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AP Chemistry
To: 2013-2014 AP Chemistry students From: Big Evergreen III, a past student of Mrs. Moses SUBJECT: Hints / strategies / review to survive AP Chemistry. Think categorically: know acid from base, strong from weak, metal from nonmetal,
ionic from covalent, etc. Know your nomenclature, you will need it for everything. When you are taught something, learn it: many concepts are reused within other
concepts so if you didn’t learn something in the first place it will hurt you later. Know your solubility rules: this will help so much on the reactions part of the exam! Learn the details and the relationships: How does temperature, pressure, etc. affect a
certain system? What does it mean if something is solid, liquid or gas? What are certain
numbers dependent upon?
Table of Contents 1. Atoms, Molecules, and Ions...........................................................................................................
2. Stoichiometry .................................................................................................................................
3. Reactions ........................................................................................................................................
4. Gases ..............................................................................................................................................
5. Thermochemistry ...........................................................................................................................
6. Atomic Structure & Periodicity .....................................................................................................
7. Fundamentals of Chemical Bonding ..............................................................................................
8. Theories of Chemical Bonding ......................................................................................................
9. Liquids & Solids ............................................................................................................................
10. Properties of Solutions .................................................................................................................
11. Kinetics ........................................................................................................................................
12. Chemical Equilibrium ..................................................................................................................
13. Acids and Bases ...........................................................................................................................
14. Aqueous Equilibria ......................................................................................................................
15. Spontaneity of Chemical Processes .............................................................................................
16. Electrochemistry ..........................................................................................................................
17. Nuclear Chemistry & Radiochemistry .........................................................................................
18. O-Chem aka Organic Chemistry ..................................................................................................
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Atomic Structure and Periodicity Particles and Waves
Electromagnetic Radiation
Much information about atomic electronic structure was obtained from studies on
the interaction of electromagnetic radiation with matter.
• Electromagnetic radiation carries energy through space & has a wavelike
nature. E.g. light, x-rays, microwaves
• Each wave has a characteristic wavelength and frequency.
wavelength, λ: distance between wave peaks. Units: m
frequency, ν: # of cycles (complete waves) that pass a point in one second.
Units are hertz. 1 Hz = 1 s-1
In a vacuum, all electromagnetic radiation travels at a speed of 3.00 x 108
m/s. This is the speed of light, c.
c = νλ (speed of light = frequency X wavelength)
units: m/s = s-1 m
frequency and wavelength are inversely proportional
Practice Problems
*
1. Calculate the frequency of an X ray that has a wavelength of 8.21 nm.
(hint: 1nm = 10-9
m)
Step 1: Write the formula to find frequency if wavelength is given
c = νλ
Step 2: Manipulate the formula so that you’re solving for frequency
c = νλ c/λ = ν/λ ν = c/λ
Step 3: Convert 8.21nm to m so that we can cancel out the units in the
train-and-caboose (this is kind of a given, but I just added it as a step
anyway…)
8.21 nm x 10-9
m = 8.21 x 10-9
m
1 nm
Step 3: Plug in the values and chug
ν = (3 x 108 m/s) / (8.21 x 10
-9 m)
= 3.65 x 1016
1/s or 3.65 x 1016
s-1
Now, try the rest on your own!
2. Calculate the wavelength, in nm, of infra-red radiation that has a
frequency of 9.76 x 1013
s-1
(the answer should be in nm, not m)
3. Calculate the frequency, in hertz, of a microwave that has a wavelength
of 1.07 mm (that’s right, mm not nm!) Answers: 2) 3.1 x 103 nm 3) 2.8 x 1011 s-1
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Electromagnetic Spectrum
A "continuum" of all possible wavelengths of electromagnetic radiation
Humans only see a small part of the whole EMS
The region we can see is called “visible light” (our colors)
What you need to know from the Electromagnetic Spectrum (EMS)
1. Memorize each type of wave and know how they are arranged from
lowest to highest energy (Radio, TV, Micro, Infra-red, Visible Light
(ROYGBIV), UltraViolet, X, Gamma) and their frequency
2. Know that low energy corresponds to long wavelengths and low
frequency, whereas high energy corresponds to short wavelengths and
high frequency
3. Wavelengths in the visible region range from about 400 nm to 700 nm
4. Left -> Right is from lowest energy to highest energy
Question:
1. Which light has a higher frequency: the bright red brake lights of an
automobile or the faint green light of a distant traffic signal?
