Title: Unit 8 Chapter 16 Thermochemistry
1Unit 8- Chapter 16Thermochemistry
Thermodynamics
- One of Mrs. Dorrs faaaaaaavorite topics!!!
2The first law of thermodynamics
- Recall the law of conservation of energy- energy
can be neither created or destroyed. - The 1st Law of Thermodynamics is simply a
restatement- The energy of the universe is
constant. - We are going to look at the energy involved in
chemical reactions and prove not only the 1st law
of thermodynamics, but the 2nd as well
3Systems
- System ? surroundings open system
- matter
- System ? surroundings closed system
- (matter is trapped but it can
exchange energy) - matter
- System ? surroundings Isolated system
- energy (neither the matter or
energy from the system can be
exchanged)
4Boundaries of Systems
- Diathermic (closed system) boundary that permits
heat transfer - Adibatic (isolated system) prevents heat or
matter transfer
5Work
- Work is defined as force acting over a distance
- W F d it is measured in Joules
(J) - note 1 Latm
101.32 J - Consider a frictionless piston system with a
constant Pexternal see side board - Total work
- W -?Pext dV ? -Pext?dV
- W -Pext (Vf Vi)
- Therefore W -Pext ?V
6- Example 1 Consider an ideal gas in a piston
chamber expanding against constant Pext and at
constant temperature. The gas has an initial
volume of 2.0L, a final volume of 5.50L, an
initial pressure equal to 8.00atm and an external
pressure of 1.75atm. Determine a). the
work and b). the final pressure.
7- Work
- Expansion ? W -Pext ?V
- Compression ? W Pext ?V
- If Pext 0 what happens to work?
- There is NO WORK under the condition of free
expansion (Pext 0) - The only other time there is NO WORK is when ?V
0
8Example
- Consider a can of spray paint
- A. Can of spray discharged (can system)
- B. Can of spray discharged (spray system)
- A. no work being done b/c no ?
- B. work done on atmosphere/surroundings by the
system/spray - W -Pext ?V
9System Processes
- Irreversible ? No Equilibrium
- Reversible ? continuous Equilibrium state with
the surroundings (small incremental changes) - For Reversible Changes Pext Pint
- Wrev -?Pint dV
- So we can say Wrev -? nRT/V dV
- Then see side board for full derivation
10Heat- Its getting hot in here
- Heat, q if heat is flowing in/ gaining heat
- - if heat is flowing out/ losing heat
- Heat is the measure of thermal energy transfer
that can be determined in the temperature change
of the object (its a way to follow the energy
change of a system)
11Equations with Heat
- 1. q m c ?T ?intensive property
- m is mass, c is specific heat of substance
- 2. q C ?T ?extensive property
- C is the heat capacity of substance
- 3. q IVt ?intensive property
- I is current, V is voltage, t is time
12Internal Energy The 1st Law of Thermodynamics
- Internal energy, E total energy of system
- Recall adiabatic isolated system no heat or
matter transfer! - Recall the 1st Law- For an isolated system, the
total energy of a system remains constant,
therefore ?E 0 - ?E q W (general)
- ?E W (adiabatic)
13Example
- A gas sample changes in volume from 2.0L to 4.0L
against an external pressure of 1.50 atm, while
absorbing 1,000J of heat, what is ?E of the
system?
14State Functions
- State function- path independent
- Ex- P, V, T, ?E, ?H
- NOT State functions- q and W
- In-exact differentials ?dW W
- ?dq q
- Exact differentials ?dE ?E
15Enthalpy
- At constant pressure, the change in enthalpy ?H
of the system is equal to the energy flow as heat - H E PintV
- ?H ?E ?(PV)
- ?H ?E ?ngRT
- If no gases are involved, or if ?n 0, then ?E
?H - See side of board for chain rule derivation
16Example
- A piston filled with 0.0400mol of an ideal gas
expands reversibly from 50.00mL to 375.0mL _at_
constant temperature of 37?C. As it does so, it
absorbs 208J of heat. Calculate q, W, ?U, and
?H for this process.
17?H
- ?H ?Hproducts ?Hreactants
- If ?H is positive the reaction is endothermic
- If ?H is negative the reaction is exothermic
18Enthalpy Calorimetry
- Recall a calorimeter is used to experimentally
determine the heat associated with a chemical
reaction - Calorimetry is the science of measuring heat
- Heat capacity C heat absorbed
- ______________________
- inc. in
temperature - Heat capacity can be given per gram specific
heat capacity c ? J/?Cg or J/Kg - Or it can be given per mole molar heat capacity
C ?J/?Cmol or J/Kmol
19Constant Pressure Calorimetry
- Constant pressure!
