intermolecular forces (IMF)
attractive forces between molecules
ion-ion force
attraction between oppositely charged ions
dipole-induced dipole
the non-polar molecule interacts with the polar molecule and the non-polar one becomes slightly polar (temporarily)
ion-dipole force
attraction between an ion and a polar molecule (oppositely charged parts)
dipole-dipole
attraction between a polar molecule and a polar molecule, strength of the reaction depends on the magnitude of the dipole
hydrogen bonding
a type of dipole-dipole; only occurs with an H and an N, O or F.
londen dispersion forces
between non-polar and some other molecule (only occurs although it is non polar because it of the random electron movement). (induced-dipole induced-dipole)
strongest to weakest IMF
1 being strongest, 5 being weakest
ion-ion
ion-dipole
hydrogen bonding
dipole-dipole
londen dispersion
big molecule
highly polarizable
small molecule
highly nonpolarizable
ionic solids
ionic bonds; strong ionic forces - brittle, high melting point, contuctswhen dissolved into a liquid
covalent network solids
connected and layered network (diamond v. graphite); rigid and hard, do not conduct electricity
molecular solids
H-bonds; e.g. ice; weaker IMFs, lower melting points
metallic solids
sea of electrons, meaning it is a good conductor, malleable, ductible
crystalline solid
nice grid
amorphus solid
not so nice grid
solid → liquid → gas
phase change
solid → liquid; weakens IMFs
liquid → gas breaks IMFs
assumptions we make about the kinetic molecular theory
gas moves in random directions of relatively large distances
collisions are perfectly elastic (no energy lost)
gasses move in straight lines intil they collide w/ the container
average KE in a sample of gas is proportional to the temperatures; KE = 1/2*m*v^2
gasses deviate from ideal conditions the most when
there is high pressure, and low temperatures
distillation
seperates mixtures by taking advantage of boiling points and differences in vapor pressures
paper chromatography
seperates mixtures by taking of polarity and nonpolarity
E (energy) =
h*v
energy =planck’s constant * frequency
c (speed of light) =
3.00x10^8 m/s
wavelength * frequency
A (absorbance) =
a * b * c
a = molar absorpivity
b = path length
c = concentation
…however, in a lab, you can ignore that a and the b, as those will stay constant
vapor pressure
when a liquid is introduced into a closed container, it establishes a dynamic equilibrium with its vapor. the pressure of the vapor at equilibrium is referred to as the vapor pressure of the liquid.