

298

)891000(

JKS

S

T

HS

surr

surr

surr

kJHsys 891)74(965

surrsysuni SSS

127472990243

JKS

SSS

uni

surrsysuni

Is Combustion at 298K spontaneous?

Unit for ∆S - JK-1 Unit for ∆H - kJ

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Combustion at 298K - Spontaneous

C3H8(g) + 5O2 (g) → 3CO2(g) + 4H2O(l)

C3H8(g) + 5 O2 (g) → 3 CO2(g) + 4 H2O(l) ∆Hf

0 - 104 0 - 393 x 3 - 286 x 4 S0 +270 +205 x 5 +213 x 3 + 70 x 4

Reactant Product

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

1

)tan()(

376

1295919

JKS

S

SSS

sys

sys

treacproductsys kJHsys 2219)104(2323

17446

298

)2219000(

JKS

S

T

HS

surr

surr

surr

surrsysuni SSS

170707446376

JKS

SSS

uni

surrsysuni

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Combustion at 298K - Spontaneous

1 2

Page 23: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Predict entropy change - quatitatively

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Reactant Product

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

1

)tan()(

118

18870

JKS

S

SSS

sys

sys

treacproductsys

1148

298

)44000(

JKS

S

T

HS

surr

surr

surr

kJHsys 44)242(286

surrsysuni SSS

130148118

JKS

SSS

uni

surrsysuni

Is Condensation/Freezing at 298K spontaneous?

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Condensation at 298K - Spontaneous

Reactant Product

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

1

)tan()(

22

7048

JKS

S

SSS

sys

sys

treacproductsys kJHsys 6)286(292

120

298

)6000(

JKS

S

T

HS

surr

surr

surr

surrsysuni SSS

122022

JKS

SSS

uni

surrsysuni

∆S uni = ∆S sys + ∆S surr ↓

∆S uni < 0 -Freezing at 298K - Non Spontaneous

3 4 H2O (g) → H2O(l) H2O (l) → H2O(s)

H2O (g) → H2O(l) ∆Hf

0 - 242 - 286 S0 + 188 + 70

H2O (l) → H2O(s) ∆Hf

0 - 286 - 292 S0 + 70 + 48

Page 24: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Predict entropy change - quatitatively

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Reactant Product

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

1308

298

)92000(

JKS

S

T

HS

surr

surr

surr

kJHsys 92)0(92

surrsysuni SSS

1107308201

JKS

SSS

uni

surrsysuni

Are these rxn at 298K spontaneous?

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - NH3 production at 298K - Spontaneous

Reactant Product

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

kJHsys 168)1564(1732

1563

298

)168000(

JKS

S

T

HS

surr

surr

surr

surrsysuni SSS

152656337

JKS

SSS

uni

surrsysuni

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Decomposition at 298K - Spontaneous

5 6 N2(g) + 3H2(g) → 2NH3(g)

N2(g) + 3H2 (g) → 2NH3(g) ∆Hf

0 0 0 - 46 x 2 S0 + 192 + 131 x 3 + 192 x 2

1

)tan()(

201

585384

JKS

S

SSS

sys

sys

treacproductsys

4KCIO3(s) → 3KCIO4(s) + KCI(s)

4KCIO3(s) → 3KCIO4(s) + KCI(s) ∆Hf

0 - 391 x 4 - 432 x 3 - 436 S0 + 143 x 4 + 151 x 3 + 82

1

)tan()(

37

572535

JKS

S

SSS

sys

sys

treacproductsys

Page 25: IB Chemistry on Entropy and Laws of Thermodynamics

1118

1500

)178000(

JKS

S

T

HS

surr

surr

surr

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Predict entropy change - quatitatively

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Reactant Product

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

kJHsys 178)1206(1028

surrsysuni SSS

1437597160

JKS

SSS

uni

surrsysuni

∆S uni = ∆S sys + ∆S surr ↓

∆S uni < 0 - Decomposition at 298K - Non Spontaneous

Reactant Product

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

surrsysuni SSS

142118160

JKS

SSS

uni

surrsysuni

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 - Decomposition at 1500K - Spontaneous

7 8 CaCO3 (s) → CaO(s) + CO2(g)

CaCO3 (s) → CaO (s) + CO2(g) ∆Hf

0 - 1206 - 635 - 393 S0 + 93 + 40 + 213

1

)tan()(

160

93253

JKS

S

SSS

sys

sys

treacproductsys

Decomposition at 298K Decomposition at 1500K

CaCO3 (s) → CaO(s) + CO2(g)

CaCO3 (s) → CaO (s) + CO2(g) ∆Hf

0 - 1206 - 635 - 393 S0 + 93 + 40 + 213

1

)tan()(

160

93253

JKS

S

SSS

sys

sys

treacproductsys kJHsys 178)1206(1028

Rxn Temp dependent Spontaneous at High ↑Temp

Decomposition limestone CaCO3 spontaneous?

1597

298

)178000(

JKS

S

T

HS

surr

surr

surr

Page 26: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Predict entropy change - quatitatively

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Reactant Product

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

1

)tan()(

22

7048

JKS

S

SSS

sys

sys

treacproductsys kJHsys 6)286(292

surrsysuni SSS

122022

JKS

SSS

uni

surrsysuni

Is Freezing spontaneous?

