Title: Chapter 5: thermochemistry
1Chapter 5thermochemistry
- By Keyana Porter
- Period 2
- AP Chemistry
2What is thermochemistry?
- Thermodynamics the study of energy and its
transformations - Thermochemistry is one aspect of thermodynamics
- The relationship between chemical reactions and
energy changes - Transformation of energy (heat) during chemical
reactions
35.1Kinetic Potential Energy
- Energy is the capacity to do work or the transfer
heat - Objects possess energy in 2 ways
- Kinetic energy due to motion of object
- Potential/Stored energy result of its
composition or its position relative to another
object - Kinetic energy (Ek) of an object depends on its
mass (m) and speed (v) - Ek ½ mv2
- Kinetic energy increases as the speed of an
object and its mass increases - Thermal energy energy due to the substances
temperature associated with the kinetic energy
of the molecules
45.1Kinetic Potential Energy
- Potential energy is a result of attraction
repulsion - Ex an electron has potential energy when it is
near a proton due to the attraction
(electrostatic forces) - Chemical energy due to the stored energy in the
atoms of the substance
55.1Units of Energy
- joule (J) SI unit for energy
- 1 kJ 1000 J
- calorie (cal) non-SI unit for energy amount of
energy needed to raise the temperature of 1 g of
water by 1oC - 1 cal 4.184 J (exactly)
- Calorie (nutrition unit) 1000 cal 1 kcal
- A mass of 2 kg moving at a speed of 1 m/s
kinetic energy of 1 J - Ek ½ mv2 ½ (2 kg)(1 m/s)2 1 kg-m2/s2 1 J
65.1System Surroundings
- System (chemicals) portion that is singled out
of the study - Surroundings (container and environment including
you) everything else besides the system - Closed system can exchange energy, in the form
of heat work, but not matter with the
surroundings
75.1Transferring Energy Work Heat
- Energy is transferred in 2 ways
- Cause the motion of an object against a force
- Cause a temperature change
- Force (F) any kind of push or pull exerted on an
object - Ex gravity
- Work (w) energy used to cause an object to move
against force - Work equals the product of the force and the
distance (d) the object is moved - w F x d
- heat the energy transferred from a hotter object
to a colder one - Combustion reactions release chemical energy
stored in the form of heat
85.2Internal Energy
- The First Law of Thermodynamics Energy is
conserved it is neither created nor destroyed - Internal energy (E) sum of ALL the kinetic and
potential energy of all the components of the
system - The change in internal energy the difference
between Efinal Einitial - ?E Efinal Einitial
- We can determine the value of ?E even if we
dont know the specific values of Efinal and
Einitial - All energy quantities have 3 parts
- A number, a unit, and a sign (exothermic versus
endothermic)
95.2Relating ?E to Heat Work
- A chemical or physical change on a system, the
change in its internal energy is given by the
heat (q) added to or given off from the system - ?E q w
- both the heat added to and the work done on the
system increases its internal energy
10Sign Conventions Used and the Relationship Among
q, w, and ?E
Sign Convention for q q gt 0 Heat is transferred from the surroundings to the system (endothermic) q lt 0 Heat is transferred from the system to the surroundings (exothermic)
Sign convention for w w gt 0 Work is done by the surroundings on the system w lt 0 Work is done by the system on the surroundings
Sign of ?E q w q gt 0 and w gt 0 ?E gt 0 q gt 0 and w lt 0 the sign of ?E depends on the magnitudes of q and w q lt 0 and w gt 0 the sign of ?E depends on the magnitudes of q and w q lt 0 and w lt 0 ?E lt 0
