chpt1 11
DESCRIPTION
TRANSCRIPT
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chemistry
In this science we study matter and the changes it undergoes.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Matter
We define matter as anything that has mass and takes up space.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Matter
• Atoms are the building blocks of matter.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Matter
• Atoms are the building blocks of matter.• Each element is made of the same kind of atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Matter
• Atoms are the building blocks of matter.• Each element is made of the same kind of atom.• A compound is made of two or more different kinds of
elements.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
States of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Classification of Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Properties and Changes of
Matter
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Types of Properties
• Physical Properties…– Can be observed without changing a
substance into another substance.• Boiling point, density, mass, volume, etc.
• Chemical Properties…– Can only be observed when a substance is
changed into another substance.• Flammability, corrosiveness, reactivity with
acid, etc.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Types of Properties
• Intensive Properties…– Are independent of the amount of the
substance that is present.• Density, boiling point, color, etc.
• Extensive Properties…– Depend upon the amount of the substance
present.• Mass, volume, energy, etc.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Types of Changes
• Physical Changes– These are changes in matter that do not
change the composition of a substance.• Changes of state, temperature, volume, etc.
• Chemical Changes– Chemical changes result in new substances.
• Combustion, oxidation, decomposition, etc.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chemical Reactions
In the course of a chemical reaction, the reacting substances are converted to new substances.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Compounds
Compounds can be broken down into more elemental particles.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Separation of Mixtures
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Filtration
In filtration solid substances are separated from liquids and solutions.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Distillation
Distillation uses differences in the boiling points of substances to separate a homogeneous mixture into its components.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chromatography
This technique separates substances on the basis of differences in solubility in a solvent.
MatterAnd
Measurement
What do these countries have in common?
US, Liberia and Burma
© 2009, Prentice-Hall, Inc.
MatterAnd
Measurement
What do these countries have in common?
US, Liberia and Burma
• They use the imperial system
© 2009, Prentice-Hall, Inc.
MatterAnd
Measurement
View of Countries using Metric
© 2009, Prentice-Hall, Inc.
LiberiaBerma
USA
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Units of Measurement
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
SI Units
• Système International d’Unités• A different base unit is used for each quantity.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metric System
Prefixes convert the base units into units that are appropriate for the item being measured.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Volume
• The most commonly used metric units for volume are the liter (L) and the milliliter (mL).– A liter is a cube 1 dm
long on each side.– A milliliter is a cube 1 cm
long on each side.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Uncertainty in Measurement
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Uncertainty in Measurements
Different measuring devices have different uses and different degrees of accuracy.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Uncertainty in Measurements
Different measuring devices have different uses and different degrees of accuracy.
1 ml
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Uncertainty in Measurements
Different measuring devices have different uses and different degrees of accuracy.
0.1 ml
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Accuracy versus Precision
• Accuracy refers to the proximity of a measurement to the true value of a quantity.
• Precision refers to the proximity of several measurements to each other.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Significant Figures
• The term significant figures refers to digits that were measured.
• When rounding calculated numbers, we pay attention to significant figures so we do not overstate the accuracy of our answers.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Significant Figures
1. All nonzero digits are significant.
2. Zeroes between two significant figures are themselves significant.
3. Zeroes at the beginning of a number are never significant.
4. Zeroes at the end of a number are significant if a decimal point is written in the number.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Significant Figures
• When addition or subtraction is performed, answers are rounded to the least significant decimal place.
• When multiplication or division is performed, answers are rounded to the number of digits that corresponds to the least number of significant figures in any of the numbers used in the calculation.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Temperature
By definition temperature is a measure of the average kinetic energy of the particles in a sample.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Temperature• In scientific
measurements, the Celsius and Kelvin scales are most often used.
• The Celsius scale is based on the properties of water.– 0C is the freezing point
of water.– 100C is the boiling point
of water.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Temperature
• The Kelvin is the SI unit of temperature.
• It is based on the properties of gases.
• There are no negative Kelvin temperatures.
• K = C + 273.15
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Temperature
• The Fahrenheit scale is not used in scientific measurements.
F = 9/5(C) + 32 C = 5/9(F − 32)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Density
Density is a physical property of a substance.
d =mV
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dimensional Analysis
• We use dimensional analysis to convert one quantity to another.
• Most commonly dimensional analysis utilizes conversion factors (e.g., 1 in. = 2.54 cm)
1 in.
2.54 cm
2.54 cm
1 in.or
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dimensional Analysis
Use the form of the conversion factor that puts the sought-for unit in the numerator.
Given unit desired unitdesired unit
given unit
Conversion factor
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dimensional Analysis
• For example, to convert 8.00 m to inches,– convert m to cm– convert cm to in.
8.00 m100 cm
1 m
1 in.
2.54 cm 315 in.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Atomic Theory of Matter
The theory that atoms are the fundamental building blocks of matter reemerged in the early 19th century, championed by John Dalton.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dalton's Postulates
Each element is composed of extremely small particles called atoms.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dalton's Postulates
All atoms of a given element are identical to one another in mass (?) and other properties, but the atoms of one element are different from the atoms of all other elements.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dalton's Postulates
Atoms of an element are not changed into atoms of a different element by chemical reactions; atoms are neither created nor destroyed in chemical reactions.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dalton’s Postulates
Compounds are formed when atoms of more than one element combine; a given compound always has the same relative number and kind of atoms.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Law of Constant CompositionJoseph Proust (1754–1826)
• This is also known as the law of definite proportions.
• It states that the elemental composition of a pure substance never varies.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Law of Conservation of Mass
The total mass of substances present at the end of a chemical process is the same as the mass of substances present before the process took place.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Electron
• Streams of negatively charged particles were found to emanate from cathode tubes.
• J. J. Thompson is credited with their discovery (1897).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Electron
Thompson measured the charge/mass ratio of the electron to be 1.76 108 coulombs/g.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Millikan Oil Drop Experiment
Once the charge/mass ratio of the electron was known, determination of either the charge or the mass of an electron would yield the other.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Millikan Oil Drop Experiment
Robert Millikan (University of Chicago) determined the charge on the electron in 1909.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Radioactivity
• Radioactivity is the spontaneous emission of radiation by an atom.
• It was first observed by Henri Becquerel.
• Marie and Pierre Curie also studied it.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Radioactivity• Three types of radiation were discovered by
Ernest Rutherford: particles particles rays
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Atom, circa 1900
• The prevailing theory was that of the “plum pudding” model, put forward by Thompson.
• It featured a positive sphere of matter with negative electrons imbedded in it.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Discovery of the Nucleus
Ernest Rutherford shot particles at a thin sheet of gold foil and observed the pattern of scatter of the particles.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nuclear Atom
Since some particles were deflected at large angles, Thompson’s model could not be correct.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nuclear Atom• Rutherford postulated a very small,
dense nucleus with the electrons around the outside of the atom.
• Most of the volume of the atom is empty space.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Other Subatomic Particles
• Protons were discovered by Rutherford in 1919.
• Neutrons were discovered by James Chadwick in 1932.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Subatomic Particles
• Protons and electrons are the only particles that have a charge.
• Protons and neutrons have essentially the same mass.
• The mass of an electron is so small we ignore it.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Symbols of Elements
Elements are symbolized by one or two letters.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Atomic Number
All atoms of the same element have the same number of protons:
The atomic number (Z)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Atomic Mass
The mass of an atom in atomic mass units (amu) is the total number of protons and neutrons in the atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Isotopes
• Isotopes are atoms of the same element with different masses.
• Isotopes have different numbers of neutrons.
116C
126C
136C
146C
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Atomic Mass
Atomic and molecular masses can be measured with great accuracy with a mass spectrometer.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Average Mass
• Because in the real world we use large amounts of atoms and molecules, we use average masses in calculations.
• Average mass is calculated from the isotopes of an element weighted by their relative abundances.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Periodic Table
• It is a systematic catalog of the elements.
• Elements are arranged in order of atomic number.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Periodicity
When one looks at the chemical properties of elements, one notices a repeating pattern of reactivities.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Periodic Table
• The rows on the periodic chart are periods.
• Columns are groups.• Elements in the same
group have similar chemical properties.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Groups
These five groups are known by their names.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Periodic Table
Nonmetals are on the right side of the periodic table (with the exception of H).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Periodic Table
Metalloids border the stair-step line (with the exception of Al, Po, and At).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Periodic Table
Metals are on the left side of the chart.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chemical FormulasThe subscript to the right of the symbol of an element tells the number of atoms of that element in one molecule of the compound.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chemical FormulasMolecular compounds are composed of molecules and almost always contain only nonmetals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Diatomic Molecules
These seven elements occur naturally as molecules containing two atoms.
MatterAnd
Measurement
Types of Formulas
• Empirical formulas give the lowest whole-number ratio of atoms of each element in a compound.
• Molecular formulas give the exact number of atoms of each element in a compound.
© 2009, Prentice-Hall, Inc.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Types of Formulas
• Structural formulas show the order in which atoms are bonded.
• Perspective drawings also show the three-dimensional array of atoms in a compound.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ions
• When atoms lose or gain electrons, they become ions.– Cations are positive and are formed by elements
on the left side of the periodic chart.– Anions are negative and are formed by elements
on the right side of the periodic chart.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ionic Bonds
Ionic compounds (such as NaCl) are generally formed between metals and nonmetals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Formulas
• Because compounds are electrically neutral, one can determine the formula of a compound this way:– The charge on the cation becomes the subscript
on the anion.– The charge on the anion becomes the subscript
on the cation.– If these subscripts are not in the lowest whole-
number ratio, divide them by the greatest common factor.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Common Cations
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Common Anions
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Inorganic Nomenclature
• Write the name of the cation.
• If the anion is an element, change its ending to -ide; if the anion is a polyatomic ion, simply write the name of the polyatomic ion.
• If the cation can have more than one possible charge, write the charge as a Roman numeral in parentheses.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Patterns in Oxyanion Nomenclature
• When there are two oxyanions involving the same element:– The one with fewer oxygens ends in -ite.