Green light has a higher frequency than Red light, which means it has
more energy
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Just like an atom is the smallest piece of an element, a
“quantum” is the smallest amount of energy you can
gain or lose
Quantized Energy
1900 - Max Planck introduced the theory of “quantum packets of energy”. This
theory states that energy can only be absorbed or released from atoms in discrete
quantities or “bundles.” He called the smallest bundle of energy a “quantum.”
Thus, E is quantized, not continuous.
And since c = λ ν,
h = Planck’s constant = 6.63 x 10-34
J-s
hν = smallest amount of energy
Practice Problems
A “quantum” of energy
(E) = hv
A “quantum” of energy
(E) = h times c
λ
1. Calculate the energy (in Joules) and the frequency (in Hertz) of
electromagnetic radiation that is given off by a sodium vapor lamp if the
wavelength of the radiation that is 515 nm.
Step 1: Write the correct formula to find frequency
c = λ ν
Step 2: Manipulate the formula so that you’re solving for frequency
ν = c / λ
Step 3: Calculate frequency
= 5.83 x 1014
sec-1
or 5.83 x 1014
Hz
Step 4: Write the correct formula to find Energy of electromagnetic radiation
E = hv
Step 5: Use Planck’s constant and the calculated frequency to find Energy
E = hv = (6.63 x 10-34
J.s)(5.83 x 10
14 / s) = 3.87 x 10
-19 J
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*
The Photoelectric Effect
1905 - Einstein used Plank’s theory to explain the
photoelectric effect. He assumed light traveled in
energy packets called photons.
1 photon = smallest increment of radiant energy
• Energy of 1 photon: E = hν
• Thus light has both wave-like characteristics
(EM studies) & particle nature (Planck &
Einstein) a.k.a wave-particle duality of light
•More intense light would have more photons and
thus eject more electrons, whereas higher
frequency light would have more energy and give
the ejected electrons more energy
Here are some super awesome flashcards ~ http://www.funnelbrain.com/fc-14325-line-spectrum.html
Try these on your own.
2. Calculate the smallest increment of energy that can be emitted or
absorbed at a wavelength of 645 nm.
3. What frequency and wavelength of radiation has photons of energy 8.23
x 10-20
J? What type of electromagnetic radiation is this (refer to the EM
spectrum). Hint: find frequency first from the Energy formula(E = hv) and
then plug the calculated frequency into the wavelength and frequency
formula(c = λν).
Answers: 2) 3.08 x 10-19 J 3)2.41 x10-6 m, infrared radiation
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Line spectra
• When white light is passed through a prism, it separates into a continuous
spectrum of all wavelengths of visible light. (ROYGBIV)
• When the light from a heated element passes through a prism, a line spectrum
with distinct lines is observed. Each line corresponds to a specific wavelength
of visible light.
• Each atom has its own unique line spectrum.
BOHR MODEL ~1913
• Bohr tried to explain observed line spectra based on
movement of electrons.
• Niels Bohr used the "planetary model” of the atom
in which electrons orbit the nucleus like planets
orbiting the sun to explain the phenomenon of "line
spectra" (at least for hydrogen)
• charged electrons travel rapidly in orbits around the
tiny + charged nucleus
• Based on Planck's and Einstein's research, Niels Bohr proposed that the energy
possessed by electrons was also "quantized". Therefore, an electron can only be
located in specific orbits (energy levels) and not just anywhere within the electron
cloud
1. Electrons are contained in specific energy levels called orbits. These energy
levels are quantized which means only certain energies are allowed. An e- in
a permitted orbit has a specific energy.
Energy levels are designated by the principal quantum number, n.
n = 1,2,3…
n = 1 is ground state level - this is level closest to nucleus
(lowest in E).
The equation below shows how much energy an electron will have
based on its location in the electron cloud (the energy level it is on)
where...
electrons would have quantized amounts of energy so they could
either be in the first energy level (n = 1) or the second energy level (n
= 2) or the third energy level (n =3 )... and so on but they could not
exist between these levels.