- For these reactions ?H qp
- So we can use qp mc?T or qp C?T
20Example of Constant Pressure Calorimetry
- When 1.00L of 1.00M Ba(NO3)2 solution at 25.0?C
is mixed with 1.00L of 1.00M Na2SO4 solution at
the same temperature in a calorimeter, the white
solid BaSO4 forms and the temperature of the
mixture increases to 28.1?C. Assuming that the
calorimeter absorbs only a negligible quantity of
heat, that the specific heat capacity of the
solution is 4.18J/?Cg, and that the density of
the final solution formed is 1.0g/mL, calculate
the enthalpy change per mole of BaSO4 formed.
21Constant Volume Calorimetry
- Calorimetry experiments can also be done at
constant volume - For a constant volume procses, the ?V 0, so
work, w 0 also - ?E q W q qv
22Constant Volume Example
- Consider the combustion of octane, C8H18. A
0.5269g sample of octane is placed in a bomb
calorimeter known to have a heat capacity of
11.3kJ/?C. The octane is ignited in the presence
of excess oxygen, and the temperature increase of
the calorimeter is 2.25?C. Determine the amount
of energy released per mole of octane.
23Heat of Reactions
- Standard states ?H?
- For a Compound-
- The standard state of a gaseous substance is a
pressure of exactly 1 atm - For a liquid or solid the standard state is the
pure liquid or solid - For a substance present in solution, the standard
state is a concentration of exactly 1M - For an Element-
- The standard state of an element is the form in
which the element exists under conditions of 1atm
and 25?C. (ex- O2(g), Na(s), and Hg(l)
24- Standard enthalpy of formation, ?Hf? the change
in enthalpy that accompanies the formation of one
mole of a compound from its elements with all
substances in their standard states - The degree symbol ? indicates standard conditions
- ?H?rxn ??H?products - ??H?reactants
- DO NOT put pure elements in this eqn. ex-O2
- When a rxn is reversed, change the sign on ?H
- When the balanced eqn. is multiplied by an
integer, the value of ?H must be multiplied by
the same integer - Use this equation for heat of fusion, heat of
formation, heat of vaporization, heat of
combustion, heat of synthesis ? any enthalpy
change!
25Read Chapter 6, section 5 6, pages 267-281 by
Friday.
26Example
- Determine the standard enthalpy change for the
combustion of methane.
27Hesss Law
- Recall enthalpy, ?H is independent of pathway (a
state function) - Hesss Law states in going from a particular set
of reactants to a particular set of products, the
change in enthalpy is the same whether the
reaction takes place in one step or in a series
of steps - So ?H? ?npH?products - ?nr ?H?reactants
28Hesss Law Example
- Diborane (B2H6) is a highly reactive boron
hydride, which was once considered as a possible
rocket fuel for the U.S. space program.
Calculate the ?H for the synthesis of diborane
from its elements according to the equation - 2B(s) 3H3(g)
- Using the following data
- 2B(s) 3/2O2(g) ? B2O3(s) ?H -1273 kJ
- B2H6(g) 3O2(g) ? B2O3(s) 3H2O(g) ?H -2035 kJ
- H2(g) ½ O2(g) ? H2O(l) ?H -286 kJ
- H2O(l) ? H2O(g) ?H 44 kJ
29The 2nd Law of Thermodynamics
- Recall that the 1st Law of Thermodynamics deals
with energy change - The 2nd Law of Thermodynamics states that in any
spontaneous process there is always an increase
in the entropy of the universe - To reword the entropy of the universe is
increasing - Energy is conserved in the universe, but entropy
is not
30Entropy
- Spontaneous process is one that occurs without
outside intervention - Note a spontaneous process irreversible
process - If it is a reversible process ?S 0
- Thermodynamics tells us only about the direction,
not the speed. - Entropy, S the thermodynamic function that
measures randomness or disorder
31Entropy
- ?Suniv ?Ssys ?Ssurr
- If ?Suniv is , it is spontaneous in the
direction written - If ?Suniv is -, it is spontaneous in the opposite
direction - If ?Suniv 0, the process has no tendency to
occur the system is _at_ equilibrium
32The Effect of Temperature on Spontaneity
- For Reversible Irreversible processes
- ?Ssurr qsurr / Tsurr
- Since _at_ constant P q ?H we can say
- ?Ssurr - ?H / T
- This means that if the rxn is exothermic, ?H -,
but since heat flows into the surroundings,
?Ssurroundings is positive
33?Ssurr Example
- Antimony, the pure metal is recovered via
different reactions, depending on the composition
of the ore. - Iron is used to reduce antimony in sulfide ores
- Sb2S3(s) 3Fe(s) ? 2Sb(s) 3FeS(s) ?H -125kJ
- Carbon is used as the reducing agent for oxide
ores - Sb4O6(s) 6C(s) ? 4Sb(s) 6CO(g) ?H 778kJ
- Calculate ?Ssurr for each of these reactions at
25?C and 1atm.
