Solusttible Insoluble Salts
StrongAcids HCl Br Ht 4404 40103 2504 HNO
Group1
4g2 strong Bases Group 1 Metal hydroxides Cabit c short Bacon
15
Aso Beer's Law A Elc
HT wt pop inhibits
opting
soluble salt dominates
million in
Molarity M if
parts per
Molality m Kfounts
Normality
asY cnn.sn
n t forMts accept 1 proton
Rault's Law Elevation
Boiling point Freezing Point Elevation
Pa XAP
Otb Kim
Pa vapor pressure of Kyim
GTb changein temperate in keth
XA molfraction
Ifn
Pao purevaporpresume
Ky solvents constant
i Van't Hfffactor
m molality
EFFIE
Gas
Boyle's Law
pie PV p a
Charles's Law
, Avogadro's Law
K
Van
Lussac's Law Pat
Gay
hit.in ii
Ideal Gas high temp low pressure small particle elasticollis
PV NRT R 0.0821 KITT
R 8.314
Partial pressure
P X Ptotal
widefraction
Gas Density
IF
mass
P
Graham's lawofEffusion
molar mass
Ty
M
oH n In offprod m oHf fear
Cubic
simple
88 1
Body CenteredCubic It 88 2
faced centered Cubic
88 1 6 4
Internal Energy work
StrongAcids HCl Br Ht 4404 40103 2504 HNO
Group1
4g2 strong Bases Group 1 Metal hydroxides Cabit c short Bacon
15
Aso Beer's Law A Elc
HT wt pop inhibits
opting
soluble salt dominates
million in
Molarity M if
parts per
Molality m Kfounts
Normality
asY cnn.sn
n t forMts accept 1 proton
Rault's Law Elevation
Boiling point Freezing Point Elevation
Pa XAP
Otb Kim
Pa vapor pressure of Kyim
GTb changein temperate in keth
XA molfraction
Ifn
Pao purevaporpresume
Ky solvents constant
i Van't Hfffactor
m molality
EFFIE
Gas
Boyle's Law
pie PV p a
Charles's Law
, Avogadro's Law
K
Van
Lussac's Law Pat
Gay
hit.in ii
Ideal Gas high temp low pressure small particle elasticollis
PV NRT R 0.0821 KITT
R 8.314
Partial pressure
P X Ptotal
widefraction
Gas Density
IF
mass
P
Graham's lawofEffusion
molar mass
Ty
M
oH n In offprod m oHf fear
Cubic
simple
88 1
Body CenteredCubic It 88 2
faced centered Cubic
88 1 6 4
Internal Energy work