Thermodynamics - PowerPoint PPT Presentation

About This Presentation
Title:

Thermodynamics

Description:

Thermodynamics Heat Work Chemical Reactivity What drives chemical reactions? How do they occur? The first is answered by THERMODYNAMICS and the second by KINETICS. – PowerPoint PPT presentation

Number of Views:577
Avg rating:3.0/5.0
Slides: 55
Provided by: pyxi167
Category:

less

Transcript and Presenter's Notes

Title: Thermodynamics


1
Thermodynamics
Heat
Work
2
Heat is a form of energy
  • Mechanical work done on a system produces a rise
    in temperature like heat added to the system.

3
(No Transcript)
4
Joules Experiment
Joule showed that mechanical energy could
be converted into heat energy.
DT
M
F
Dx
H2O
W FDx
5
  • Thermodynamics Thermodynamics is concerned with
    interconversions of different forms of energy.
  • It was developed as a mathematical tool for
    studying phenomena such as the way in which heat
    energy can be converted into mechanical energy in
    heat engines
  • Thermodynamics provides a means for deciding
    whether a process will occur spontaneously
  • Spontaneous in this context implies nothing
    about how fast it will take place - e.g.
    combustion of a diamond
  • Thermodynamics is linked at a fundamental level
    to the nature of the universe
  • The Industrial Revolution depended on heat
    engines, most of which (like these steam engines)
    were of very low efficiency. The development of
    physical theories, and mathematical tools, to
    analyse these systems led to rapid improvements
    in technology.

6
  • Energy can be divided into two categories -
    kinetic energy and potential energy
  • Kinetic energy includes all forms of energy that
    result from movement - either linear motion or
    rotation.
  • Heat, which is molecular motion.
  • Radiant energy - the kinetic energy of photons of
    light and other electromagnetic radiation
  • Mechanical energy
  • Electrical energy as currents of moving electrons
    or charged particles
  • Potential energy includes all forms of energy
    that are stored.
  • Energy stored in chemical bonds
  • Energy stored in concentration gradients
  • Energy stored as electrical potential (separation
    of charges)
  • Energy stored in the nuclei of atoms
  • The basic unit of energy is the Joule (J)

7
Thermodynamic Systems
  • A thermodynamic system is a collection of matter
    which has distinct boundaries. OR
  • A real or imaginary portion of universe whish has
    distinct boundaries is called system. OR
  • A thermodynamic system is that part of universe
    which is under thermodynamic study.

8
Systems
Thermodynamic System A quantity of matter or a
region in space chosen for study. Surroundings Ev
erything external to the system. Boundary Surface
that separates the system from the surrounding.
It may be fixed or movable
9
Closed and Open Systems
Closed system (Control mass) A fixed amount of
mass chosen for study (no mass can cross its
boundary). Heat and work can cross the boundary,
volume may also change. e.g. piston
cylinder. Open system (Control volume) A
selected region chosen for study. Mass, heat and
work can cross its boundary, volume may also
change. e.g. water heater, car radiator, turbine,
nozzle. Isolated system A system closed to
mass, heat and work flows. It is not affected by
the surroundings.
10
Open Systems
11
Properties of a system
Thermodynamic Property A measurable quantity that
defines the condition of a system e.g.
temperature T pressure P mass
m volume V
density ?
12
Extensive and Intensive properties
  • Properties are of 2 types
  • Intensive properties Independent of mass. e.g.
    P, T, v, ?.
  • Extensive properties Change with mass. e.g. m, V,
    Energy

13
(No Transcript)
14
Temperature and 0th law of thermodynamics
Temperature Degree of hotness of coldness 0th
law of thermodynamics When 2 bodies have equality
of temperature with a 3rd body, then they have
equality of temperature with each other.
TA
TB
TC
15
Absolute scale of temperature
16
Internal Energy (E)
  • Definition The total of the kinetic and
    potential energy in a system.
  • E Kinetic Energy Potential Energy

17
The First Law of Thermodynamics
  • Internal Energy
  • Internal Energy total energy of a system.
  • Involves translational, rotational, vibrational
    motions.
  • Cannot measure absolute internal energy.
  • Change in internal energy,

18
First Law of Thermodynamics
  • The change in the internal energy of a system E,
    is equal to the heat input Q minus the work done
    by the system.
  • ?E Q-W
  • The internal energy is the energy stored in the
    system.
  • For an ideal gas the internal energy is the
    kinetic energy of the gas

19
The First Law of Thermodynamics
  • Relating DE to Heat(q) and Work(w)
  • Energy cannot be created or destroyed.
  • Energy of (system surroundings) is constant.
  • Any energy transferred from a system must be
    transferred to the surroundings (and vice versa).
  • From the first law of thermodynamics

20
Work
  • Work is a form of energy. Its the energy
    involved in moving something. If nothing moves,
    no work is done.
  • Work in chemical terms is usually done with
    pressure and volume changes.