Practice Problem
E = energy of an electron
RH = Rydberg constant = 2.178 x 10-18
J
n = the energy level of the electron
Calculate the amount of energy an electron must have a) to be in the 1st
energy level of a hydrogen atom and b) to be in the third energy level
of a hydrogen atom
a) E =
=
= -2.18 x 10
-18 J
b) E =
=
= -2.42 x 10
-19 J
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2. Electrons circle the nucleus at specific radii. (r α n2)
3. Electrons can jump from one level to another by absorbing or emitting
photons of specific frequencies. (e- must gain energy from heat, radiation,
etc. to jump to higher level.)
An electron at n=1 is in its “ground” state.
In order to jump to a higher energy level (an
“excited” state), the electron must absorb
energy in the form of photons of light.
Since everything wants to be low energy, an
excited electron will eventually transition
from an excited state to a lower energy level
(moves closer to the nucleus). To do this,
the electron must release/emit energy in the
form of photons of light.
This emission is the cause of line spectra!
The emitted energy has a specific
frequency(E=h ) and wavelength(c = λν)
that corresponds to a specific part of the
electromagnetic spectrum. If it falls in the
visible portion of the spectrum, we see it as
a colored spectral “line”. Mystery Solved!
Bohr's theory explains 4 observed lines in line spectra for hydrogen.
Lines correspond to emitted radiation in visible portion of the EM
spectrum when e- jumps from 1 level to another.
This process is responsible for colors of fireworks & neon signs.
Electrons are excited by heat or electricity and electrons jump to
higher energy levels. Light is emitted when electrons lose energy and
drop back down to lower energy levels. The colors correspond to
wavelengths of emitted light waves.
• Calculating ΔE (the transition energy)
This tells you how much energy must be absorbed or emitted to move
from one level to another
1. ΔE = Efinal – Einitial =
2. (-) J means that energy was released/emitted
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Practice Problem
How does Bohr’s model of the atom explain the concept of line spectra?
Planck said energy is quantized
Einstein said light is energy so it must also be quantized (photons)
Bohr said the amount of energy an electron has must also be quantized
So when excited electrons move to a level that is closer to the nucleus by
emitting energy, the energy they emit is represented by
ΔE = hv
which shows the frequency of the emitted energy. With a known frequency,
the wavelength can be calculated (using c = λν) and we can use the
electromagnetic spectrum to determine what type of energy was emitted. If it
is in the visible region, we can see a color (a spectral line).
Practice Problem
***So, excited electrons transitioning from higher to lower energy levels will
emit/release/lose photons of specific wavelengths and frequencies that are often
visible as "colored lines" (line spectra) when viewed through a prism.
Calculate ΔE when an electron moves from n=5 to n=2.
Step 1: Write out the formula you’re going to use
ΔE = Efinal – Einitial =
Step 2: Plug & Chug
ΔE = Efinal – Einitial =
= -4.58 x 10
-19 J
Calculate the frequency and wavelength of light emitted in a hydrogen atom
when an electron goes from n=5 to n=2.
Step 1: Find change in energy
ΔE = Efinal – Einitial =
= -4.58 x 10
-19 J
Step 2: Find frequency
ΔE = hv
V =
= 6.90 x 10
14 s
-1
Step 3: Find wavelength
c = λν
λ =
= 4.3 x 10
-7 m
Step 4: Convert meters to nanometers
4.3 x 10-7
m x 1 nm = 430 nm
10-9
m
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These are the known transitions that
can be made by electrons in a
hydrogen atom. You DO NOT need
to memorize them, but be aware of
the scientist’s names that were used
to name them.