115.2Endothermic Exothermic Processes
- Endothermic system absorbs heat
- Ex melting of ice
- Exothermic system loses heat and the heat flows
into the surroundings - Ex freezing of ice
- The internal energy is an example of a state
function - Value of any state function depends only on the
state or condition of the system (temperature,
pressure, location), not how it came to be in
that particular state - ?E q w but, q and w are not state functions
125.3Enthalpy
- Enthalpy (H) state function the heat absorbed
or released under constant pressure - The change in enthalpy equals the heat (qP)
gained or lost by the system when the process
occurs under constant pressure - ?H Hfinal Hinitial qP
- only under the condition of constant pressure is
the heat that is transferred equal to the change
in the enthalpy - The sign on ?H indicated the direction of heat
transfer - value of ?H means it is endothermic
- - value of ?H means it is exothermic
135.4Enthalpies of Reaction
- Enthalpy of reaction (?Hrxn) the enthalpy change
that accompanies a reaction - The enthalpy change for a chemical reaction is
given by the enthalpy of the products minus the
reactants - ?H H(products) H(reactants)
- Thermochemical equations balanced chemical
equations that show the associated enthalpy
change - The magnitude of ?H is directly proportional to
the amount or reactant consumed in the process
145.4Enthalpies of Reaction
- The enthalpy change for the reaction is equal in
magnitude but opposite in sign to ?H for the
reverse reaction - CO2(g) 2H2O(l) ? CH4(g) 2O2(g) ?H 890 kJ
CH4(g) 2O2(g)
Enthalpy ?
Reversing a reaction changes the sign but not the
magnitude of the enthalpy change ?H2 - ?H1
?H1 - 890 kJ
?H2 890 kJ
CO2(g) 2H2O(l)
155.4Enthalpies of Reaction
- The enthalpy change for a reaction depends on the
state of the reactants and products - Ex CH4 (g) 2O2 (g) ? CO2 (g) 2H2O (l)
- ?H -890 kJ
- If the product was H2O (g) instead of H2O (l),
the ?H would be - 820 kJ instead of - 890 kJ
165.5Calorimetry/Heat Capacity Specific Heat
- Calorimetry the measure of heat flow
- Calorimeter measures heat flow
- Heat capacity the amount of heat required to
raise its temperature by 1 K - The greater the heat capacity of a body, the
greater the heat required to produce a given rise
in temperature - Molar heat capacity the heat capacity of 1 mol
of a substance - Specific heat the heat capacity of 1 g of a
substance measured by temperature change (?T)
that a known mass (m) of the substance undergoes
when it gains or loses a specific quantity of
heat (q) -
175.5Calorimetry/Heat Capacity Specific Heat
- specific heat quantity of heat transferred
- (grams of substance) x (temperature
change) - q
- m x ?T
- Practice Exercise (BL page 160)
- Calculate the quantity of heat absorbed by 50 kg
of rocks if their temperature increases by 12.0
OC. (Assume the specific heat of the rocks is .82
J/g-K.)
185.5Calorimetry/Heat Capacity Specific Heat
- Solving the problem
- q (specific heat) x (grams of substance) x ?T
- (0.82 J/g-K)(50,000 g)(285 K)
- 4.9 x 105 J
195.5Constant-Pressure Calorimetry
- The heat gained by the solution (qsoln) is equal
in magnitude and opposite in sign from the heat
of the reaction - qsoln (specific heat of solution) x (grams of
solution) x ?T - qrxn - For dilute aqueous solutions, the specific heat
of the solution is approx. the same as water
(4.18 J/g-K) - Practice Exercise (BL page 161)
- When 50 mL of .100M AgNO3 and 50.0 mL of .100 M
