Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of the universe (the system) Definitions: System: part of the universe in which we are interested Surroundings: where we make our observations (the universe) Boundary: separates above two
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Thermodynamics from Greek thermo dy’namis (heat and power) Studies energy changes and the direction of flow of energy usually in a well-defined part of.
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Thermodynamicsfrom Greek thermo dy’namis (heat and power)Studies energy changes and the direction of flow of energy usually in a well-defined
part of the universe (the system)
Definitions:
System: part of the universe in which we are interested
Surroundings: where we make our observations (the universe)
Boundary: separates above two
Heat and WorkHeat: transfer of energy that changes motions of atoms in the surroundings in a chaotic manner
Work: transfer of energy that changes motions of atoms in the surroundings in a uniform manner
= F x d
Energy• Definition: the capacity to do WORK• Units are Joules (J) = kg.m2/s2
(from KE=1/2mv2)
Work done on a system - system gains energy (w +ve)Work done by the system - system loses energy (w -ve)Heat absorbed by the system (endothermic) - system gains energy (q +ve)Heat released by the system (exothermic) - system loses energy (q +ve)
SYSTEM TOTAL ENERGY (kinetic plus potential) is the INTERNAL ENERGY (U sometimes E)
Usually measure CHANGE in internal energy ( U )U=Ufinal – Uinitial
U is a STATE FUNCTION (independent of path)
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1st LAW of ThermodynamicsInternal energy of an isolated system is constant
(energy can neither be created nor destroyed)
U = q+w
Pressure-Volume work
Against constant external pressure
w = -F.dz but Pex=F/A therefore w= -Pex.dV
Free expansion
w = 0
Calorimetry
Can measure internal energy changes in a “bomb” calorimeter
U=q-P V, but in a constant volume “bomb”, V=0
Thus U=q
Heat Capacity
Amount of energy required to raise the temperature of a substance by 1C (extensive property)
For 1 mol of substance: molar heat capacity (intensive property)
For 1g of substance: specific heat capacity (intensive property)
VV
VV
qTCU
T
UC
If heat capacity is independent of Temperature over the range of interest
Most reactions we investigate occur under conditions of constant PRESSURE (not Volume)
EnthalpyHeat of reaction at constant pressure!
PqH
VPbut
VPUH
PVUH
- w
Use a “coffee-cup” calorimeter
to measure it
PP
PP
qTCH
T
HC
Heat capacity
Excercise: When 50mL of 1M HCl is mixed with 50mL of 1M NaOH in a coffee-cup calorimeter, the temperature increases from 21oC to 27.5oC. What is the enthalpy change, if the density is 1g/mL and specific heat 4.18 J/g.K?
Problem: Heat Capacities & Temperature ChangesHow much heat is required to raise the temperature of 10 g of water and 10g of lead from 0 to 50oC?specific heat of H2O = 4.18 J/g-oCspecific heat of Pb = 0.128 J/g-oC
Problem: Heats of Chemical Reaction100 ml solutions of 1.00 M NaCl and 1.00 M AgNO3 at 22.4 oC are mixed in coffee cup calorimeter and the resulting temperature rises to 30.2 oC.What is the heat per mole of product? Assume the solution density and specific heat
are the same as pure water.Write balanced chemical reaction:Net ionic: Ag+(aq) + Cl-(aq) → AgCl(s)Determine heat of reaction:qrxn= -qcal = -m×c×∆T
m = 200 ml × 1.0g/ml = 200gc = cH2O = 4.18 J/g-oC
= -200g × 4.18 J/g-oC × (30.2-22.4)= -6,520 JDetermine heat per mole of product:stoichiometric reactants, 0.1 mol in 100 mlqrxn/mol = -6.52 kJ/0.1 mol= -65.2 kJ/mol
Hess’s LawHess‘s Law is particularly useful for calculating fHo which would not be easy to measure experimentally. fHo for CO cannot be measured
as CO2 is also formed when graphite is burned
C(s) + 1/2O2 CO fHo = x
CO + 1/2O2 CO2 rxnHo = -283 kJmol-1
_______________________________________
C(s) + O2 CO2 fHo = -393.5 kJmol-1
From looking at these equations it is fairly obvious that the sum of the first two enthalpies is equal to the third by Hess‘s Law.
i.e. x - 283 = -393.5 or x = -110.5 kJmol-1.
1/2H2(g)
Enthalpy Changes and Bond Energies
Energy is absorbed when bonds break. The energy required to break the bonds is absorbed from the surroundings.
If there was some way to figure out how much energy a single bond absorbed when broken, the enthalpy of reaction could be estimated by subtracting the bond energies for bonds formed from the total bond energies for bonds broken.
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
We can estimate the bond enthalpies of O=O, H-H, and O-H as 490.4 kJ/mol, 431.2 kJ/mol, and 457.7 kJ/mol, respectively.
2H2(g) + O2(g) 2H2O(g) H°= ?
2H2(g) + O2(g) 2H2O(g)
moles of bonds broken
Energy absorbedmoles of bonds formed Energy released
2 H-H @ 431.2 kJ each 862.4kJ 4 O-H @ 457.7 kJ each 1830.9kJ
1 O=O @ 490.4 kJ each 490.4kJ_____________________________________________
1352.7kJ 1830.9kJ
H°= 1352.7 - 1830.9 kJ = -478.2 kJ.
(Remember that the minus sign means "energy released", so you add the bond energies for broken bonds and subtract energies for bonds formed to get the total energy.)
A calculation based on enthalpies of formation gave H° = -483.7 kJ
Bonds in a molecule influence each other, which means that bond energies aren't really additive. An O-H bond in a water molecule has a slightly different energy than an O-H bond in H2O2,
because it's in a slightly different environment.
Reaction enthalpies calculated from bond energies are very rough approximations!
Foods and FuelsEnthalpies (heats) of combustion: complete reaction of compounds
with oxygen. Measure using a bomb calorimeter.Most chemical reactions used for the production of heat are
combustion reactions. The energy released when 1g of material is combusted is its Fuel Value. Since all heats of combustion are exothermic, fuel values are reported as positive.
Most of the energy our body needs comes from fats and carbohydrates. Carbohydrates are broken down in the intestines to glucose. Glucose is transported in the blood to cells where it is oxidized to produce CO2, H2O and energy:
C6H12O6(s) + 6O2(g) 6CO2(g) + 6H2O(l) H°rxn=-2816 kJThe breakdown of fats also produces CO2 and H2O
Any excess energy in the body is stored as fats
CompoundFuel Value (kJ/gram)
Fats 38
Carbohydrates
17
Proteins 17
About 100 kJ per kilogram of body weight per day is required to keep the body functioning at a minimum level
Fuels
The greater the percentage of carbon and hydrogen in the fuel the higher the fuel value
FuelC
(%)H
(%)O
(%)
Fuel Value (kJ/g)
Wood 50 6 44 18
Coal 77 5 7 32
Petrol 85 15 0 48
Hydrogen 0 100 0 142
Energy comes primarily from the combustion of fossil fuels Coal represents 90% of the fossil fuels on earth. However, it typically contains sulfur, which when combusted can lead to environmental pollution (acid rain)Solar energy: on a clear day the sun's energy which strikes the earth equals 1kJ
per square meter per second. Hydrogen: clean burning (produces only water) and high fuel value. Hydrogen
can be made from coal as well as methane C(coal) + H2O(g) CO(g)+H2(g)
CH4(g) + H2O(g) CO(g) + 3H2(g)
Fuel cells
• Biofuel cell research in NUIG• Biomednano website• Combustion chemistry