• NO2− : nitrite; SO3
2− : sulfite
– The one with more oxygens ends in -ate.• NO3
− : nitrate; SO42− : sulfate
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Patterns in Oxyanion Nomenclature
• The one with the second fewest oxygens ends in -ite.– ClO2
− : chlorite
• The one with the second most oxygens ends in -ate.– ClO3
− : chlorate
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Patterns in Oxyanion Nomenclature
• The one with the fewest oxygens has the prefix hypo- and ends in -ite.
– ClO− : hypochlorite
• The one with the most oxygens has the prefix per- and ends in -ate.
– ClO4− : perchlorate
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Acid Nomenclature
• If the anion in the acid ends in -ide, change the ending to -ic acid and add the prefix hydro- .– HCl: hydrochloric acid– HBr: hydrobromic acid– HI: hydroiodic acid
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Acid Nomenclature
• If the anion in the acid ends in -ite, change the ending to -ous acid.– HClO: hypochlorous
acid
– HClO2: chlorous acid
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Acid Nomenclature
• If the anion in the acid ends in -ate, change the ending to -ic acid.– HClO3: chloric acid
– HClO4: perchloric acid
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nomenclature of Binary Compounds
• The less electronegative atom is usually listed first.
• A prefix is used to denote the number of atoms of each element in the compound (mono- is not used on the first element listed, however) .
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nomenclature of Binary Compounds
• The ending on the more electronegative element is changed to -ide.
– CO2: carbon dioxide– CCl4: carbon tetrachloride
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nomenclature of Binary Compounds
• If the prefix ends with a or o and the name of the element begins with a vowel, the two successive vowels are often elided into one.
N2O5: dinitrogen pentoxide
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nomenclature of Organic Compounds
• Organic chemistry is the study of carbon.• Organic chemistry has its own system of
nomenclature.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nomenclature of Organic Compounds
The simplest hydrocarbons (compounds containing only carbon and hydrogen) are alkanes.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nomenclature of Organic Compounds
The first part of the names above correspond to the number of carbons (meth- = 1, eth- = 2, prop- = 3, etc.).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nomenclature of Organic Compounds
• When a hydrogen in an alkane is replaced with something else (a functional group, like -OH in the compounds above), the name is derived from the name of the alkane.
• The ending denotes the type of compound.– An alcohol ends in -ol.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Law of Conservation of Mass“We may lay it down as an
incontestable axiom that, in all the operations of art and nature,
nothing is created; an equal amount of matter exists both
before and after the experiment. Upon this principle, the whole art
of performing chemical experiments depends.”
--Antoine Lavoisier, 1789
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chemical Equations
Chemical equations are concise representations of chemical reactions.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Anatomy of a Chemical Equation
CH4 (g) + 2 O2 (g) CO2 (g) + 2 H2O (g)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Anatomy of a Chemical Equation
Reactants appear on the left side of the equation.
CH4 (g) + 2 O2 (g) CO2 (g) + 2 H2O (g)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Anatomy of a Chemical Equation
Products appear on the right side of the equation.
CH4 (g) + 2 O2 (g) CO2 (g) + 2 H2O (g)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Anatomy of a Chemical Equation
The states of the reactants and products are written in parentheses to the right of each compound.
CH4 (g) + 2 O2 (g) CO2 (g) + 2 H2O (g)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Anatomy of a Chemical Equation
Coefficients are inserted to balance the equation.
CH4 (g) + 2 O2 (g) CO2 (g) + 2 H2O (g)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Subscripts and Coefficients Give Different Information
• Subscripts tell the number of atoms of each element in a molecule.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Subscripts and Coefficients Give Different Information
• Subscripts tell the number of atoms of each element in a molecule
• Coefficients tell the number of molecules.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Reaction Types
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Combination Reactions
• Examples:– 2 Mg (s) + O2 (g) 2 MgO (s)
– N2 (g) + 3 H2 (g) 2 NH3 (g)
– C3H6 (g) + Br2 (l) C3H6Br2 (l)
• In this type of reaction two or more substances react to form one product.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
• In a decomposition one substance breaks down into two or more substances.
Decomposition Reactions
• Examples:– CaCO3 (s) CaO (s) + CO2 (g)
– 2 KClO3 (s) 2 KCl (s) + O2 (g)
– 2 NaN3 (s) 2 Na (s) + 3 N2 (g)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Combustion Reactions
• Examples:– CH4 (g) + 2 O2 (g) CO2 (g) + 2 H2O (g)
– C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (g)
• These are generally rapid reactions that produce a flame.
• Most often involve hydrocarbons reacting with oxygen in the air.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Formula Weights
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Formula Weight (FW)• A formula weight is the sum of the
atomic weights for the atoms in a chemical formula.
• So, the formula weight of calcium chloride, CaCl2, would be
Ca: 1(40.1 amu)
+ Cl: 2(35.5 amu)
111.1 amu
• Formula weights are generally reported for ionic compounds.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Weight (MW)
• A molecular weight is the sum of the atomic weights of the atoms in a molecule.
• For the molecule ethane, C2H6, the molecular weight would be
C: 2(12.0 amu)
30.0 amu+ H: 6(1.0 amu)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Percent Composition
One can find the percentage of the mass of a compound that comes from each of the elements in the compound by using this equation:
% element =(number of atoms)(atomic weight)
(FW of the compound)x 100
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Percent Composition
So the percentage of carbon in ethane is…
%C =(2)(12.0 amu)
(30.0 amu)
24.0 amu
30.0 amu= x 100
= 80.0%
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Moles
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Avogadro’s Number
• 6.02 x 1023
• 1 mole of 12C has a mass of 12 g.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molar Mass
• By definition, a molar mass is the mass of 1 mol of a substance (i.e., g/mol).– The molar mass of an element is the mass
number for the element that we find on the periodic table.
– The formula weight (in amu’s) will be the same number as the molar mass (in g/mol).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Using Moles
Moles provide a bridge from the molecular scale to the real-world scale.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Mole Relationships
• One mole of atoms, ions, or molecules contains Avogadro’s number of those particles.
• One mole of molecules or formula units contains Avogadro’s number times the number of atoms or ions of each element in the compound.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Finding Empirical Formulas
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculating Empirical Formulas
One can calculate the empirical formula from the percent composition.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculating Empirical Formulas
The compound para-aminobenzoic acid (you may have seen it listed as PABA on your bottle of sunscreen) is composed of carbon (61.31%), hydrogen (5.14%), nitrogen (10.21%), and oxygen (23.33%). Find the empirical formula of PABA.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculating Empirical Formulas
Assuming 100.00 g of para-aminobenzoic acid,
C: 61.31 g x = 5.105 mol C
H: 5.14 g x = 5.09 mol H
N: 10.21 g x = 0.7288 mol N
O: 23.33 g x = 1.456 mol O
1 mol12.01 g
1 mol14.01 g
1 mol1.01 g
1 mol16.00 g
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculating Empirical Formulas
Calculate the mole ratio by dividing by the smallest number of moles:
C: = 7.005 7
H: = 6.984 7
N: = 1.000
O: = 2.001 2
5.105 mol0.7288 mol
5.09 mol0.7288 mol
0.7288 mol0.7288 mol
1.458 mol0.7288 mol
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculating Empirical Formulas
These are the subscripts for the empirical formula:
C7H7NO2
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Combustion Analysis
• Compounds containing C, H and O are routinely analyzed through combustion in a chamber like this.– C is determined from the mass of CO2 produced.
– H is determined from the mass of H2O produced.
– O is determined by difference after the C and H have been determined.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Elemental Analyses
Compounds containing other elements are analyzed using methods analogous to those used for C, H and O.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Stoichiometric Calculations
The coefficients in the balanced equation give the ratio of moles of reactants and products.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Stoichiometric Calculations
Starting with the mass of Substance A you can use the ratio of the coefficients of A and B to calculate the mass of Substance B formed (if it’s a product) or used (if it’s a reactant).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Stoichiometric Calculations
Starting with 1.00 g of C6H12O6… we calculate the moles of C6H12O6…use the coefficients to find the moles of H2O…and then turn the moles of water to grams.
C6H12O6 + 6 O2 6 CO2 + 6 H2O
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Limiting Reactants
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
How Many Cookies Can I Make?
• You can make cookies until you run out of one of the ingredients.
• Once this family runs out of sugar, they will stop making cookies (at least any cookies you would want to eat).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
How Many Cookies Can I Make?
• In this example the sugar would be the limiting reactant, because it will limit the amount of cookies you can make.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Limiting Reactants
• The limiting reactant is the reactant present in the smallest stoichiometric amount.– In other words, it’s the reactant you’ll run out of first (in
this case, the H2).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Limiting Reactants
In the example below, the O2 would be the excess reagent.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Theoretical Yield
• The theoretical yield is the maximum amount of product that can be made.– In other words it’s the amount of product
possible as calculated through the stoichiometry problem.
• This is different from the actual yield, which is the amount one actually produces and measures.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Percent Yield
One finds the percent yield by comparing the amount actually obtained (actual yield) to the amount it was possible to make (theoretical yield).
Actual YieldTheoretical YieldPercent Yield = x 100
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Solutions
• Solutions are defined as homogeneous mixtures of two or more pure substances.
• The solvent is present in greatest abundance.
• All other substances are solutes.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dissociation
• When an ionic substance dissolves in water, the solvent pulls the individual ions from the crystal and solvates them.
• This process is called dissociation.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dissociation
• An electrolyte is a substances that dissociates into ions when dissolved in water.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electrolytes
• An electrolyte is a substances that dissociates into ions when dissolved in water.
• A nonelectrolyte may dissolve in water, but it does not dissociate into ions when it does so.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electrolytes and Nonelectrolytes
Soluble ionic compounds tend to be electrolytes.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electrolytes and Nonelectrolytes
Molecular compounds tend to be nonelectrolytes, except for acids and bases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electrolytes
• A strong electrolyte dissociates completely when dissolved in water.
