a=Edge of the unit cell

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1.SOLID STATE
Number of atoms in a unit cell:
Type of unit cell
Simple (Primitive)cubic
lattice
Body centered unit cell
Face cetred cubic cell
No of
atoms per
unit cell(Z)
1
2
4
Relation between atomic radius(r) and the edge length (a):
Simple cube :
r=
Face centred:
r=
Body centred:
r=
π‘Ž
2
π‘Ž
2√2
√3π‘Ž
4
=0.3535a
=0.433a
Relationship betweenDensity and edge of cubic crystals:
ρ=
𝑍 𝑀
𝑁𝐴 π‘Ž3
Where ρ= density of the crystal in g mol-1
Z=Number of particles per unit cell
M=Molar mass of the element.
a=Edge of the unit cell
2. SOLUTIONS
1. Molarity
=
π‘π‘’π‘šπ‘π‘’π‘Ÿ π‘œπ‘“ π‘šπ‘œπ‘™π‘’π‘  π‘œπ‘“ π‘‘β„Žπ‘’ π‘ π‘œπ‘™π‘’π‘‘π‘’
π‘‰π‘œπ‘™π‘’π‘šπ‘’ π‘œπ‘“ π‘‘β„Žπ‘’ π‘ π‘œπ‘™π‘’π‘‘π‘–π‘œπ‘› 𝑖𝑛 𝐿
2. Mole fraction =
3. Molality
𝑛1
𝑛1 +𝑛2
π‘π‘’π‘šπ‘π‘’π‘Ÿ π‘œπ‘“ π‘šπ‘œπ‘™π‘’π‘  π‘œπ‘“ π‘ π‘œπ‘™π‘’π‘‘π‘’
=
π‘€π‘Žπ‘ π‘  π‘œπ‘“ π‘ π‘œπ‘™π‘£π‘’π‘›π‘‘ 𝑖𝑛 𝐾𝑔
Henry’s law:
The mass of a gas dissolved in a given volume of of the liquid at constant
temperature is directly proportional to the pressure of the gas present in
equilibrium with the liquid.
m = kH p
The widely used form of Henry’s Law is
“The partial pressure of a gas in vapour phase is directly proportional to
the mole fraction of the gas in the solution.”
π’«π’œ= 𝒦ℋ π’³π’œ
Raoult’s law:
“The vapour pressure of a solution containing non-volatile solute is directly
proportional to the mole fraction of the solvent.”
𝒫 A=𝒫 β—¦A𝒳 A
Raoult’s law as a special case of Henry”s law:
Comparing the two laws, the following conclusion can be drawn:
Pressure of the volatile component of a solution is directly proportional to
its mole fraction.
The two equations become identical when KH becomes equal to 𝒫 β—¦A
.
Colligative properties:
Those properties which depend only on the number of particles of the
solute not on the nature of the solute particles.
