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Chapter 5. Thermochemistry. Definitions. Thermochemistry - the study of how energy in the form of heat is consumed and produced by chemical reactions. Thermochemical Reaction : Example H 2 ( g ) + O 2 ( g ) 2 H 2 O ( l ) + heat
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Chapter 5 Thermochemistry
Definitions • Thermochemistry - the study of how energy in the form of heat is consumed and produced by chemical reactions. • ThermochemicalReaction: Example H2(g) + O2(g) 2 H2O (l) + heat • Energy is anything having the capacity to do work or to transfer heat. • Work is Force X Distance • Thermodynamics The study of energy and its transformation from one form to another.
Energy Examples Definition-Energy is anything with the capacity to do work, or create heat. • Food • Gasoline • Electricity • An apple on a tree • A baseball moving
Energy Units Units of Energy • Joules = kg(m/s)2 • Calories, an older unit; the energy to increase one gram of water one deg. C • Calories, unit of food energy = kcal
DefinitionsContinued • Heat is energy transferred between objects because of a difference in their temperatures. • Thermodynamics is the study of relationship between chemical reactions and changes in heat energy. • Heat transfer is the process of heat energy flowing from one object into another
Two Types of Energy Potential:due to position or composition - can be converted to work PE = mgh (m = mass, kg, g = force of gravity(9.8m/s2), and h = vertical distance in meters) • These units multiplied together = joule • (chemical energy is a form of potential energy) • Kinetic:due to motion of the object KE = 1/2 mv 2 (m = mass(kg), v = velocity(m/s)) • These units multiplied together also equal a joule • Joule = kg(m/s)2
Potential Energy: A State Function • Depends only on the present state of the system - not how it arrived there. • It is independent of pathway.
Other State Functions? • Heat (a form of energy)? • Work? Altitude? • Altitude?
Other State Functions? • Heat (a form of energy)? Yes, not path dependent • Work? • Altitude?
Other State Functions? • Heat (a form of energy)? Yes, not path dependent • Work? No, work depends on path • Altitude?
Other State Functions? • Heat (a form of energy)? Yes, not path dependent • Work? No, work depends on path • Altitude? Yes, does not depend on path • Enthalpy ΔH,?
Other State Functions? • Heat (a form of energy)? Yes, not path dependent • Work? No, work depends on path • Altitude? Yes, does not depend on path • Enthalpy ΔH,? Yes, does not depend on path
The Nature of Energy • Energy is conserved: Law of Conservation of Energy states that energy cannot be created nor destroyed, but converted from one form to another
Energy at the Molecular Level Kinetic energy at the molecular level depends on the mass and velocity of the particle but because its velocity depends on temperature KE does too. • As temperature increases then the KE of the same will increase. One of the most important forms of potential energy at the atomic-molecular level arises from electrostatic interactions. Potential can be converted into kinetic • Example: an apple falling from a tree
Electrostatic Potential Energy Coulombic attraction, not gravitational force, determines the potential energy of matter at the atomic level. • Eel is the electrostatic potential energy • Q is the charge in coulombs • d is the distance between particles
Electrostatic Potential Energy Bond length Energy of an ionic bond • Bonds contain potential energy • Energy required to break bonds • Energy released when bonds are created
Crystal Lattice of NaCl Ionic compounds do not exist as discrete molecules. Instead they exist as crystals where ions of opposite charges occupy positions known as lattice sites. In an ionic compound the ions organize in such a way as to minimize repulsive and maximize attractive forces.
- + + - The arrangement of charged particles in a covalent bond organized in such a way as to minimize repulsive and maximize attractive forces to give the lowest potential energy.
Terms Describing Energy Transfer • System: the part of the universe that is the focus of a thermodynamic study. • Example a beaker or test tube in the lab • Surroundings: everything in the universe that is not part of the system. • Universe = System + Surroundings • An isolated system exchanges neither energy nor matter with the surroundings.
Heat Flow • In an exothermic process, heat flows from a system into its surroundings. • In an endothermic process, heat flows from the surroundings into the system
Internal Energy • The internal energy of a system is the sum of all the KE and PE of all of the components of the system.
First Law of Thermodynamics • The first law of thermodynamics states that the energy gained or lost by a system must equal the energy lost or gained by surroundings. ΔE = q + w (mathematical statement) • The calorie (cal) is the amount of heat necessary to raise the temperature of 1 g of water 1oC. • The joule (J) is the SI unit of energy; 4.184 J = 1 cal.
Change in Internal Energy E = q + w • E = change in system’s internal energy • q = heat • Endothermic +q • Exothermic -q • Expansion –w (since system is losing energy to do work) • Compression +w
First Law Problem Find the change in energy of a system when 12 j of energy flows into the system while the system is doing 8 j of work on the surroundings.