• A weak electrolyte only dissociates partially when dissolved in water.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Strong Electrolytes Are…
• Strong acids• Strong bases
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Strong Electrolytes Are…
• Strong acids• Strong bases• Soluble ionic salts
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Precipitation Reactions
When one mixes ions that form compounds that are insoluble (as could be predicted by the solubility guidelines), a precipitate is formed.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metathesis (Exchange) Reactions• Metathesis comes from a Greek word that
means “to transpose.”
AgNO3 (aq) + KCl (aq) AgCl (s) + KNO3 (aq)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metathesis (Exchange) Reactions• Metathesis comes from a Greek word that
means “to transpose.”• It appears the ions in the reactant
compounds exchange, or transpose, ions.
AgNO3 (aq) + KCl (aq) AgCl (s) + KNO3 (aq)
MatterAnd
Measurement
Cl- Br- I- NO3- SO4
2- CO32- PO4
3-
Li+ S S S S S S S S
Na+ S S S S S S S S
K+ S S S S S S S S
Mg2+ NS S S S S S NS NS
Ca2+ S S S S S S NS NS
Sr2+ S S S S S NS NS NS
Ba2+ S S S S S NS NS NS
Fe2+ NS S S S S S NS NS
Fe3+ NS S S S S S NS NS
Ni2+ NS S S S S S NS NS
Cu+ NS S S S S S NS NS
Cu2+ NS S S S S S NS NS
Al3+ NS S S S S S NS NS
Zn2+ NS S S S S S NS NS
Ag+ NS NS NS NS S S NS NS
Pb2+ NS NS NS NS S NS NS NS
Solubility of different compounds(NS = non soluble in water, S = soluble in water)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Solution Chemistry
• It is helpful to pay attention to exactly what species are present in a reaction mixture (i.e., solid, liquid, gas, aqueous solution).
• If we are to understand reactivity, we must be aware of just what is changing during the course of a reaction.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Equation
The molecular equation lists the reactants and products in their molecular form.
AgNO3 (aq) + KCl (aq) AgCl (s) + KNO3 (aq)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ionic Equation• In the ionic equation all strong electrolytes (strong
acids, strong bases, and soluble ionic salts) are dissociated into their ions.
• This more accurately reflects the species that are found in the reaction mixture.
Ag+ (aq) + NO3- (aq) + K+ (aq) + Cl- (aq)
AgCl (s) + K+ (aq) + NO3- (aq)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Net Ionic Equation• To form the net ionic equation, cross out anything
that does not change from the left side of the equation to the right.
Ag+(aq) + NO3-(aq) + K+(aq) + Cl-(aq)
AgCl (s) + K+(aq) + NO3-(aq)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Net Ionic Equation• To form the net ionic equation, cross out anything
that does not change from the left side of the equation to the right.
• The only things left in the equation are those things that change (i.e., react) during the course of the reaction.
Ag+(aq) + Cl-(aq) AgCl (s)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Net Ionic Equation• To form the net ionic equation, cross out anything
that does not change from the left side of the equation to the right.
• The only things left in the equation are those things that change (i.e., react) during the course of the reaction.
• Those things that didn’t change (and were deleted from the net ionic equation) are called spectator ions.
Ag+(aq) + NO3-(aq) + K+(aq) + Cl-(aq)
AgCl (s) + K+(aq) + NO3-(aq)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Net Ionic Equations
1. Write a balanced molecular equation.
2. Dissociate all strong electrolytes.
3. Cross out anything that remains unchanged from the left side to the right side of the equation.
4. Write the net ionic equation with the species that remain.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Acids
• Arrhenius defined acids as substances that increase the concentration of H+ when dissolved in water.
• Brønsted and Lowry defined them as proton donors.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Acids
There are only seven strong acids:• Hydrochloric (HCl)• Hydrobromic (HBr)• Hydroiodic (HI)
• Nitric (HNO3)
• Sulfuric (H2SO4)
• Chloric (HClO3)
• Perchloric (HClO4)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Bases• Arrhenius defined bases
as substances that increase the concentration of OH− when dissolved in water.
• Brønsted and Lowry defined them as proton acceptors.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Bases
The strong bases are the soluble metal salts of hydroxide ion:• Alkali metals• Calcium• Strontium• Barium
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Acid-Base Reactions
In an acid-base reaction, the acid donates a proton (H+) to the base.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Neutralization ReactionsGenerally, when solutions of an acid and a base are combined, the products are a salt and water.
CH3COOH (aq) + NaOH (aq) CH3COONa (aq) + H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Neutralization ReactionsWhen a strong acid reacts with a strong base, the net ionic equation is…
HCl (aq) + NaOH (aq) NaCl (aq) + H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Neutralization ReactionsWhen a strong acid reacts with a strong base, the net ionic equation is…
HCl (aq) + NaOH (aq) NaCl (aq) + H2O (l)
H+ (aq) + Cl- (aq) + Na+ (aq) + OH-(aq)
Na+ (aq) + Cl- (aq) + H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Neutralization ReactionsWhen a strong acid reacts with a strong base, the net ionic equation is…
HCl (aq) + NaOH (aq) NaCl (aq) + H2O (l)
H+ (aq) + Cl- (aq) + Na+ (aq) + OH-(aq)
Na+ (aq) + Cl- (aq) + H2O (l)
H+ (aq) + OH- (aq) H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Gas-Forming Reactions
• Some metathesis reactions do not give the product expected.
• In this reaction, the expected product (H2CO3) decomposes to give a gaseous product (CO2).
CaCO3 (s) + HCl (aq) CaCl2 (aq) + CO2 (g) + H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Gas-Forming Reactions
When a carbonate or bicarbonate reacts with an acid, the products are a salt, carbon dioxide, and water.
CaCO3 (s) + HCl (aq) CaCl2 (aq) + CO2 (g) + H2O (l)
NaHCO3 (aq) + HBr (aq) NaBr (aq) + CO2 (g) + H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Gas-Forming Reactions
Similarly, when a sulfite reacts with an acid, the products are a salt, sulfur dioxide, and water.
SrSO3 (s) + 2 HI (aq) SrI2 (aq) + SO2 (g) + H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Gas-Forming Reactions
• This reaction gives the predicted product, but you had better carry it out in the hood, or you will be very unpopular!
• But just as in the previous examples, a gas is formed as a product of this reaction.
Na2S (aq) + H2SO4 (aq) Na2SO4 (aq) + H2S (g)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Oxidation-Reduction Reactions
• An oxidation occurs when an atom or ion loses electrons.
• A reduction occurs when an atom or ion gains electrons.
• One cannot occur without the other.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Oxidation Numbers
To determine if an oxidation-reduction reaction has occurred, we assign an oxidation number to each element in a neutral compound or charged entity.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Oxidation Numbers
• Elements in their elemental form have an oxidation number of 0.
• The oxidation number of a monatomic ion is the same as its charge.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Oxidation Numbers
• Nonmetals tend to have negative oxidation numbers, although some are positive in certain compounds or ions.Oxygen has an oxidation number of −2,
except in the peroxide ion in which it has an oxidation number of −1.
Hydrogen is −1 when bonded to a metal, +1 when bonded to a nonmetal.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Oxidation Numbers
• Nonmetals tend to have negative oxidation numbers, although some are positive in certain compounds or ions.Fluorine always has an oxidation number
of −1.The other halogens have an oxidation
number of −1 when they are negative; they can have positive oxidation numbers, however, most notably in oxyanions.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Oxidation Numbers
• The sum of the oxidation numbers in a neutral compound is 0.
• The sum of the oxidation numbers in a polyatomic ion is the charge on the ion.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Displacement Reactions
• In displacement reactions, ions oxidize an element.
• The ions, then, are reduced.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Displacement Reactions
In this reaction,
silver ions oxidize
copper metal.
Cu (s) + 2 Ag+ (aq) Cu2+ (aq) + 2 Ag (s)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Displacement Reactions
The reverse reaction,
however, does not
occur.
Cu2+ (aq) + 2 Ag (s) Cu (s) + 2 Ag+ (aq) x
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Activity Series
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molarity• Two solutions can contain the same
compounds but be quite different because the proportions of those compounds are different.
• Molarity is one way to measure the concentration of a solution.
moles of solute
volume of solution in litersMolarity (M) =
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Mixing a Solution
• To create a solution of a known molarity, one weighs out a known mass (and, therefore, number of moles) of the solute.
• The solute is added to a volumetric flask, and solvent is added to the line on the neck of the flask.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dilution• One can also dilute a more concentrated
solution by– Using a pipet to deliver a volume of the solution to
a new volumetric flask, and– Adding solvent to the line on the neck of the new
flask.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
DilutionThe molarity of the new solution can be determined from the equation
Mc Vc = Md Vd,
where Mc and Md are the molarity of the concentrated and dilute solutions, respectively, and Vc and Vd are the volumes of the two solutions.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Using Molarities inStoichiometric Calculations
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Titration
Titration is an analytical technique in which one can calculate the concentration of a solute in a solution.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chapter 5Thermochemistry
John D. BookstaverSt. Charles Community College
Cottleville, MO
Chemistry, The Central Science, 11th editionTheodore L. Brown; H. Eugene LeMay, Jr.;
and Bruce E. Bursten
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energy
• Energy is the ability to do work or transfer heat.– Energy used to cause an object that has
mass to move is called work.– Energy used to cause the temperature of
an object to rise is called heat.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Potential Energy
Potential energy is energy an object possesses by virtue of its position or chemical composition.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Kinetic Energy
Kinetic energy is energy an object possesses by virtue of its motion.
12
KE = mv2
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Units of Energy
• The SI unit of energy is the joule (J).
• An older, non-SI unit is still in widespread use: the calorie (cal).
1 cal = 4.184 J
1 J = 1 kg m2
s2
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Definitions:System and Surroundings
• The system includes the molecules we want to study (here, the hydrogen and oxygen molecules).
• The surroundings are everything else (here, the cylinder and piston).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Definitions: Work
• Energy used to move an object over some distance is work.
• w = F dwhere w is work, F is the force, and d is the distance over which the force is exerted.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Heat
• Energy can also be transferred as heat.
• Heat flows from warmer objects to cooler objects.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Conversion of Energy
• Energy can be converted from one type to another.