21
The First Law of Thermodynamics
22
QUIZ
  • Calculate the energy change for a system
    undergoing a process in which 15.4 kJ of heat
    flows and where 6.3 kJ of work is done on the
    system.

23
ANSWER
  • ?E q w
  • q - 15.40 J
  • w 06.30 J
  • ?E - 15.40 J 06.30 J - 09.10 J

24
The First Law of Thermodynamics
  • Exothermic and Endothermic Processes
  • Endothermic absorbs heat from the surroundings.
  • An endothermic reaction feels cold.
  • Exothermic transfers heat to the surroundings.
  • An exothermic reaction feels hot.

25
Pressure-volume work
  • P f / A
  • Work done by the system (gas)
  • w f ?x
  • w P ?V

26
  • Example 2
  • A gas expands by 0.50 L against a constant
    pressure of 0.50 atm at 25 C. What is the work
    in erg done by the system? (1.0 atm 1.013 x 106
    dyne/cm2)
  • Solution
  • W - P?V
  • - (0.50 x 1.013 x 106 dyne/cm2) x 500 cm3
  • - 2.50 x 103 dyne/cm
  • - 2.50 x 103 erg

27
Reversible work
  • Isothermal work expansion against variable
    pressure.
  • n number of moles, R gas constant (8.314
    JK-1mol-1, 1.987 cal K-1mol-1, 0.0802 L.atm.
    K-1mol-1)
  • T absolute temperature

28
  • Example
  • What is the maximum work done in the isothermal
    reversible expansion of 2 moles of an ideal gas
    from 1 to 5 litres at 25 C?
  • Solution
  • 7976.43 J

29
Special Forms of the 1st law
  • ?E q w
  • Case 1 Isothermal process
  • ?E 0, hence, q - w
  • Case 2 Isochoic process
  • w 0, ?E qv
  • Case 3 Adiabatic process
  • q 0, ?E w
  • Case 4 Isobaric
  • ?E q w

30
(No Transcript)
31
(No Transcript)
32
Energy Changes in ChemicalReactions
  • How are energy changes measured?
  • One Answer Calorimetry, q Ccal?T
  • What thermodynamic quantities do we get?
  • Constant Volume qv ?E.
  • Constant Pressure qP ?H
  • In most calorimetry, ?T is very small, initial
  • and final states are at nearly constant T

33

34
Chemical Reactivity
  • What drives chemical reactions? How do they
    occur?
  • The first is answered by THERMODYNAMICS and the
    second by KINETICS.
  • Have already seen a number of driving forces
    for reactions that are PRODUCT-FAVORED.
  • formation of a precipitate
  • gas formation
  • H2O formation (acid-base reaction)
  • electron transfer in a battery

35
Chemical Reactivity
  • But energy transfer also allows us to predict
    reactivity.
  • In general, reactions that transfer energy to
    their surroundings are product-favored.

So, let us consider heat transfer in chemical
processes.
36
(No Transcript)
37
Enthalpy of Reaction from Heat of Formation
  • Standard Heat of Formation (?Hof)
  • The amount of energy gained or lost when1 mole
    of the substance is formed from its elements
    under standard conditions(25C, 1 atm 101.3
    kPa)

38
  • Example 2
  • Standard enthalpies of formation are C2H5OH(l)
    -228, CO2 (g) -394, and H2O(l) -286 kJ/mol.
    Calculate the enthalpy of the reaction,
  • C2H5OH (l) 3O2 (g) 2 CO2 (g) 3 H2O (l)
  • Solution
  • ?HR 3x?Hf(H2O (l)) 2x?Hf(CO2(g)) 1x?Hf
    C2H5OH(l) 3x?HfO2(g)
  • 3molX-286 kJ/mol 2molx-394
    kJ/mol-1molx-228 kJ/mol 3molx0.0 kJ/mol
  • - 858 (-788) -228 - 1546 228
    - 1418 kJ

39
Heat of Reactions from Bond Energies
  • When bonds are formed, energy is released.
  • In order to break bonds, energy must be absorbed
  • Exothermic Products have stronger bonds than
    the reactants.
  • Endothermic Products have weaker bonds than the
    reactants.