WEAKNESS IN BOHR’S THEORY
Bohr’s calculations fell apart when applied to atom others than hydrogen
(atoms with more than one electron)
Bohr did not take into consideration the interactions that take place when
other electrons are present
o Electrons repel other electrons
o Electrons “shield” each other from nuclear attraction
Interactions with other electrons alter the amount of energy required by
electrons to transition from one level to another
The Particles and Waves section is done
Do these in order to reinforce what you just learned:
1. https://staff.rockwood.k12.mo.us/grayted/apchemistry/Documents/U5%20At
omic%20Structure/PROBSET%201%20Transition%20Energy.pdf (only 2
problems!! )
2. https://docs.google.com/viewer?a=v&pid=sites&srcid=bHNuZXBhbC5jb21
8YXAtY2hlbWlzdHJ5fGd4Ojc4NTlkYjFjNzNmYjUwMzc (only do
questions # 6 and 48(part a- i and ii, part b- i, ii, and iii(you’re smart, I know
you can think of a plausible reason for part iii!!))
3. https://staff.rockwood.k12.mo.us/grayted/apchemistry/Documents/U5%20At
omic%20Structure/PROBSET%205%20Test%20Prep%20Atomic%20Struct
ure.pdf (do #1, 2, 3, 4, 5, 6, 7, 8, 9, 14, 15, 16, and 23(if you want but I’ll
explain how to do this at the tutoring sesh) you can do the other ones too, but
some of them are a bit redundant)
I’ll post a review key for these questions when I get a chance.
By the end of the semester, you’ll be able to answer all the question on the
review don’t let these questions intimidate you!
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Quantum Numbers
THE QUANTUM-MECHANICAL MODEL OF THE ATOM
This is how we envision the atom today
Planck noted that excited matter emits energy
Einstein showed that energy acts like both a wave (it has frequency and
wavelength) and a particle (bundled into packets called photons)
Louis DeBroglie wondered, “If light waves can act like particles of matter,
could particles of matter act like waves?”
o DeBroglie discovered that electrons could behave like waves… a
standing wave (like a vibrating guitar string). The particle and wave
properties are related by:
λ =
where h = Planck’s constant
m = mass of particle
v = velocity
Erwin Schrodinger developed an equation that describes electron behavior
as both a particle and a wave (the equation has a wave function, Ψ)
1. When you square the wave function, Ψ, you get a 3-dimensional
probability map that describes regions in space (the electron cloud)
where electrons are likely to be. We call these regions “orbitals”
(This relates to QUANTUM NUMBERS!!! I really liked
quantum numbers obvs)
2. He also set-up and solved a series of complex equations that took into
account:
KE (kinetic energy) of an electron
Wavelength of an electron
Attraction of electron for nucleus
Repulsions between electrons
Heisenberg Uncertainty Principle
Both the position and the
momentum of an electron cannot be
exactly known at the same time (ask
Moses to give her example about the
speed ticket for this principle, it’ll help
you remember)
1. In order to known either
the location or momentum of an
electron, light must hit the electron and
bounce back to your eye or measuring
device… however, the light that hits the
electron will cause it to change
momentum and/or location… it’s a no-
win situation
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QUANTUM NUMBERS (eep, i’m so excited! i loved quantum numbers last year!)
Mathematical solutions to Schrodinger’s equation are associated with a set
of 3 quantum numbers
1. Principal quantum number, n
2. Azimuthal quantum number, m
3. Magnetic quantum number, ml
They are kind of like an “address” that tells us where each electron lives
within a given atom
Every electron within an atom has a unique set of quantum numbers
Principal Quantum Number (n)
Generally referred to as the “shell”
Tells the average distance from the nucleus an electron is
1. As “n” becomes larger, the radius that the electron can travel away
from the nucleus gets larger
2. Think of “n” as similar to the Bohr energy levels
Each shell can hold a max of electrons equal to 2n2
1. The first four shells can hold 2, 8, 18, and 32 electrons, respectively
Angular Momentum Quantum Number (l)
Generally referred to as the “sublevel” or “subshell” (i’m going to call them
the sublevel)
Tells the shape of the orbital
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Allowed values of l = 0, 1, 2, 3, …
o The number of sublevels possible in each shell is equal to the value of
n for that subshell
The 3rd
subshell (n = 3) may contain a maximum of three
sublevels
o The value of l can never be greater than n – 1
Sublevels in the Atom
Principal Level / Shell (n) Sublevel Number, l Sublevel Letter
1 0 s
2 0,1 s, p
3 0,1,2 s, p, d
4 0,1,2,3 s, p, d, f
Problem: If n=3, what are the allowed values of l
Answer: 0, 1, 2 (s, p, d)
Magnetic Quantum Number
Generally referred to as the “orbital”
Tells the orientation of the orbital in space
Any orbital can hold a maximum of two electrons
YOU MUST KNOW HOW MANY ORIENTATIONS ARE POSSIBLE
FOR EACH ORBITAL
o 1 for s
o 3 for p
o 5 for d
o 7 for f
The number of orbitals that a sublevel may have depends on the azimuthal
quantum number, l, of the sublevel and is equal to 2l + 1
Orbitals in the Atom
Sublevel
number, l
Sublevel letter Number of
orbitals, 2l + 1
Number of
electrons per
sublevel
0 s 1 2
1 p 3 6
2 d 5 10
3 f 7 14
Allowed values ml = -l… -3, -2, -1, 0, 1, 2, 3, … l
o Orbital s = 0
o Orbital p = -1, 0 +1
o Orbital d = -2, -1, 0, +1, +2
o Orbital f = -3, -2, -1, 0, +1, +2, +3
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Problem: If l = 2, what are the allowed values ml?