First Law Problem Find the change in energy of a system when 12 j of energy flows into the system while the system is doing 8 j of work on the surroundings. ΔE = q + w ↔ ΔE = + 12 – 8 = 4 j
PV Work Expansion Facts Atm = 14 lb/in2 W = F x d ↓ A P = F/A F = PA h W = PA x d A ΔV = A x d W = P ΔV ΔV = Vfinal – Vinitial
PV Work Facts Expansion ΔV = Vfinal – Vinitial ΔV = A x d h A W = F x d P = F/A F = PA Since expansion is defined as negative work and ΔV is positive for expansion, then we change the sign of PΔV to–PΔV, Substituting W = PxAxd W = PΔV ΔE = q - P ΔV
PV Work Facts Expansion ΔV = Vfinal – Vinitial ΔV = A x d h A W = F x d P = F/A F = PA Since expansion is defined as negative work and ΔV is positive for expansion, then we change the sign of PΔV to–PΔV, Substituting W = PxAxd W = PΔV ΔE = q - P ΔV (L-atm = 101.3 j)
Calculation of Work Calculate the work in L•atm and joules associated with the expansion of a gas in a cylinder from 54 L to 72 L at a constant external pressure of 18 atm (Note that as the gas expands, it does work on its surroundings. Energy flows out of the gas, so it is a negative quantity)
Calculation of Work Calculate the work in L•atm and joules associated with the expansion of a gas in a cylinder from 54 L to 72 L at a constant external pressure of 18 atm (Note that as the gas expands, it does work on its surroundings. Energy flows out of the gas, so it is a negative quantity) W = -pΔV W = -18atm(72-54)L = -320L-atm j -320L-atm = -3.2 j 101.3 L-atm
Calculation of Work Calculate the work in L•atm and joules associated with the expansion of a gas in a cylinder from 54 L to 72 L at a constant external pressure of 18 atm (Note that as the gas expands, it does work on its surroundings. Energy flows out of the gas, so it is a negative quantity) Note: The result is negative, which we would predict relative to expansion. This is the reason that work is -pΔV, to give the correct sign for expansion. W = -pΔV W = -18atm(72-54)L = -320L-atm j -320L-atm = -3.2 j 101.3 L-atm
Enthalpy and Change in Enthalpy • Enthalpy (H) = E + PV ( mathematical definition) • Change in Enthalpy (H) = E + PV • At constant P, qP = E + PV, therefore qP = H • H = change in enthalpy: an energy flow as heat (at constant pressure) • H > 0, Endothermic; H < 0, Exothermic
Heat Capacities • Molar heat capacity (cp) is the heat required to raise the temperature of 1 mole of a substance by 1oC at constant pressure. • q = ncpT • Specific heat (cs) is the heat required to raise the temperature of 1 gram of a substance by 1oC at constant pressure. • Heat capacity (Cp) is the quantity of heat needed to raise the temperature of some specific object by 1oC at constant pressure.
Phase Change and Energy • Molar heat of fusion (Hfus) - the heat required to convert 1 mole of a solid substance at its melting point to 1 mole of liquid. • q = nHfus • Molar heat of vaporization (Hvap) - the heat required to convert 1 mole of a substance at its boiling point to 1 mole of vapor. • q = nHvap
WATER THERMO VALUES • Ice H2O (s) 2.06 j/g-°C • Water H2O (l) 4.184 j/g-°C • Steam H2O (g) 1.86 j/g-°C • Heat of Fusion (melting) 334.0 j/g • Heat of vaporization (evaporation) 2257 j/g
Practice During a strenuous workout, a student generates 2000 kJ of heat energy. What mass of water would have to evaporate from the student’s skin to dissipate this much heat?
Practice During a strenuous workout, a student generates 2000 kJ of heat energy. What mass of water would have to evaporate from the student’s skin to dissipate this much heat? g 2257 j
Practice During a strenuous workout, a student generates 2000 kJ of heat energy. What mass of water would have to evaporate from the student’s skin to dissipate this much heat? g 10 3 j 2257 j kj
Practice During a strenuous workout, a student generates 2000 kJ of heat energy. What mass of water would have to evaporate from the student’s skin to dissipate this much heat? g 10 3 j 2000 kj 2257 j kj
Practice During a strenuous workout, a student generates 2000 kJ of heat energy. What mass of water would have to evaporate from the student’s skin to dissipate this much heat? g 10 3 j 2000 kj = 886 g water 2257 j kj
Practice5.53 From Text Exactly 10 mL of water at 25oC was added to a hot iron skillet. All of the water was converted into steam at 100oC. If the mass of the pan was 1.20 kg and the molar heat capacity of iron is 25.19 J/mol•oC, what was the temperature change of the skillet?
Sample Problem Solution mole-°C 25.19 j
Sample Problem Solution mole-°C 55.85 g 25.19 j mole
Sample Problem Solution mole-°C 55.85 g kg 25.19 j mole 103 g
Sample Problem Solution mole-°C 55.85 g kg 25.19 j mole 103 g 1.20 kg