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at which conditions are gases most ideal
high temp, low pressure, no IMFs
if real pressure is greater than ideal:
size of the particle is not negligible
iI real pressure is less than ideal
due to attractive forces
boltzmann curve
higher peak/more to the left
cold
lower peak more to right
hot
2 different particles at the same temperature
same kinetic energy
heavier one will move slower, vise versa
2 same particles at same temp
KE and speed the same
2 same particles at diff temps
hotter = higher KE and speed
cooler = lower KE and speed
combustion analysis
finding empirical formula for CxHy
what can change the eq. constant
only temp
Le Chat’s increase V or decrease P
move to side with more moles
decrease V increase P
move to side with less moles
equal moles
no shift
redox titration in acicidc solutions
add H2Os to balance O’s and H+ to balance H’s
basic solutions
same as acidic and then add OH- to side H+ was added to and cancel out H2Os
water at temp > 25 Deg C
more acidic, vise versa
strong acids
HCl, HI, HBr, HClO4, HNO3, HClO3, H2SO4
strong bases
NaOH, LiOH, CsOH, RbOH, KOH, Ca(OH)2, Ba(OH)2, Sr(OH)2
WA + WB
Ka = [H3O+][A-]/[HA]
Ka = x²/[HA]
x = [H+]
-log(x)= pH
WA + SB
HA + OH- →A- + H2O
H+ donated from HA to OH
WB + SA
B + H3O+ → HB+ + H2O
H+ donated from H3O+ to B
perfect buffer
[HA] = [A-], pH = pKa
titrations
SA + SB pH = 7
WA + SB pH > 7
SA + WB pH < 7
buffers continued WB + WA
if more WA pH< pKa
if more WB pH>pka
percent ionization
[H+]/[HA]
buffer capacity
smaller concs = lower, vise versa
Henderson Hassle-Bach
pH = pKa + log [A-]/[HA]
if equal concs of A- and HA, log 1 = 0, so pH= pKa (perf buffer)
diamagnetic
no unpaired e-s, can’t be made magnetic
paramagnetic
unpaired e-s, can be made magnetic
effective nuclear charge
number of protons minus number of inner e-
ionization energy exceptions
group 2→ 3 ex. Be to B
2s orbital has a small probability of being closer to the nucleus than 2p so Be is smaller than B, breaking the trend
group 5 → 6 ex. N vs. O
IE for O is less than N because it has a greater repulsion in the p orbital
photoelectron spectra graphs, more protons:
peaks shift to the left
types of light in order from high Energy/High freq/short wavelength to low energy/low frew/long wavelength
GXUVIMR
gamma ray, x-ray, ultra vioelt, visible, infrared, microwave, radio
C (speed of light) =
wavelength * frequency
Eneergy (J) =
planck’s * frequency
X-ray light
removes core e-s
UV, visible
removes valence e-s, excites valence e-s
infrared
vibrational
microwave
polar molecules
translational and rotational energy
Rydberg formula
1/wwavelength = (1.097× 10^7)*(1/(n1)² - 1/(n2)²)
chemical reactivity
top right diagonal of periodic tbl = easy to anion
bottom left = easy to cation
noble gases: nonreactive
changes to concentrations in galvanic cells
Q = [products]/[reactants]
products = oxidated
reactants = reduced
Ecell = Ecell - RT/nF lnQ, so if lnQ is negative Ecell increases, if positive, Ecell decreases
kinetic molecular theory
The temperature of a gas is proportional to its kinetic energy.
collisions that are elastic, momentum is conserved
gas particles have NO IMFs.
size of each atom is insignificant.
K> 10³
rxn goes to completion
K < 10^-4
rxn doesn’t occur
Eq. Hess’ Law
reaction reversed
new Keq = 1/Keq
coefficients multiplied
keq^factor multiplied by
reactions added
indiv keqs multiplied
Ksp
Ksp = concs of ions in solution
bonds breaking
endothermic, vise versa
Hess’ Law for delta H
multiply coeffs by a factor, multiple delta H by same factor
if rxn is reversed, flip sign
if rxns are added, add H values
bond enthalpy
sum of bond enthalpy of reactants - sum of bond enthalpy of products
reverse of regular enthalpy (products - reactants)
Gibbs Free Energy
= delta H - T delta S
if positive: unfavorable
if negative: favorable
favorable
exothermic (-H) and high entropy (+S)
for +H and +S, favorable at high temps
unfavorable
endothermic and low entropy
for -H and -S, favorable at low temps
delta H for melting and freezing
(-)m delta H fusion
poisitve for melting, negative for freezing
for condensing and vaporizing
(-)m delta H vaporization
positive for evaporating, negative for condensing
freezing and condensing
exothermic
melting and vaporizing
endothermic
collisions
must have enough force and correct orientation
unit for rate constant
M^-x times time^-1
x is overall order minus 1
differential rate law
conc. vs. rate
integrated rate law
conc. vs time
zero order
rate = k
linear
[A]t-[A]0=-kt
slope = -k
first order
rate = k[A]
rxn slows down as it proceeds bc concs of reactants decrease
ln[A]t-ln[A]0=-kt
slope = -k
2nd order
rate = k[A]²
less steep than 1st order
1/[A]t-1/[A]0=kt
slope = k
intermediate
formed in one step, used up in later step
catalyst
used in one step, reappears in later step
“rules” for rxn mechanisms
elementary steps add up to overall
unimolecular or bimolecular (must be small for probable collision)
must correlate with observed rate law
quickie method
when slow step is not first step
cross out intermidates
circle remaining reactants and use those to make rate law
products before the slow step go in the denominator
1st order half life
t.5=.693/k
best to use bc isn’t dependent on concentration
electronegativity and acid strength
more electronegative = greater electron drawing = more polarized = H is more attracted to water
stronger the acid = easier to dissociate