Answer: -2, -1, 0, 1, 2
Note that when l = 2 that corresponds to a “d” orbital. There are 5 possible
orientations of “d” orbitals, right? When l = 2, there are also 5 possible values for
ml. See the relationship?
Electron Spin Quantum Number (ms)
Generally referred to as the “spin”
This quantum number is NOT part of a solution to Schrodinger’s equation. It
was later added to ensure that each electron (even those paired up in the
same orbital) has its own unique set of quantum numbers to identify it
o Pauli Exclusion’s Principle: no two electrons in the same atom may
have the same four quantum numbers
Tells the spin of the electron within the orbital
Spinning charges produce a magnetic field. In order for two electrons to
exist in the same orbital, they must spin in opposite directions thereby
creating opposite magnetic fields that cancel each other out. This minimizes
electron-to-electron repulsion and thus creates a lower energy state that is
more stable
Allowed values of ms = +1/2 or -1/2
A Summary of Schrodinger’s “Quantum-Mechanical” Model of the Atom
1. Electrons don't just move around the nucleus of
the atom in simple circular "orbits" as Bohr had
predicted. Schrodinger developed complex equations
that describe 3-dimensional regions within the atom
where electrons are likely to be found. These regions
are called "orbitals", and 90% of the time, electrons
will be found somewhere within that region.
2. Possible solutions to Schrodinger's equations
result in a set of 3 quantum numbers (n, l, ml) that describe the size, shape, and
orientation of the orbitals, respectively. They are sort of like an "address" for each
electron within an atom.
3. According to Heisenberg's Uncertainty Principle, the more you know about an
electron's location, the less you know about its momentum and vice versa.
Schrodinger’s Quantum Mechanical Model > Bohr’s Model
Problem: Write all possible sets of quantum numbers for an electron in a 3p orbital
n = 3; l = 1 since it is a “p” orbital; there are three orbitals, so ml = -1, 0, 1
(3, 1, -1, ½) (3, 1, -1, -1/2)
(3, 1, 0, ½) (3, 1, 0, -1/2)
(3, 1, 1, ½) (3, 1, 1, -1/2)
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The Quantum Numbers section is done
Do these in order to reinforce what you just learned:
1. https://staff.rockwood.k12.mo.us/grayted/apchemistry/Documents/U5%20At
omic%20Structure/PROBSET%202%20Quantum%20Numbers.pdf (only 15
questions) 2. https://staff.rockwood.k12.mo.us/grayted/apchemistry/Documents/U5%20At
omic%20Structure/PROBSET%205%20Test%20Prep%20Quantum%20Nu
mbers.pdf (only do a few problems from the first 5 pages) 3. http://www.pwista.com/Midterm%20Review.pdf (there are A LOAD of
questions on here. But just do #1-12 or just #7-12)
I’ll post an answer key for these questions when I get a chance. If I don’t
post ‘em fast enough, bring the questions to tutoring and I’ll give you the
answers then.
By the end of the semester you’ll be able to answer all the question on the
review don’t let these questions intimidate you!