Relative lowering of vapour pressure:
πœŸπ’‘
=
π’‘πŸŽ 𝑨
π’‘πŸŽ 𝑨−𝒑𝑨
π’‘πŸŽ 𝑨
= 𝓧B =
𝑾 𝑩 ⁄𝑴 𝑩
𝑾𝑨 ⁄𝑴𝑨+ 𝑾𝑩 ⁄𝑴𝑩
Δp= Depression in vapour pressure
𝑝0 𝐴=Vapour pressure of pure solvent
π’«π’œ = π‘‰π‘Žπ‘π‘œπ‘’π‘Ÿ π‘π‘Ÿπ‘’π‘ π‘ π‘’π‘Ÿπ‘’ π‘œπ‘“ π‘ π‘œπ‘™π‘’π‘‘π‘–π‘œπ‘›
𝒳ℬ = π‘šπ‘œπ‘™π‘’ π‘“π‘Ÿπ‘Žπ‘π‘‘π‘–π‘œπ‘› π‘œπ‘“ π‘π‘œπ‘šπ‘π‘œπ‘›π‘’π‘›π‘‘ 𝐡(π‘†π‘œπ‘™π‘’π‘‘π‘’)
𝒲A=Mass of component A(solvent)
Elevation in boiling point:
ΔTb=𝒦 b m= 𝒦 b
π‘Šπ΅ ×1000
𝑀𝐡 π‘Šπ΄
ΔTb= Elevation in boiling point
𝒦 b = molal elvation constant in K Kg mol-1
m = molality( mol/g)
WB= Mass of solute(g)
MB= Molar mass of solute
WA =Mass of solvent in g
Kb =
𝑀𝐴 𝑅𝑇𝑏2
π›₯π‘£π‘Žπ‘ 𝐻×1000
Kb = Molal elevation constant (K Kg mol-1)
MA=molar mas of solvent
R= Universal gas constant (8.314 J K-1mol-1; 8.314*10-2 L bar K-1mol-1;
8.21*10-2 L atm K-1mol-1)
π›₯π‘£π‘Žπ‘ 𝐻=Enthalpy of vaporization of solvent
𝑇𝑏 = π΅π‘œπ‘–π‘™π‘–π‘›π‘” π‘π‘œπ‘–π‘›π‘‘ π‘œπ‘“ π‘π‘’π‘Ÿπ‘’ π‘ π‘œπ‘™π‘£π‘’π‘›π‘‘
Depression in freezing point:
ΔT f= K f m
ΔTf=
𝐾𝑓 ×π‘Šπ΅ ×1000
𝑀𝐡 π‘Šπ΄
Kf= Molal freezing constant
Determination of molar mass from osmotic pressure:
πœ‹=
π‘Šπ΅ ×𝑅𝑇
𝑉𝑀𝐡
(𝑂𝑅)
πœ‹ = 𝐢𝑅𝑇
Π = Osmotic pressure
C= Molarity
V= Volume of solution in L
Units of pressure:
1 bar = 10 5 pascal
1atm = 1.01*10 5 Pa
=760 torr
= 1.01 bar
= 760 mm Hg
1 mmHg= 1 torr
1 torr= 1.33*10 -3 bar
VAN’T HOFF’S FACTOR:
π‘‚π‘π‘ π‘’π‘Ÿπ‘£π‘’π‘‘ π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ π‘π‘œπ‘™π‘™π‘–π‘”π‘Žπ‘‘π‘–π‘£π‘’ π‘π‘Ÿπ‘œπ‘π‘’π‘Ÿπ‘‘π‘–π‘’π‘ 
i = π‘π‘œπ‘Ÿπ‘šπ‘Žπ‘™ π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ π‘π‘œπ‘™π‘™π‘–π‘”π‘Žπ‘‘π‘–π‘£π‘’ π‘π‘Ÿπ‘œπ‘π‘’π‘Ÿπ‘‘π‘–π‘’π‘ 
(π‘Žπ‘ π‘ π‘’π‘šπ‘–π‘›π‘” π‘›π‘œ π‘Žπ‘ π‘ π‘œπ‘ π‘–π‘Žπ‘‘π‘–π‘œπ‘› π‘œπ‘Ÿ π‘‘π‘–π‘ π‘ π‘œπ‘ π‘–π‘Žπ‘‘π‘–π‘œπ‘›)
𝑖−1
𝛼=
𝑛−1
𝛼 =the degree of dissociation
i= Vant’ Hoff factor
i=1 if the solute behaves normally
i>1 if solute undergoes dissociation
𝛼=
𝑖−1
𝑛−1
i<1 if the solution undergoes association
𝛼=
1−𝑖
1
𝑛
1−
n = no of ions produced on dissociation/no of ions undergoing
association.