40
(No Transcript)
41
  • O2(g) 2O(g) ?H 490.4 kJ
  • H2(g) 2H(g) ?H 431.2 kJ
  • H2O(g) 2H(g) O(g) ?H 915.6 kJ
  • 2H2(g) O2(g) 2H2O(g)    ?H ?
  • ?H reaction bonds broken Energy (absorbed)
    - bonds formed Energy (released)
  • 2 H-H OO 4 O-H
  • 2 x 431.2 1 x 490.4 4 x 457.8
  • 862.4 490.4 1831.2
  • 1532.8 1831.2
  • - 478.4 kJ

42
(No Transcript)
43
Heat of Combustion
  • IS the Heat Evolved when One mole of a Fuel is
    Burned in Enough Oxygen

44
  • EXample
  • How much heat is evolved when 54.0 g glucose
    (C6H12O6) is burned according to this equation?
  • ?Hcomb -2808 kJ/mol, C 12, O 16, H 1
  • C6H12O6(s) 6O2(g) 6H2O(l)
    6CO2(g)
  • Answer
  • Mass of glucose 54.0 g C6H12O6
  • ?Hcomb -2808 kJ
  • Energy (q) ?
  • Convert grams of C6H12O6 to moles of C6H12O6
  • 54.0 g / 180 g mol-1 0.300 mol C6H12O6
  • ? H 0.300 mol x - 2808 kJ/mol - 842 kJ

45
Heat at constant VOLUME
  • If we consider a system at constant volume. ?V is
    zero. If ?V is zero, then the work is zero.
  • At constant volume the heat is equal to ?U.
  • We can measure heat at constant volume in a Bomb
    Calorimeter.
  • The calculations are the same for bomb
    calorimetry as for coffee-cup calorimetry.
  • The heat calculated is a measure of the INTERNAL
    ENERGY change instead of Enthalpy.

46
Finding ?H from ?E
  • We can find ?E from bomb calorimetry. But that is
    at constant volume.
  • How do we find ?H?
  • Here ?n is the change in number of moles of GAS
    in the balanced chemical equation.
  • ?E qp w ?H - P?V ?H - ?nRT

47
  • ?nRT
  • This is an amount of energy that would be
    represented as work if work could be done.
  • This can be zero if there is no change in number
    of moles of gas.

48
Application
  • For the reaction
  • Mg (s) ½ O2 (g) MgO (s)
  • the enthalpy change is -601.2 kJ. What is the
    internal energy change for this reaction? How
    many g of magnesium must react to effect an
    internal energy change of -22.4 kcal?

49
Hesss Law
  • The Enthalpy of a Reaction is the Same if it
    takes place in One or More than One step.

50
Hesss Law Energy Level Diagrams
Forming H2O can occur in a single step or in a
two steps. ?Htotal is the same no matter which
path is followed.
51
USING ENTHALPY
  • Making H2O from H2 involves two steps.
  • H2(g) 1/2 O2(g) ---gt H2O(g) 242 kJ
  • H2O(g) ---gt H2O(liq) 44 kJ
  • --------------------------------------------------
    ---------------
  • H2(g) 1/2 O2(g) --gt H2O(liq) 286 kJ
  • Example of HESSS LAW
  • If a rxn. is the sum of 2 or more others, the net
    ?H is the sum of the ?Hs of the other rxns.

52
(No Transcript)
53
QUIZs
  • The standard heat of formation, ?Hof, for sulfur
    dioxide (SO2) is -297 kJ/mol. How many kJ of
    energy are given off when 25.0 g of SO2 (g) is
    produced from its elements? 
  • The heat of reaction for the combustion of 1 mol
    of ethyl alcohol is -9.50 102 kJC2H5OH (l)
    3 O2 (g) ? 2 CO2 (g) 3 H2O (l) 9.5 102 kJ.
  • How much heat is produced when 11.5 g of
    alcohol is burned?
  • ?H for the complete combustion of 1 mol of
    propane is
  • -2.22 103 kJ
  • C3H8 (g) 5 O2 (g) ? 3 CO2 (g) 4 H2O (l)
  • Calculate the heat of reaction for the
    combustion of 33.0 g of propane.

54
(No Transcript)
Write a Comment
User Comments (0)
About PowerShow.com