Unit for ∆S - JK-1 Unit for ∆H - kJ

∆S uni = ∆S sys + ∆S surr ↓

∆S uni < 0 - Freezing at 298K - Non Spontaneous

Reactant Product

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Hsysθ = ∑∆Hf

θ(pro) - ∑∆Hf

θ(react)

1

)tan()(

22

7048

JKS

S

SSS

sys

sys

treacproductsys kJHsys 6)286(292

18.22

263

)6000(

JKS

S

T

HS

surr

surr

surr

surrsysuni SSS

18.08.2222

JKS

SSS

uni

surrsysuni

∆S uni = ∆S sys + ∆S surr ↓

∆S uni > 0 -Freezing at 263K - Spontaneous

9 10 H2O (l) → H2O(s) H2O (l) → H2O(s)

H2O (l) → H2O(s) ∆Hf

0 - 286 - 292 S0 + 70 + 48

H2O (l) → H2O(s) ∆Hf

0 - 286 - 292 S0 + 70 + 48

Freezing at 298K (25C) Freezing at 263K (-10C)

Rxn Temp dependent Spontaneous at Low ↓ temp

120

298

)6000(

JKS

S

T

HS

surr

surr

surr

Page 27: IB Chemistry on Entropy and Laws of Thermodynamics

N2O4 (g) → 2NO2(g)

Reactant Product

Entropy

Ice (s) Water (l)

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Method to calculate entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Qualitatively

Solid → Liquid NaCI(s) → Na+(aq) + CI -(aq)

N2O4 (g) → 2NO2(g)

Reactant Product

S θ Less More

More microstates (More dispersion/random/freedom of motion)

Solid → liq → gas

Higher ↑ entropy

Greater number particles in product More liq/gas in product

Dispersion Energy Microstate

More dispersion of energy (Electronic, translational, rotational, vibrational, thermal)

Higher entropy ∆S > 0 (+ve) - Spontaneous

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Srysθ = More - Less

= +ve > 0

S θ Less More

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Ssysθ = More - Less

= +ve > 0

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Ssysθ = More - Less

= +ve > 0

NaCI(s) → Na+(aq) + CI -(aq)

S θ Less More

Reactant Product

Qualitatively

Unit - J mol -1 K-1

Page 28: IB Chemistry on Entropy and Laws of Thermodynamics

Reactant Product

Entropy

Liq N2(l) Gas N2 (g)

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Method to calculate entropy

Gas mixes Solution diffuse Heat flow hot →cold

X X X

Qualitatively

Liquid → Gas

Reactant Product

S θ Less More

More microstates (More dispersion/random/freedom of motion)

Solid → liq → gas

Higher entropy

Greater number particles in product More liq/gas in product

Dispersion Energy Microstate

More dispersion of energy (Electronic, translational, rotational, vibrational, thermal)

Higher entropy ∆S > 0 (+ve) - Spontaneous

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Ssysθ = More - Less

= +ve > 0

S θ Less More

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Ssysθ = More - Less

= +ve > 0

∆Ssysθ = ∑Sf

θ(pro) - ∑Sf

θ(react)

∆Ssysθ = More - Less

= +ve > 0

NH4NO3(s) → NH4+

(aq) + NO3 -(aq)

S θ Less More

Reactant Product

Qualitatively

NH4NO3 (s) → NH4 +(aq) + NO3 - (aq) Ba(OH)2 .8H2O(s) + 2NH4NO3 (s) →

Ba2+(aq) + 2NO3

-(aq) + 2NH3 (g) + 10H2O(aq)

Ba(OH)2 .8H2O(s) + 2NH4NO3 (s) → Ba2+(aq) + 2NO3

- (aq) + 2NH3 (g) +10H2O(aq)

Unit - J mol -1 K-1

+

Page 29: IB Chemistry on Entropy and Laws of Thermodynamics

Entropy decrease ↓

Entropy

Why gas mixes and not unmix? Why conc solution diffuse and not undiffuse? Why heat flow from hot to cold?

Predict entropy change - qualitatively

Gas mixes Solution diffuse Heat flow hot →cold

X X X

NH4NO3 (s) → NH4 +(aq) + NO3 - (aq)

C3H8(g) + 5O2 (g) → 3CO2(g) + 4H2O(g) 2H2(g) + O2 (g) → 2H2O(l)

2Cu(s) + O2 (g) → 2CuO(s)

Br2(l) → Br2(g)

Ag+(aq) + Br-

(aq) → AgBr(s) H2(g) + CI2 (g) → 2HCI(g)

Cu2+(aq) + Zn(s) → Cu(s) + Zn2+

(aq) CaCO3 (s) → CaO(s) + CO2 (g)

1

Entropy decrease ↓

Entropy decrease ↓ Entropy increase ↑

Entropy increase ↑ Entropy increase ↑

Entropy increase ↑

Little change

Little change

2 3

4

Reactant Product

aq - more disorder solid - more order S higher ↑ S - Lower ↓

Reactant Product

g - more disorder solid - more order S higher ↑ S - Lower ↓

Reactant Product

Both sides equal number mol gas

Reactant Product

g - more disorder liq - more order S higher ↑ S - Lower ↓

Reactant Product

liq- more order g - more disorder S Lower ↓ S - Higher↑

Reactant Product

less g- more order more g - more disorder S Lower ↓ S - Higher↑

Reactant Product

Both sides equal number mol solid

Reactant Product

solid- more order aq - more disorder S Lower ↓ S - Higher↑

Reactant Product

solid- more order g - more disorder S Lower ↓ S - Higher↑

5 6

7 8 9