HCl are mixed in a constant-pressure calorimeter,
the temperature of the mixture increases from
22.30oC to 23.11oC. The temperature increase is
caused by this reaction - AgNO3 HCl ? AgCl HNO3
- Calculate ?H for this reaction, assuming that the
combined solution has a mass of 100 g and a
specific heat of 4.18 J/g-oC
205.5Constant-Pressure Calorimetry
- Solving the problem
- qrxn -(specific heat of solution) x (grams of
solution) x ?T - - (4.18 J/g-oC)(100 g)(0.8 K)
- - 68,000 J/mol
215.5Bomb Calorimetry (Constant-Volume Calorimetry)
- Bomb calorimeter used to study combustion
reactions - Heat is released when combustion occurs, absorbed
by the calorimeter contents, raising the
temperature of the water (measured before and
after the reaction) - To calculate the heat of combustion from the
measured temperature increase in the bomb
calorimeter, you must know the heat capacity of
the calorimeter (Ccal) - qrxn - Ccal x ?T
225.6Hesss Law
- Hesss Law if a reaction is carried out in a
series of steps, ?H for the reaction will be
equal to the sum of the enthalpy changes for the
individual steps - CH4 (g) 2O2 (g) ? CO2 (g) 2H2O (g) ?H -802
kJ - (ADD)2H2O (g) ? 2H2O (l) ?H -88 kJ
- CH4 (g) 2O2 (g) 2H2O (g)? CO2 (g) 2H2O (g)
2H2O (l) - ?H -890 kJ
235.6Hesss Law
- Practice Exercise 5.8 (BL page 165)
- Calculate ?H for the reaction
- 2C (s) H2 ? C2H2 (g)
- Given the following reactions and their
respective enthalpy changes - C2H2 (g) 5/2 O2 ? 2CO2 (g) H2O (l) ?H
-1299.6 kJ - C (s) O2 (g) ? CO2 (g) ?H -393.5 kJ
- H2 (g) ½ O2 (g) ? H2O (l) ?H -285.8 kJ
245.6Hesss Law
- Solving the problem
- 2CO2 (g) H2O (l) ? C2H2 (g) 5/2 O2 ?H
1299.6 kJ - 2C (s) 2O2 (g) ? 2CO2 (g) ?H -393.5 kJ
(2) - -787.0 kJ
- H2 (g) ½ O2 (g) ? H2O (l) ?H -285.8 kJ
- 2C (s) H2 ? C2H2 (g) ?H 226.8 kJ
- if the reaction is reversed, the sign of ?H
changes - if reaction is multiplied, so is ?H
25Enthalpy Diagram
- The quantity of heat generated by combustion of 1
mol CH4 is independent of whether the reaction
takes place in one or more steps - ?H1 ?H2 ?H3
265.7Enthalpies of Formation
- Enthalpies of vaporization ?H for converting
liquids to gases - Enthalpies of fusion ?H for melting solids
- Enthalpies of combustion ?H for combusting a
substance in oxygen - Enthalpy of formation (?Hf) enthalpy change
where the substance has been formed from its
elements - Standard enthalpy (?H o) enthalpy change when
all reactants and products are at 1 atm pressure
and specific temperature (298 K) - Standard enthalpy of formation (?Hof) the
enthalpy change for the reaction that forms 1 mol
of the compound from its elements, with all
substances in their standard states - ?Hof 0 for any element in its purest form at
295 K and 1 atm pressure
275.7Enthalpies of Formation
- The standard enthalpy change for any reaction can
be calculated from the summations of the
reactants and products in the reaction - ?H orxn n ?H of (products) - m?H
of (reactants) - Practice Problem 5.9 (BL page 169)
- Calculate the standard enthalpy change for the
combustion of 1 mol of benzene, C6H6 (l), to CO2
(g) and H2O (l).
285.7Enthalpies of Formation
- Solving the problem
- C6H6 (l) 15/2 O2 (g) ? 6CO2 (g) 3H2O (l)
- ?H orxn 6? H of (CO2) 3? H of (H2O) ?H of
(C6H6) 15/2 ?H of (O2) - 6(-393.5 kJ) 3(-285.8 kJ) (49.0 kJ)
15/2 (0 kJ) - (-2361 857.4 49.0) kJ
- -3267 kJ
29Extra Equations
- Force mass x 9.8 m/s2
- Internal energy ?E Efinal Einitial
- Entropy ? S Sfinal Sinitial
- Enthalpy ? H Hfinal Hinitial
- Gibbs Free Energy ? G Gfinal Ginitial
- ? S ? H / T