• For example, the cyclist above has potential energy as she sits on top of the hill.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Conversion of Energy
• As she coasts down the hill, her potential energy is converted to kinetic energy.
• At the bottom, all the potential energy she had at the top of the hill is now kinetic energy.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
First Law of Thermodynamics• Energy is neither created nor destroyed.• In other words, the total energy of the universe is
a constant; if the system loses energy, it must be gained by the surroundings, and vice versa.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Internal EnergyThe internal energy of a system is the sum of all kinetic and potential energies of all components of the system; we call it E.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Internal EnergyBy definition, the change in internal energy, E, is the final energy of the system minus the initial energy of the system:
E = Efinal − Einitial
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Changes in Internal Energy
• If E > 0, Efinal > Einitial
– Therefore, the system absorbed energy from the surroundings.
– This energy change is called endergonic.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Changes in Internal Energy
• If E < 0, Efinal < Einitial
– Therefore, the system released energy to the surroundings.
– This energy change is called exergonic.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Changes in Internal Energy
• When energy is exchanged between the system and the surroundings, it is exchanged as either heat (q) or work (w).
• That is, E = q + w.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
E, q, w, and Their Signs
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Exchange of Heat between System and Surroundings
• When heat is absorbed by the system from the surroundings, the process is endothermic.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Exchange of Heat between System and Surroundings
• When heat is absorbed by the system from the surroundings, the process is endothermic.
• When heat is released by the system into the surroundings, the process is exothermic.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
State Functions
Usually we have no way of knowing the internal energy of a system; finding that value is simply too complex a problem.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
State Functions• However, we do know that the internal energy
of a system is independent of the path by which the system achieved that state.– In the system below, the water could have reached
room temperature from either direction.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
State Functions• Therefore, internal energy is a state function.• It depends only on the present state of the
system, not on the path by which the system arrived at that state.
• And so, E depends only on Einitial and Efinal.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
State Functions
• However, q and w are not state functions.
• Whether the battery is shorted out or is discharged by running the fan, its E is the same.– But q and w are different
in the two cases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Work
Usually in an open container the only work done is by a gas pushing on the surroundings (or by the surroundings pushing on the gas).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
WorkWe can measure the work done by the gas if the reaction is done in a vessel that has been fitted with a piston.
w = -PV
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpy
• If a process takes place at constant pressure (as the majority of processes we study do) and the only work done is this pressure-volume work, we can account for heat flow during the process by measuring the enthalpy of the system.
• Enthalpy is the internal energy plus the product of pressure and volume:
H = E + PV
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpy
• When the system changes at constant pressure, the change in enthalpy, H, is
H = (E + PV)
• This can be written
H = E + PV
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpy
• Since E = q + w and w = -PV, we can substitute these into the enthalpy expression:
H = E + PV
H = (q+w) − w
H = q
• So, at constant pressure, the change in enthalpy is the heat gained or lost.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Endothermicity and Exothermicity
• A process is endothermic when H is positive.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Endothermicity and Exothermicity
• A process is endothermic when H is positive.
• A process is exothermic when H is negative.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpy of Reaction
The change in enthalpy, H, is the enthalpy of the products minus the enthalpy of the reactants:
H = Hproducts − Hreactants
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpy of Reaction
This quantity, H, is called the enthalpy of reaction, or the heat of reaction.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Truth about Enthalpy
1. Enthalpy is an extensive property.
2. H for a reaction in the forward direction is equal in size, but opposite in sign, to H for the reverse reaction.
3. H for a reaction depends on the state of the products and the state of the reactants.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calorimetry
Since we cannot know the exact enthalpy of the reactants and products, we measure H through calorimetry, the measurement of heat flow.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Heat Capacity and Specific Heat
The amount of energy required to raise the temperature of a substance by 1 K (1C) is its heat capacity.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Heat Capacity and Specific Heat
We define specific heat capacity (or simply specific heat) as the amount of energy required to raise the temperature of 1 g of a substance by 1 K.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Heat Capacity and Specific Heat
Specific heat, then, is
Specific heat =heat transferred
mass temperature change
s =q
m T
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Constant Pressure Calorimetry
By carrying out a reaction in aqueous solution in a simple calorimeter such as this one, one can indirectly measure the heat change for the system by measuring the heat change for the water in the calorimeter.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Constant Pressure Calorimetry
Because the specific heat for water is well known (4.184 J/g-K), we can measure H for the reaction with this equation:
q = m s T
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Bomb Calorimetry
• Reactions can be carried out in a sealed “bomb” such as this one.
• The heat absorbed (or released) by the water is a very good approximation of the enthalpy change for the reaction.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Bomb Calorimetry
• Because the volume in the bomb calorimeter is constant, what is measured is really the change in internal energy, E, not H.
• For most reactions, the difference is very small.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpies of Formation
Enthalpy of formation, Hf, is ….
the enthalpy change for the reaction in which a compound is made from its constituent elements in their elemental forms.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hess's Law
If a reaction is carried out in a series of steps, H
for the overall reaction = the sum of the enthalpy changes for individual steps.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculation of H
• Imagine this as occurringin three steps:
C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)
C3H8 (g) 3 C (graphite) + 4 H2 (g)
3 C (graphite) + 3 O2 (g) 3 CO2 (g)
4 H2 (g) + 2 O2 (g) 4 H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculation of H
• Imagine this as occurringin three steps:
C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)
C3H8 (g) 3 C (graphite) + 4 H2 (g)
3 C (graphite) + 3 O2 (g) 3 CO2 (g)
4 H2 (g) + 2 O2 (g) 4 H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculation of H
• Imagine this as occurringin three steps:
C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)
C3H8 (g) 3 C (graphite) + 4 H2 (g)
3 C (graphite) + 3 O2 (g) 3 CO2 (g)
4 H2 (g) + 2 O2 (g) 4 H2O (l)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)
C3H8 (g) 3 C (graphite) + 4 H2 (g)
3 C (graphite) + 3 O2 (g) 3 CO2 (g)
4 H2 (g) + 2 O2 (g) 4 H2O (l)
C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)
Calculation of H
• The sum of these equations is:
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Calculation of H
We can use Hess’s law in this way:
H = nHf°products – mHf° reactants
where n and m are the stoichiometric coefficients.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
H = [3(-393.5 kJ) + 4(-285.8 kJ)] – [1(-103.85 kJ) + 5(0 kJ)]
= [(-1180.5 kJ) + (-1143.2 kJ)] – [(-103.85 kJ) + (0 kJ)]= (-2323.7 kJ) – (-103.85 kJ) = -2219.9 kJ
C3H8 (g) + 5 O2 (g) 3 CO2 (g) + 4 H2O (l)
Calculation of H
Hf of the most stable
Form of any element Is 0 ...no formationNeeded.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hess’s Law
H is well known for many reactions, and it is inconvenient to measure H for every reaction in which we are interested.
• However, we can estimate H using published H values and the properties of enthalpy.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hess’s Law
Hess’s law states that “[i]f a reaction is carried out in a series of steps, H for the overall reaction will be equal to the sum of the enthalpy changes for the individual steps.”
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hess’s Law
Because H is a state function, the total enthalpy change depends only on the initial state of the reactants and the final state of the products.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energy in FoodsMost of the fuel in the food we eat comes from carbohydrates and fats.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energy in Fuels
The vast majority of the energy consumed in this country comes from fossil fuels.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chapter 6Electronic Structureof Atoms
Chemistry, The Central Science, 11th editionTheodore L. Brown; H. Eugene LeMay, Jr.; and Bruce E. Bursten
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
• Why an object can glow when its temperature increases?
• The wave nature of light does not explain it
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Waves
• To understand the electronic structure of atoms, one must understand the nature of electromagnetic radiation.
• The distance between corresponding points on adjacent waves is the wavelength ().
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Waves
• The number of waves passing a given point per unit of time is the frequency ().
• For waves traveling at the same velocity, the longer the wavelength, the smaller the frequency.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electromagnetic Radiation
• All electromagnetic radiation travels at the same velocity: the speed of light (c), 3.00 108 m/s.
• Therefore,c =
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
Another mystery in the early 20th century involved the emission spectra observed from energy emitted by atoms and molecules.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
• For atoms and molecules one does not observe a continuous spectrum, as one gets from a white light source.
• Only a line spectrum of discrete wavelengths is observed.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
• Max Planck explained it by assuming that energy comes in packets called quanta.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
• Einstein used this assumption to explain the photoelectric effect.
• He concluded that energy is proportional to frequency:
E = hwhere h is Planck’s constant, 6.626 10−34 J-s.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
• Therefore, if one knows the wavelength of light, one can calculate the energy in one photon, or packet, of that light:
c = E = h
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
• Niels Bohr adopted Planck’s assumption and explained these phenomena in this way:1. Electrons in an atom can only
occupy certain orbits (corresponding to certain energies).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
• Niels Bohr adopted Planck’s assumption and explained these phenomena in this way:1. Electrons in permitted orbits
have specific, “allowed” energies; these energies will not be radiated from the atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
• Niels Bohr adopted Planck’s assumption and explained these phenomena in this way:1. Energy is only absorbed or
emitted in such a way as to move an electron from one “allowed” energy state to another; the energy is defined by
E = h
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Nature of Energy
The energy absorbed or emitted from the process of electron promotion or demotion can be calculated by the equation:
E = −hcRH ( )1nf
2
1ni
2-
where RH is the Rydberg constant, and ni and nf are the initial and final energy levels of the electron.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Wave Nature of Matter
• Louis de Broglie posited that if light can have material properties, matter should exhibit wave properties.
• He demonstrated that the relationship between mass and wavelength was
=hmv
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The Uncertainty Principle
• Heisenberg showed that the more precisely the momentum of a particle is known, the less precisely is its position known:
• In many cases, our uncertainty of the whereabouts of an electron is greater than the size of the atom itself!
(x) (mv) h4
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Quantum Mechanics
• Erwin Schrödinger developed a mathematical treatment into which both the wave and particle nature of matter could be incorporated.
• It is known as quantum mechanics.