34Summary of Entropy
- Recall ?Suniv ?Ssurr ?Ssys
- _______________________________________
- ?Ssys ?Ssurr ?Suniv Spontaneous?
- Yes
- - - - No
- - ? Yes, if ?Ssys is larger
than ?Ssurr - - ? Yes, if ?Ssurr is larger than
?Ssys
35Free Energy
- Free energy, G is defined by the following
relationship ?GRxn ??Gproducts -
??Greactants - And G H - TS
- For a process that occurs _at_ constant T, the
change in free energy ?G is - ?G? ?H? - T?S? This is called the
Gibbs-Helmholtz Eqn. - To relate it to spontaneity
- ?Suniv - ?G / T _at_ constant T P
- This means _at_ constant T P a process is
spontaneous only if ?G is NEGATIVE.
36- We can re-phrase this to say a process (_at_
constant T P) is spontaneous in the direction
in which the free energy decreases (-?G means
?Suniv). - We now have two variables that determine
spontaneity (?G), ?S ?H - Case Result
- ?S , ?H - Spontaneous _at_ all temps.
- ?S , ?H Spontaneous _at_ high temps.
- ?S -, ?H - Spontaneous _at_ low temps.
- ?S , ?H NOT Spontaneous _at_ ANY Temperature
37Example
- At what temperatures is the following process
spontaneous _at_ 1atm? - Br2(l) ? Br2(g)
- ?H? 31.0kJ/mol ?S? 93.0J/Kmol
- What is the normal boiling point of liquid Br2?
38Entropy the States of Matter
- Solids have low entropy, liquids have higher
entropy, solutions have higher entropy, gases
have the highest entropy - If the of gaseous molecules in the products is
greater than the of gaseous molecules in the
reactants, the forward rxn favors entropy, its - The reverse rxn is favored if the opposite is
true - Ex Predict the sign of ?S? for each rxn
- CaCO3(s) ? CaO(s) CO2(g)
- 2SO2(g) O2(g) ? 2SO3(g)
39Free Energy Chemical Reactions
- Standard free energy change, ?G?, the change in
free energy that will occur if the reactants in
their standard states are converted to the
products in their standard states - Note you can use Hesss Law with ?G?!
- ?G? ?npG?products - ?nr ?G?reactants
- ?G? 0 for the formation of an element in its
standard state
40Pressure Free Energy
- Free energy is affected by Pressure
- G G? RTln(P)
- G is the free energy of the gas _at_ pressure P, G?
is the free energy of the gas _at_ 1atm, and R is
the universal gas constant, use 3.14 J/molK - Also, ?G nRTln(Pf/Pi)
- ?G ?G? RTlnQ ? Q is the rxn quotient
- For 2A 3B ? 4C Q C4/ A2B3
41Pressure Example
- Calculate ?G at 25?C for this rxn where carbon
monoxide gas at 5.0 atm and hydrogen gas at
3.0atm are converted to liquid methanol - CO(g) 2H2(g) ? CH3OH(l)
42Free Energy Equilibrium
- Equilibrium represents the lowest free energy
value available - _at_ equilibrium ?G 0 and Q K
- So, ?G 0 ?G ? RTln(K) or ?G ? -RTln(K)
- K is the equilibrium constant where
eA fB ? gC hD - Cg Dh
- K ------------
- Ae Bf
43?G ? and K yes, memorize these!!!
- ?G ? K
- --------------------------------------------------
------- - ?G ?0 K 1
- ?G ? lt 0 K gt 1
- ?G ? gt 0 K lt 1
44- Also, when ?G 0, then then ?H T?S or T ?H
/ ?S
45Equilibrium Example
- The overall reaction for the corrosion (rusting)
of iron by oxygen is - 4Fe(s) 3O2(g) ? 2Fe2O3(s)
- Using the following data, calculate the
equilibrium constant for this reaction at 25?C. - Substance ?H?f (kJ/mol) S? (J/Kmol)
- Fe2O3(s) -826 90
- Fe(s) 0 27
- O2(g) 0 205
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