3.ELECTROCHEMISTRY
For the reaction
aA+ bB
cC +dD
Nernst equation to calculate the electrode potential of the cell is
E cell= Eβ—¦cell -
0.0591
𝑛
log
[𝐢]𝑐 [𝐷]𝑑
[𝐴]π‘Ž [𝐡]𝑏
STANDARD ELECTRODE POTENTIAL:
E0cell= E0cathode - E0anode
AT EQUILLIBRIUM, Ecell= 0 ,then
E0cell=
𝟎.πŸŽπŸ“πŸ—
𝒏
log Kc
GIBB’S FREE ENERGY/MAXIMUM WORK DONE
ΔGo= -nF E0cell
G=
1
𝑅
π‘Ž
ρ=R
1
𝜌
G*=R πœ…
πœ…×1000
𝐢
Λm=
πœ…
Λm=𝐢∗1000
C= mol L-1;
𝛼=
π›¬π‘π‘š
𝛬°π‘š
G= Conductance,
a= area,
𝑙
πœ…=
where
R= Resistance
l=length
πœ…=conductivity;
ρ=resistivity
G*= cell constant
Λm=molar conductivity in S cm2 mol-1
k=conductivity in S cm-1
C= molarity in mol/dm3
( 1dm3=1000cm3)
Λm =molar conductivity in S m2 mol-1
K = conductivity in S m-1
C =molarity in mol/m3
( 1m3=1000L; 1L=1/1000m3;L-1 = 1000 m-3)
π›¬π‘π‘š =molar conducitivty of solutions at any
concentration.
𝛬°π‘š =limiting molar conductivity.
4. CHEMICAL KINETICS
Rate=
π‘β„Žπ‘Žπ‘›π‘”π‘’ 𝑖𝑛 π‘‘β„Žπ‘’ π‘π‘œπ‘›π‘π‘’π‘›π‘‘π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘› π‘œπ‘“ π‘Ÿπ‘’π‘Žπ‘π‘‘π‘Žπ‘›π‘‘ π‘œπ‘Ÿ π‘π‘Ÿπ‘œπ‘π‘’π‘π‘‘
π‘‘π‘–π‘šπ‘’
πΉπ‘œπ‘Ÿ π‘‘β„Žπ‘’ π‘Ÿπ‘’π‘Žπ‘π‘‘π‘–π‘œπ‘› 𝐴
𝐡
Rate= -d[R] = d[P]
dt
dt
Rate= K [A]α[𝐡]𝛽
Order=𝛼 + 𝛽
Unit for k:
Zero order reaction
=mol L-1 s-1
First order reaction
=sec-1
Second order reaction =L mol-1 sec-1
Differential rate equation:
πΉπ‘œπ‘Ÿ π‘‘β„Žπ‘’ π‘Ÿπ‘’π‘Žπ‘π‘‘π‘–π‘œπ‘› 𝐴
−
𝑑[𝑅]
𝑑π‘₯
𝐡
= π‘˜[𝑅]𝑛 (For n order)
Integrated rate equation:
1. Zero order
1
π‘˜ = 𝑑 [[𝑅]0− [𝑅]] (Rate of reaction= Rate constant )
2. First order reaction:
k=
2.303
[𝑅]0
π‘™π‘œπ‘”
𝑑
[𝑅]
3. First ordeReaction for gaseous substances
k=
2.303
𝑝𝑖
π‘™π‘œπ‘”
𝑑
(2𝑝𝑖 − 𝑝𝑑 )
where pi =initial pressure,
pt = total pressure
Half life period:
Zero order:
𝑑1/2 =
[𝑅]0
2π‘˜
First order:
𝑑1
2=
0.693
π‘˜
Arrhenius Equation:
K= A𝑒 −πΈπ‘Ž⁄𝑅𝑇
𝑒 −πΈπ‘Ž⁄𝑅𝑇 = Fraction of molecules that have energy
equal to or greater than Ea
π„πš
Log k= logA -
log
π‘˜2
π‘˜1
=
πΈπ‘Ž
2.303 𝑅
𝟐.πŸ‘πŸŽπŸ‘π‘π“
[
𝑇2− 𝑇1
𝑇2 𝑇1
]
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