MatterAnd
Measurement
Schrödinger equation
Time dependent form
Time independent form
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Quantum Mechanics
• The wave equation is designated with a lower case Greek psi ().
• The square of the wave equation, 2, gives a probability density map of where an electron has a certain statistical likelihood of being at any given instant in time.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Quantum Numbers
• Solving the wave equation gives a set of wave functions, or orbitals, and their corresponding energies.
• Each orbital describes a spatial distribution of electron density.
• An orbital is described by a set of three quantum numbers.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Principal Quantum Number (n)
• The principal quantum number, n, describes the energy level on which the orbital resides.
• The values of n are integers ≥ 1.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Angular Momentum Quantum Number (l)
• This quantum number defines the shape of the orbital.
• Allowed values of l are integers ranging from 0 to n − 1.
• We use letter designations to communicate the different values of l and, therefore, the shapes and types of orbitals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Angular Momentum Quantum Number (l)
Value of l 0 1 2 3
Type of orbital s p d f
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Magnetic Quantum Number (ml)
• The magnetic quantum number describes the three-dimensional orientation of the orbital.
• Allowed values of ml are integers ranging from -l to l:
−l ≤ ml ≤ l.• Therefore, on any given energy level,
there can be up to 1 s orbital, 3 p orbitals, 5 d orbitals, 7 f orbitals, etc.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Magnetic Quantum Number (ml)
• Orbitals with the same value of n form a shell.• Different orbital types within a shell are
subshells.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
s Orbitals
• The value of l for s orbitals is 0.
• They are spherical in shape.
• The radius of the sphere increases with the value of n.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
s Orbitals
Observing a graph of probabilities of finding an electron versus distance from the nucleus, we see that s orbitals possess n−1 nodes, or regions where there is 0 probability of finding an electron.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
p Orbitals
• The value of l for p orbitals is 1.• They have two lobes with a node between
them.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
d Orbitals
• The value of l for a d orbital is 2.
• Four of the five d orbitals have 4 lobes; the other resembles a p orbital with a doughnut around the center.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energies of Orbitals
• For a one-electron hydrogen atom, orbitals on the same energy level have the same energy.
• That is, they are degenerate.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energies of Orbitals
• As the number of electrons increases, though, so does the repulsion between them.
• Therefore, in many-electron atoms, orbitals on the same energy level are no longer degenerate.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Spin Quantum Number, ms
• In the 1920s, it was discovered that two electrons in the same orbital do not have exactly the same energy.
• The “spin” of an electron describes its magnetic field, which affects its energy.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Spin Quantum Number, ms
• This led to a fourth quantum number, the spin quantum number, ms.
• The spin quantum number has only 2 allowed values: +1/2 and −1/2.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Pauli Exclusion Principle
• No two electrons in the same atom can have exactly the same energy.
• Therefore, no two electrons in the same atom can have identical sets of quantum numbers.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electron Configurations
• This shows the distribution of all electrons in an atom.
• Each component consists of – A number denoting the
energy level,
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electron Configurations
• This shows the distribution of all electrons in an atom
• Each component consists of – A number denoting the
energy level,– A letter denoting the type
of orbital,
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electron Configurations
• This shows the distribution of all electrons in an atom.
• Each component consists of – A number denoting the
energy level,– A letter denoting the type
of orbital,– A superscript denoting
the number of electrons in those orbitals.
MatterAnd
Measurement
First Klechkovsky’s Rule
As atomic number increases, filling of orbitals in the atom goes from orbitals with the smaller sum of n and l (n+l) to orbitals with the larger sum of n and l (n+l).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Orbital Diagrams
• Each box in the diagram represents one orbital.
• Half-arrows represent the electrons.
• The direction of the arrow represents the relative spin of the electron.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hund’s Rule
“For degenerate orbitals, the lowest energy is attained when the number of electrons with the same spin is maximized.”
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Periodic Table
• We fill orbitals in increasing order of energy.
• Different blocks on the periodic table (shaded in different colors in this chart) correspond to different types of orbitals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Some Anomalies
For instance, the electron configuration for copper is
[Ar] 4s1 3d5
rather than the expected
[Ar] 4s2 3d4.
MatterAnd
Measurement
Second Klechkovsky’s Rule
When the sum of n and l (n+l) is identical, the filling of orbitals goes in the direction of rising of the main quantum number (n).
Exceptions: Cr, Cu, Nb, Mo, Ru, Rh, Pd, Ag, Pt, Au
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Some Anomalies
Some irregularities occur when there are enough electrons to half-fill s and d orbitals on a given row.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Some Anomalies
• This occurs because the 4s and 3d orbitals are very close in energy.
• These anomalies occur in f-block atoms, as well.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chapter 7Periodic Properties
of the Elements
Chemistry, The Central Science, 11th editionTheodore L. Brown; H. Eugene LeMay, Jr.;
and Bruce E. Bursten
John D. BookstaverSt. Charles Community College
Cottleville, MO
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Development of Periodic Table
• Elements in the same group generally have similar chemical properties.
• Physical properties are not necessarily similar, however.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Development of Periodic Table
Dmitri Mendeleev and Lothar Meyer independently came to the same conclusion about how elements should be grouped.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Development of Periodic Table
Mendeleev, for instance, predicted the discovery of germanium (which he called eka-silicon) as an element with an atomic weight between that of zinc and arsenic, but with chemical properties similar to those of silicon.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Periodic Trends
• In this chapter, we will rationalize observed trends in– Sizes of atoms and ions.– Ionization energy.– Electron affinity.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Effective Nuclear Charge
• In a many-electron atom, electrons are both attracted to the nucleus and repelled by other electrons.
• The nuclear charge that an electron experiences depends on both factors.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Effective Nuclear Charge
The effective nuclear charge, Zeff, is found this way:
Zeff = Z − S
where Z is the atomic number and S is a screening constant, usually close to the number of inner electrons.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Group
Other electrons in
the same group
Electrons in group(s) with principal quantum number n-1
Electrons in all group(s) with principal quantum number
< n-1
[1s] 0.3 N/A N/A
[ns,np] 0.35 0.85 1
[nd] or [nf] 0.35 1 1
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
What Is the Size of an Atom?
The bonding atomic radius is defined as one-half of the distance between covalently bonded nuclei.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Sizes of Atoms
Bonding atomic radius tends to… …decrease from left to
right across a row(due to increasing Zeff).
…increase from top to bottom of a column
(due to increasing value of n).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Sizes of Ions
• Ionic size depends upon:– The nuclear
charge.– The number of
electrons.– The orbitals in
which electrons reside.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Sizes of Ions
• Cations are smaller than their parent atoms.– The outermost
electron is removed and repulsions between electrons are reduced.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Sizes of Ions
• Anions are larger than their parent atoms.– Electrons are
added and repulsions between electrons are increased.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Sizes of Ions
• Ions increase in size as you go down a column.– This is due to
increasing value of n.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Sizes of Ions
• In an isoelectronic series, ions have the same number of electrons.
• Ionic size decreases with an increasing nuclear charge.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ionization Energy
• The ionization energy is the amount of energy required to remove an electron from the ground state of a gaseous atom or ion.– The first ionization energy is that energy
required to remove first electron.– The second ionization energy is that
energy required to remove second electron, etc.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ionization Energy• It requires more energy to remove each
successive electron.• When all valence electrons have been removed,
the ionization energy takes a quantum leap.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in First Ionization Energies
• As one goes down a column, less energy is required to remove the first electron.– For atoms in the same
group, Zeff is essentially the same, but the valence electrons are farther from the nucleus.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in First Ionization Energies
• Generally, as one goes across a row, it gets harder to remove an electron.– As you go from left to
right, Zeff increases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in First Ionization Energies
However, there are two apparent discontinuities in this trend.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in First Ionization Energies
• The first occurs between Groups IIA and IIIA.
• In this case the electron is removed from a p-orbital rather than an s-orbital.– The electron removed
is farther from nucleus.– There is also a small
amount of repulsion by the s electrons.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in First Ionization Energies
• The second occurs between Groups VA and VIA.– The electron removed
comes from doubly occupied orbital.
– Repulsion from the other electron in the orbital aids in its removal.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electron Affinity
Electron affinity is the energy change accompanying the addition of an electron to a gaseous atom:
Cl + e− Cl−
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in Electron Affinity
In general, electron affinity becomes more exothermic as you go from left to right across a row.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in Electron Affinity
There are again, however, two discontinuities in this trend.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in Electron Affinity
• The first occurs between Groups IA and IIA.– The added electron
must go in a p-orbital, not an s-orbital.
– The electron is farther from nucleus and feels repulsion from the s-electrons.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trends in Electron Affinity
• The second occurs between Groups IVA and VA.– Group VA has no
empty orbitals.– The extra electron
must go into an already occupied orbital, creating repulsion.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Properties of Metal, Nonmetals,
and Metalloids
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metals versus Nonmetals
Differences between metals and nonmetals tend to revolve around these properties.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metals versus Nonmetals
• Metals tend to form cations.• Nonmetals tend to form anions.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metals
They tend to be lustrous, malleable, ductile, and good conductors of heat and electricity.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metals
• Compounds formed between metals and nonmetals tend to be ionic.
• Metal oxides tend to be basic.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nonmetals
• These are dull, brittle substances that are poor conductors of heat and electricity.
• They tend to gain electrons in reactions with metals to acquire a noble gas configuration.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nonmetals
• Substances containing only nonmetals are molecular compounds.
• Most nonmetal oxides are acidic.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metalloids
• These have some characteristics of metals and some of nonmetals.
• For instance, silicon looks shiny, but is brittle and fairly poor conductor.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Group Trends
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Alkali Metals
• Alkali metals are soft, metallic solids.
• The name comes from the Arabic word for ashes.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Alkali Metals
• They are found only in compounds in nature, not in their elemental forms.
• They have low densities and melting points.• They also have low ionization energies.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Alkali Metals
Their reactions with water are famously exothermic.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Alkali Metals• Alkali metals (except Li) react with oxygen to
form peroxides.• K, Rb, and Cs also form superoxides:
K + O2 KO2
• They produce bright colors when placed in a flame.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Alkaline Earth Metals
• Alkaline earth metals have higher densities and melting points than alkali metals.
• Their ionization energies are low, but not as low as those of alkali metals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Alkaline Earth Metals
• Beryllium does not react with water and magnesium reacts only with steam, but the others react readily with water.
• Reactivity tends to increase as you go down the group.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Group 6A
• Oxygen, sulfur, and selenium are nonmetals.• Tellurium is a metalloid.• The radioactive polonium is a metal.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Oxygen• There are two allotropes of
oxygen:– O2
– O3, ozone
• There can be three anions:– O2−, oxide– O2
2−, peroxide– O2
1−, superoxide
• It tends to take electrons from other elements (oxidation).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Sulfur
• Sulfur is a weaker oxidizer than oxygen.
• The most stable allotrope is S8, a ringed molecule.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Group VIIA: Halogens
• The halogens are prototypical nonmetals.• The name comes from the Greek words halos
and gennao: “salt formers”.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Group VIIA: Halogens
• They have large, negative electron affinities.– Therefore, they tend to
oxidize other elements easily.
• They react directly with metals to form metal halides.
• Chlorine is added to water supplies to serve as a disinfectant
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Group VIIIA: Noble Gases
• The noble gases have astronomical ionization energies.
• Their electron affinities are positive.– Therefore, they are relatively unreactive.
• They are found as monatomic gases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Group VIIIA: Noble Gases
• Xe forms three compounds:– XeF2
– XeF4 (at right)
– XeF6
• Kr forms only one stable compound:– KrF2
• The unstable HArF was synthesized in 2000.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chapter 8Concepts of Chemical
Bonding
Chemistry, The Central Science, 11th editionTheodore L. Brown, H. Eugene LeMay, Jr.,
and Bruce E. Bursten
John D. BookstaverSt. Charles Community College
Cottleville, MO
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chemical Bonds• Three basic types of
bonds– Ionic
• Electrostatic attraction between ions
– Covalent• Sharing of electrons
– Metallic• Metal atoms bonded to
several other atoms
• Lewis Symbols• Octet Rule
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ionic Bonding
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energetics of Ionic Bonding
As we saw in the last chapter, it takes 495 kJ/mol to remove electrons from sodium.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energetics of Ionic Bonding
We get 349 kJ/mol back by giving electrons to chlorine.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energetics of Ionic Bonding
But these numbers don’t explain why the reaction of sodium metal and chlorine gas to form sodium chloride is so exothermic!
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energetics of Ionic Bonding
• There must be a third piece to the puzzle.
• What is as yet unaccounted for is the electrostatic attraction between the newly-formed sodium cation and chloride anion.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Lattice Energy
• This third piece of the puzzle is the lattice energy:– The energy required to completely separate a mole
of a solid ionic compound into its gaseous ions.
• The energy associated with electrostatic interactions is governed by Coulomb’s law:
Eel = Q1Q2
d
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Lattice Energy
• Lattice energy, then, increases with the charge on the ions.
• It also increases with decreasing size of ions.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energetics of Ionic Bonding:Born-Haber cycle
By accounting for all three energies (ionization energy, electron affinity, and lattice energy), we can get a good idea of the energetics involved in such a process.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energetics of Ionic Bonding
• These phenomena also helps explain the “octet rule.”
• Metals, for instance, tend to stop losing electrons once they attain a noble gas configuration because energy would be expended that cannot be overcome by lattice energies.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Covalent Bonding
• In covalent bonds atoms share electrons.
• There are several electrostatic interactions in these bonds:– Attractions between electrons
and nuclei– Repulsions between electrons– Repulsions between nuclei
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Polar Covalent Bonds
• Though atoms often form compounds by sharing electrons, the electrons are not always shared equally.
• Fluorine pulls harder on the electrons it shares with hydrogen than hydrogen does.
• Therefore, the fluorine end of the molecule has more electron density than the hydrogen end.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electronegativity
• Electronegativity is the ability of atoms in a molecule to attract electrons to themselves.
• On the periodic chart, electronegativity increases as you go…– …from left to right across
a row.– …from the bottom to the
top of a column.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Polar Covalent Bonds
• When two atoms share electrons unequally, a bond dipole results.
• The dipole moment, , produced by two equal but opposite charges separated by a distance, r, is calculated:
= Qr• It is measured in debyes (D).
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Polar Covalent Bonds
The greater the difference in electronegativity, the more polar is the bond.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Lewis Structures
Lewis structures are representations of molecules showing all electrons, bonding and nonbonding.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Lewis Structures
1. Find the sum of valence electrons of all atoms in the polyatomic ion or molecule.– If it is an anion, add one
electron for each negative charge.
– If it is a cation, subtract one electron for each positive charge.
PCl3
5 + 3(7) = 26
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Lewis Structures
2. The central atom is the least electronegative element that isn’t hydrogen. Connect the outer atoms to it by single bonds.
Keep track of the electrons:
26 - 6 = 20
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Lewis Structures
3. Fill the octets of the outer atoms.
Keep track of the electrons:
26 - 6 = 20; 20 - 18 = 2
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Lewis Structures
4. Fill the octet of the central atom.
Keep track of the electrons:
26 - 6 = 20; 20 - 18 = 2; 2 - 2 = 0
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Lewis Structures
5. If you run out of electrons before the central atom has an octet…
…form multiple bonds until it does.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Lewis Structures
• Then assign formal charges.– For each atom, count the electrons in lone pairs and
half the electrons it shares with other atoms.– Subtract that from the number of valence electrons for
that atom: the difference is its formal charge.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Writing Lewis Structures
• The best Lewis structure…– …is the one with the fewest charges.– …puts a negative charge on the most
electronegative atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Resonance
This is the Lewis structure we would draw for ozone, O3. -
+
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Resonance
• But this is at odds with the true, observed structure of ozone, in which…– …both O-O bonds
are the same length.– …both outer
oxygens have a charge of -1/2.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Resonance
• One Lewis structure cannot accurately depict a molecule like ozone.
• We use multiple structures, resonance structures, to describe the molecule.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Resonance
Just as green is a synthesis of blue and yellow…
…ozone is a synthesis of these two resonance structures.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Resonance
• In truth, the electrons that form the second C-O bond in the double bonds below do not always sit between that C and that O, but rather can move among the two oxygens and the carbon.
• They are not localized; they are delocalized.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Resonance
• The organic compound benzene, C6H6, has two resonance structures.
• It is commonly depicted as a hexagon with a circle inside to signify the delocalized electrons in the ring.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Exceptions to the Octet Rule
• There are three types of ions or molecules that do not follow the octet rule:– Ions or molecules with an odd number of
electrons– Ions or molecules with less than an octet– Ions or molecules with more than eight
valence electrons (an expanded octet)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Odd Number of Electrons
Though relatively rare and usually quite unstable and reactive, there are ions and molecules with an odd number of electrons.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Fewer Than Eight Electrons
• Consider BF3:– Giving boron a filled octet places a negative
charge on the boron and a positive charge on fluorine.
– This would not be an accurate picture of the distribution of electrons in BF3.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Fewer Than Eight Electrons
Therefore, structures that put a double bond between boron and fluorine are much less important than the one that leaves boron with only 6 valence electrons.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Fewer Than Eight Electrons
The lesson is: if filling the octet of the central atom results in a negative charge on the central atom and a positive charge on the more electronegative outer atom, don’t fill the octet of the central atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
More Than Eight Electrons
• The only way PCl5 can exist is if phosphorus has 10 electrons around it.
• It is allowed to expand the octet of atoms on the 3rd row or below.– Presumably d orbitals in
these atoms participate in bonding.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
More Than Eight Electrons
Even though we can draw a Lewis structure for the phosphate ion that has only 8 electrons around the central phosphorus, the better structure puts a double bond between the phosphorus and one of the oxygens.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
More Than Eight Electrons
• This eliminates the charge on the phosphorus and the charge on one of the oxygens.
• The lesson is: when the central atom in on the 3rd row or below and expanding its octet eliminates some formal charges, do so.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Covalent Bond Strength
• Most simply, the strength of a bond is measured by determining how much energy is required to break the bond.
• This is the bond enthalpy.• The bond enthalpy for a Cl-Cl bond, D(Cl-Cl),
is measured to be 242 kJ/mol.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Average Bond Enthalpies
• This table lists the average bond enthalpies for many different types of bonds.
• Average bond enthalpies are positive, because bond breaking is an endothermic process.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Average Bond Enthalpies
NOTE: These are average bond enthalpies, not absolute bond enthalpies; the C-H bonds in methane, CH4, will be a bit different than the C-H bond in chloroform, CHCl3.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpies of Reaction
• Yet another way to estimate H for a reaction is to compare the bond enthalpies of bonds broken to the bond enthalpies of the new bonds formed.
• In other words, Hrxn = (bond enthalpies of bonds broken) -
(bond enthalpies of bonds formed)
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpies of Reaction
CH4 (g) + Cl2 (g)
CH3Cl (g) + HCl (g)
In this example, one C-H bond and one Cl-Cl bond are broken; one C-Cl and one H-Cl bond are formed.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Enthalpies of Reaction
So,
H = [D(C-H) + D(Cl-Cl)] - [D(C-Cl) + D(H-Cl)]
= [(413 kJ) + (242 kJ)] - [(328 kJ) + (431 kJ)]
= (655 kJ) - (759 kJ)
= -104 kJ
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Bond Enthalpy and Bond Length
• We can also measure an average bond length for different bond types.
• As the number of bonds between two atoms increases, the bond length decreases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chapter 9Molecular Geometriesand Bonding Theories
Chemistry, The Central Science, 11th editionTheodore L. Brown, H. Eugene LeMay, Jr.,
and Bruce E. Bursten
John D. BookstaverSt. Charles Community College
Cottleville, MO
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Shapes
• The shape of a molecule plays an important role in its reactivity.
• By noting the number of bonding and nonbonding electron pairs we can easily predict the shape of the molecule.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
What Determines the Shape of a Molecule?
• Simply put, electron pairs, whether they be bonding or nonbonding, repel each other.
• By assuming the electron pairs are placed as far as possible from each other, we can predict the shape of the molecule.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electron Domains
• We can refer to the electron pairs as electron domains.
• In a double or triple bond, all electrons shared between those two atoms are on the same side of the central atom; therefore, they count as one electron domain.
• The central atom in this molecule, A, has four electron domains.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Valence Shell Electron Pair Repulsion Theory (VSEPR)
“The best arrangement of a given number of electron domains is the one that minimizes the repulsions among them.”
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electron-Domain Geometries
These are the electron-domain geometries for two through six electron domains around a central atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Electron-Domain Geometries
• All one must do is count the number of electron domains in the Lewis structure.
• The geometry will be that which corresponds to the number of electron domains.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Geometries
• The electron-domain geometry is often not the shape of the molecule, however.
• The molecular geometry is that defined by the positions of only the atoms in the molecules, not the nonbonding pairs.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Geometries
Within each electron domain, then, there might be more than one molecular geometry.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Linear Electron Domain
• In the linear domain, there is only one molecular geometry: linear.
• NOTE: If there are only two atoms in the molecule, the molecule will be linear no matter what the electron domain is.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trigonal Planar Electron Domain
• There are two molecular geometries:– Trigonal planar, if all the electron domains are
bonding,– Bent, if one of the domains is a nonbonding pair.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Nonbonding Pairs and Bond Angle
• Nonbonding pairs are physically larger than bonding pairs.
• Therefore, their repulsions are greater; this tends to decrease bond angles in a molecule.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Multiple Bonds and Bond Angles
• Double and triple bonds place greater electron density on one side of the central atom than do single bonds.
• Therefore, they also affect bond angles.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Tetrahedral Electron Domain
• There are three molecular geometries:– Tetrahedral, if all are bonding pairs,– Trigonal pyramidal if one is a nonbonding pair,– Bent if there are two nonbonding pairs.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trigonal Bipyramidal Electron Domain
• There are two distinct positions in this geometry:– Axial– Equatorial
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trigonal Bipyramidal Electron Domain
Lower-energy conformations result from having nonbonding electron pairs in equatorial, rather than axial, positions in this geometry.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Trigonal Bipyramidal Electron Domain
• There are four distinct molecular geometries in this domain:– Trigonal bipyramidal– Seesaw– T-shaped– Linear
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Octahedral Electron Domain
• All positions are equivalent in the octahedral domain.
• There are three molecular geometries:– Octahedral– Square pyramidal– Square planar
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Larger Molecules
In larger molecules, it makes more sense to talk about the geometry about a particular atom rather than the geometry of the molecule as a whole.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Larger Molecules
This approach makes sense, especially because larger molecules tend to react at a particular site in the molecule.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Polarity
• In Chapter 8 we discussed bond dipoles.
• But just because a molecule possesses polar bonds does not mean the molecule as a whole will be polar.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Polarity
By adding the individual bond dipoles, one can determine the overall dipole moment for the molecule.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Polarity
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Overlap and Bonding
• We think of covalent bonds forming through the sharing of electrons by adjacent atoms.
• In such an approach this can only occur when orbitals on the two atoms overlap.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Overlap and Bonding
• Increased overlap brings the electrons and nuclei closer together while simultaneously decreasing electron-electron repulsion.
• However, if atoms get too close, the internuclear repulsion greatly raises the energy.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
But it’s hard to imagine tetrahedral, trigonal bipyramidal, and other geometries arising from the atomic orbitals we recognize.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
• Consider beryllium:– In its ground electronic
state, it would not be able to form bonds because it has no singly-occupied orbitals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
But if it absorbs the small amount of energy needed to promote an electron from the 2s to the 2p orbital, it can form two bonds.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
• Mixing the s and p orbitals yields two degenerate orbitals that are hybrids of the two orbitals.– These sp hybrid orbitals have two lobes like a p orbital.– One of the lobes is larger and more rounded as is the s
orbital.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
• These two degenerate orbitals would align themselves 180 from each other.
• This is consistent with the observed geometry of beryllium compounds: linear.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
• With hybrid orbitals the orbital diagram for beryllium would look like this.
• The sp orbitals are higher in energy than the 1s orbital but lower than the 2p.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
Using a similar model for boron leads to…
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
…three degenerate sp2 orbitals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
With carbon we get…
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
…four degenerate
sp3 orbitals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
For geometries involving expanded octets on the central atom, we must use d orbitals in our hybrids.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
This leads to five degenerate sp3d orbitals…
…or six degenerate sp3d2 orbitals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hybrid Orbitals
Once you know the electron-domain geometry, you know the hybridization state of the atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Valence Bond Theory
• Hybridization is a major player in this approach to bonding.
• There are two ways orbitals can overlap to form bonds between atoms.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Sigma () Bonds
• Sigma bonds are characterized by– Head-to-head overlap.– Cylindrical symmetry of electron density about the
internuclear axis.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Pi () Bonds
• Pi bonds are characterized by– Side-to-side overlap.– Electron density
above and below the internuclear axis.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Single Bonds
Single bonds are always bonds, because overlap is greater, resulting in a stronger bond and more energy lowering.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Multiple Bonds
In a multiple bond one of the bonds is a bond and the rest are bonds.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Multiple Bonds
• In a molecule like formaldehyde (shown at left) an sp2 orbital on carbon overlaps in fashion with the corresponding orbital on the oxygen.
• The unhybridized p orbitals overlap in fashion.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Multiple Bonds
In triple bonds, as in acetylene, two sp orbitals form a bond between the carbons, and two pairs of p orbitals overlap in fashion to form the two bonds.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Delocalized Electrons: Resonance
When writing Lewis structures for species like the nitrate ion, we draw resonance structures to more accurately reflect the structure of the molecule or ion.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Delocalized Electrons: Resonance
• In reality, each of the four atoms in the nitrate ion has a p orbital.
• The p orbitals on all three oxygens overlap with the p orbital on the central nitrogen.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Delocalized Electrons: Resonance
This means the electrons are not localized between the nitrogen and one of the oxygens, but rather are delocalized throughout the ion.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Resonance
The organic molecule benzene has six bonds and a p orbital on each carbon atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Resonance
• In reality the electrons in benzene are not localized, but delocalized.
• The even distribution of the electrons in benzene makes the molecule unusually stable.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Orbital (MO) Theory
Though valence bond theory effectively conveys most observed properties of ions and molecules, there are some concepts better represented by molecular orbitals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Orbital (MO) Theory
• In MO theory, we invoke the wave nature of electrons.
• If waves interact constructively, the resulting orbital is lower in energy: a bonding molecular orbital.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Orbital (MO) Theory
If waves interact destructively, the resulting orbital is higher in energy: an antibonding molecular orbital.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
MO Theory
• In H2 the two electrons go into the bonding molecular orbital.
• The bond order is one half the difference between the number of bonding and antibonding electrons.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
MO Theory
For hydrogen, with two electrons in the bonding MO and none in the antibonding MO, the bond order is
12
(2 - 0) = 1
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
MO Theory
• In the case of He2, the bond order would be
12
(2 - 2) = 0
• Therefore, He2 does not exist.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
MO Theory
• For atoms with both s and p orbitals, there are two types of interactions:– The s and the p orbitals
that face each other overlap in fashion.
– The other two sets of p orbitals overlap in fashion.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
MO Theory
• The resulting MO diagram looks like this.
• There are both and bonding molecular orbitals and * and * antibonding molecular orbitals.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
MO Theory
• The smaller p-block elements in the second period have a sizeable interaction between the s and p orbitals.
• This flips the order of the and molecular orbitals in these elements.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Second-Row MO Diagrams
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chapter 10Gases
Chemistry, The Central Science, 11th editionTheodore L. Brown; H. Eugene LeMay, Jr.;
and Bruce E. Bursten
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Characteristics of Gases
• Unlike liquids and solids, gases– expand to fill their containers;– are highly compressible;– have extremely low densities.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
• Pressure is the amount of force applied to an area.
Pressure
• Atmospheric pressure is the weight of air per unit of area.
P =FA
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Units of Pressure
• Pascals– 1 Pa = 1 N/m2
• Bar– 1 bar = 105 Pa = 100 kPa
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Units of Pressure
• mm Hg or torr–These units are literally the difference in the heights measured in mm (h) of two connected columns of mercury.
• Atmosphere1.00 atm = 760 torr
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Standard Pressure
• Normal atmospheric pressure at sea level is referred to as standard pressure.
• It is equal to1.00 atm
760 torr (760 mm Hg)101.325 kPa
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Manometer
This device is used to measure the difference in pressure between atmospheric pressure and that of a gas in a vessel.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Boyle’s Law
The volume of a fixed quantity of gas at constant temperature is inversely proportional to the pressure.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
As P and V areinversely proportional
A plot of V versus P results in a curve.
Since
V = k (1/P)This means a plot of V versus 1/P will be a straight line.
PV = k
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Charles’s Law
• The volume of a fixed amount of gas at constant pressure is directly proportional to its absolute temperature.
A plot of V versus T will be a straight line.
• i.e.,VT
= k
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Avogadro’s Law
• The volume of a gas at constant temperature and pressure is directly proportional to the number of moles of the gas.
• Mathematically, this means V = kn
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ideal-Gas Equation
V 1/P (Boyle’s law)V T (Charles’s law)V n (Avogadro’s law)
• So far we’ve seen that
• Combining these, we get
V nTP
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ideal-Gas Equation
The constant of proportionality is known as R, the gas constant.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ideal-Gas Equation
The relationship
then becomes
nTP
V
nTP
V = R
or
PV = nRT
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Densities of Gases
If we divide both sides of the ideal-gas equation by V and by RT, we get
nV
PRT
=
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
• We know thatmoles molecular mass = mass
Densities of Gases
• So multiplying both sides by the molecular mass () gives
n = m
PRT
mV
=
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Densities of Gases
• Mass volume = density
• So,
Note: One only needs to know the molecular mass, the pressure, and the temperature to calculate the density of a gas.
PRT
mV
=d =
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Molecular Mass
We can manipulate the density equation to enable us to find the molecular mass of a gas:
Becomes
PRT
d =
dRTP =
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dalton’s Law ofPartial Pressures
• The total pressure of a mixture of gases equals the sum of the pressures that each would exert if it were present alone.
• In other words,
Ptotal = P1 + P2 + P3 + …
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Partial Pressures
• When one collects a gas over water, there is water vapor mixed in with the gas.
• To find only the pressure of the desired gas, one must subtract the vapor pressure of water from the total pressure.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Kinetic-Molecular Theory
This is a model that aids in our understanding of what happens to gas particles as environmental conditions change.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Main Tenets of Kinetic-Molecular Theory
Gases consist of large numbers of molecules that are in continuous, random motion.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Main Tenets of Kinetic-Molecular Theory
The combined volume of all the molecules of the gas is negligible relative to the total volume in which the gas is contained.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Main Tenets of Kinetic-Molecular Theory
Attractive and repulsive forces between gas molecules are negligible.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Main Tenets of Kinetic-Molecular Theory
Energy can be transferred between molecules during collisions, but the average kinetic energy of the molecules does not change with time, as long as the temperature of the gas remains constant.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Main Tenets of Kinetic-Molecular Theory
The average kinetic energy of the molecules is proportional to the absolute temperature.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Effusion
Effusion is the escape of gas molecules through a tiny hole into an evacuated space.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Effusion
The difference in the rates of effusion for helium and nitrogen, for example, explains a helium balloon would deflate faster.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Diffusion
Diffusion is the spread of one substance throughout a space or throughout a second substance.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Graham's Law
KE1 KE2=
1/2 m1v12 1/2 m2v2
2=
=m1
m2
v22
v12
m1
m2
v22
v12
= v2
v1
=
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Real Gases
In the real world, the behavior of gases only conforms to the ideal-gas equation at relatively high temperature and low pressure.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Real Gases
Even the same gas will show wildly different behavior under high pressure at different temperatures.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Deviations from Ideal Behavior
The assumptions made in the kinetic-molecular model (negligible volume of gas molecules themselves, no attractive forces between gas molecules, etc.) break down at high pressure and/or low temperature.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Corrections for Nonideal Behavior
• The ideal-gas equation can be adjusted to take these deviations from ideal behavior into account.
• The corrected ideal-gas equation is known as the van der Waals equation.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The van der Waals Equation
) (V − nb) = nRTn2aV2(P +
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Chapter 11Intermolecular Forces,
Liquids, and Solids
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
States of MatterThe fundamental difference between states of matter is the distance between particles.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
States of MatterBecause in the solid and liquid states particles are closer together, we refer to them as condensed phases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
The States of Matter
• The state a substance is in at a particular temperature and pressure depends on two antagonistic entities:
– the kinetic energy of the particles;
– the strength of the attractions between the particles.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Intermolecular Forces
The attractions between molecules are not nearly as strong as the intramolecular attractions that hold compounds together.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Intermolecular Forces
They are, however, strong enough to control physical properties such as boiling and melting points, vapor pressures, and viscosities.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Intermolecular Forces
These intermolecular forces as a group are referred to as van der Waals forces.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
van der Waals Forces
• Dipole-dipole interactions
• Hydrogen bonding
• London dispersion forces
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ion-Dipole Interactions
• Ion-dipole interactions (a fourth type of force), are important in solutions of ions.
• The strength of these forces are what make it possible for ionic substances to dissolve in polar solvents.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dipole-Dipole Interactions
• Molecules that have permanent dipoles are attracted to each other.– The positive end of one is
attracted to the negative end of the other and vice-versa.
– These forces are only important when the molecules are close to each other.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Dipole-Dipole Interactions
The more polar the molecule, the higher is its boiling point.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
London Dispersion Forces
While the electrons in the 1s orbital of helium would repel each other (and, therefore, tend to stay far away from each other), it does happen that they occasionally wind up on the same side of the atom.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
London Dispersion Forces
At that instant, then, the helium atom is polar, with an excess of electrons on the left side and a shortage on the right side.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
London Dispersion Forces
Another helium nearby, then, would have a dipole induced in it, as the electrons on the left side of helium atom 2 repel the electrons in the cloud on helium atom 1.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
London Dispersion Forces
London dispersion forces, or dispersion forces, are attractions between an instantaneous dipole and an induced dipole.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
London Dispersion Forces
• These forces are present in all molecules, whether they are polar or nonpolar.
• The tendency of an electron cloud to distort in this way is called polarizability.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Factors Affecting London Forces
• The shape of the molecule affects the strength of dispersion forces: long, skinny molecules (like n-pentane tend to have stronger dispersion forces than short, fat ones (like neopentane).
• This is due to the increased surface area in n-pentane.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Factors Affecting London Forces
• The strength of dispersion forces tends to increase with increased molecular weight.
• Larger atoms have larger electron clouds which are easier to polarize.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Which Have a Greater Effect?Dipole-Dipole Interactions or Dispersion Forces
• If two molecules are of comparable size and shape, dipole-dipole interactions will likely the dominating force.
• If one molecule is much larger than another, dispersion forces will likely determine its physical properties.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
How Do We Explain This?
• The nonpolar series (SnH4 to CH4) follow the expected trend.
• The polar series follows the trend from H2Te through H2S, but water is quite an anomaly.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hydrogen Bonding
• The dipole-dipole interactions experienced when H is bonded to N, O, or F are unusually strong.
• We call these interactions hydrogen bonds.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Hydrogen Bonding
• Hydrogen bonding arises in part from the high electronegativity of nitrogen, oxygen, and fluorine.
Also, when hydrogen is bonded to one of those very electronegative elements, the hydrogen nucleus is exposed.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Summarizing Intermolecular Forces
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Intermolecular Forces Affect Many Physical Properties
The strength of the attractions between particles can greatly affect the properties of a substance or solution.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Viscosity• Resistance of a liquid
to flow is called viscosity.
• It is related to the ease with which molecules can move past each other.
• Viscosity increases with stronger intermolecular forces and decreases with higher temperature.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Surface Tension
Surface tension results from the net inward force experienced by the molecules on the surface of a liquid.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Solids
• We can think of solids as falling into two groups:– crystalline, in which
particles are in highly ordered arrangement.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Solids
• We can think of solids as falling into two groups:– amorphous, in which
there is no particular order in the arrangement of particles.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Crystalline SolidsBecause of the ordered in a crystal, we can focus on the repeating pattern of arrangement called the unit cell.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Crystalline Solids
There are several types of basic arrangements in crystals, like the ones depicted above.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Crystalline Solids
We can determine the empirical formula of an ionic solid by determining how many ions of each element fall within the unit cell.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Ionic Solids
• What are the empirical formulas for these compounds?– (a) Green: chlorine; Gray: cesium– (b) Yellow: sulfur; Gray: zinc– (c) Gray: calcium; Blue: fluorine
CsCl ZnS CaF2
(a) (b) (c)
MatterAnd
Measurement
MatterAnd
Measurement
MatterAnd
Measurement
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Attractions in Ionic CrystalsIn ionic crystals, ions pack themselves so as to maximize the attractions and minimize repulsions between the ions.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Types of Bonding in Crystalline Solids
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Covalent-Network andMolecular Solids
• Diamonds are an example of a covalent-network solid, in which atoms are covalently bonded to each other.– They tend to be hard and have high melting
points.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Covalent-Network andMolecular Solids
• Graphite is an example of a molecular solid, in which atoms are held together with van der Waals forces.– They tend to be softer and have lower melting
points.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Metallic Solids
• Metals are not covalently bonded, but the attractions between atoms are too strong to be van der Waals forces.
• In metals valence electrons are delocalized throughout the solid.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Changes
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energy Changes Associated with Changes of State
The heat of fusion is the energy required to change a solid at its melting point to a liquid.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energy Changes Associated with Changes of State
The heat of vaporization is defined as the energy required to change a liquid at its boiling point to a gas.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Energy Changes Associated with Changes of State
• The heat added to the system at the melting and boiling points goes into pulling the molecules farther apart from each other.
• The temperature of the substance does not rise during a phase change.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Vapor Pressure
• At any temperature some molecules in a liquid have enough energy to escape.
• As the temperature rises, the fraction of molecules that have enough energy to escape increases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Vapor Pressure
As more molecules escape the liquid, the pressure they exert increases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Vapor Pressure
The liquid and vapor reach a state of dynamic equilibrium: liquid molecules evaporate and vapor molecules condense at the same rate.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Vapor Pressure
• The boiling point of a liquid is the temperature at which it’s vapor pressure equals atmospheric pressure.
• The normal boiling point is the temperature at which its vapor pressure is 760 torr.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagrams
Phase diagrams display the state of a substance at various pressures and temperatures and the places where equilibria exist between phases.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagrams
• The circled line is the liquid-vapor interface.• It starts at the triple point (T), the point at
which all three states are in equilibrium.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagrams
It ends at the critical point (C); above this critical temperature and critical pressure the liquid and vapor are indistinguishable from each other.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagrams
Each point along this line is the boiling point of the substance at that pressure.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagrams
• The circled line in the diagram below is the interface between liquid and solid.
• The melting point at each pressure can be found along this line.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagrams• Below the triple point the substance cannot
exist in the liquid state.• Along the circled line the solid and gas
phases are in equilibrium; the sublimation point at each pressure is along this line.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagram of Water
• Note the high critical temperature and critical pressure.– These are due to the
strong van der Waals forces between water molecules.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagram of Water
• The slope of the solid-liquid line is negative.– This means that as the
pressure is increased at a temperature just below the melting point, water goes from a solid to a liquid.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagram of Carbon Dioxide
Carbon dioxide cannot exist in the liquid state at pressures below 5.11 atm; CO2 sublimes at normal pressures.
MatterAnd
Measurement
© 2009, Prentice-Hall, Inc.
Phase Diagram of Carbon Dioxide
The low critical temperature and critical pressure for CO2 make supercritical CO2 a good solvent for extracting nonpolar substances (like caffeine)