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CHY1009 ; Module 2
-States of mater and adsorption isotherms
Sates of mater
The Physical States of Matter - Particulate
theory of matter
Greek philosopher Democritus described matter as made up of tiny
microscopic particles.
the particulate theory of matter was first presented by Democritus
in 400 BC
Traditionally there are three states of matter
John Dalton who is credited with first developing the modern
atomic theory of matter in the early 1800s.
The theory presented by Democritus was predominately a
philosophical statement and therefore not widely accepted.
In contrast, Dalton’s theory was based on careful experimental
observations and measurements and so became the first atomic
theory of matter founded on scientific concepts and principles.
According to the modern atomic theory, matter can be classified
according to both its physical and chemical state
The Physical States of Matter - Particulate
theory of matter
The Physical States of Matter - Particulate
theory of matter
Physical States of Mater- Properties
Gas Liquid Solid
These characteristics affect the physical properties of matter,
such as volume occupancy, density, light scattering, etc.,
Interparticle distance decreases, this decreases volume.
Density (ρ ) ∝ 1/Volume (V)
Density (mass/cm3) of Gas, Liquid, Solids
ρ = mass/unit volume = M/V
For a given mass of substance, density increases while going
from gas-to-liquid and liquid-to-solid.
Solid
(g/cm3)
Liquid (g/cm3)
Gas
(g/cm3)
Ar 1.65 1.40 0.001784
N2 1.026 0.8081 0.001251
O2 1.426 1.149 0.001429
Density (mass/cm3) of Gas, Liquid, Solids - Examples
-the density of a typical solid is about 20% larger than the
corresponding liquid,
-while the liquid is roughly 800 times as dense as the gas.
Plasma – 4th states
of Matter
• Plasma is a “superheated matter”
comprised of ions formed from atoms or
molecules by striping of at least one electron.
• It comprises over 99% of the visible universe.
• In the night sky, plasma glows in the form of
stars, nebulas, and even the auroras that
sometimes ripple above the north and south
poles.
• Plasma is often called “the fourth state of
matter,” along with solid, liquid and gas.
https://www.nasa.gov/sites/default/files/thumbnails/image/147515main_phases_large.jpg
Adsorption isotherms
Surface chemistry is the study of processes that occur
at the interface of two bulk phases.
Bulk phase may be a solid or liquid or gas
Liquid- liquid
Interaction Open Surfaces
solid with Gases
Phenomena of Adsorption
Adsorbate
Adsorbent
Except in special cases, adsorption is an exothermic process,
releases heat to the surrounding.
Enthalpy change is negative ∆Had = -Ve
The phenomena of interaction of a gas or liquid, or ionic species
with a solid surface is referred as adsorption.
Adsorptive
Examples of Adsorption
 (i) Adsorption of O2, H2, CO, Cl2, NH3 or SO2 on surface of charcoal,
 (ii) In a solution of an organic dye, say methylene blue on the
surface of charcoal, i.e., are adsorbed.
 (iii) Aqueous solution of raw sugar, when passed over beds of
animal charcoal, becomes colourless as the colouring substances
are adsorbed by the charcoal.
 (iv) The air becomes dry in the presence of silica gel because the
water molecules get adsorbed on the surface of the gel.
The process of removing an adsorbed substance from a surface
on which it is adsorbed is called desorption.
The attractive interaction can be either long range or short
range
1. Long range interaction: Physical contact, due to Van der
Waals force.
2. Short range interaction: Chemical bonding, such as covalent,
ionic, metallic bonding
What kind of bonding interaction occurs
between adsorbent and adsorbate?
Accordingly, the first one is called physisorption (Physical adsorption)
and the second one is called chemisorption (Chemical adsorption).
Sticking of benzene-like molecules, for example coronene,
on the surface of gold (111) is an example of physisorption.
Example of Physisorption
Surface of gold atoms
Coronene
a) Metal surface (adsorbent)
b) Physisorption of H2 through van der Waals interaction
c) Chemisorptions of H2 through M-H bond (metal hydrides)
d) Chemisorbed H atom may slid into the bulk metal through diffusion
Example of Chemisorption
http://cdn.intechopen.com/pdfs-wm/40231.pdf
“Chemisorption always accompanied by physisorption”
Metal hydride is formed through
chemical bonding, hence,
chemisorption.
Thermodynamic Considerations
• Adsorption (or any) spontaneous process
requires ∆G < 0. Because the translational freedom
of the adsorbate is reduced when it is adsorbed, ∆S
is negative.
• Therefore, in order for ∆G = ∆ H − T∆S to be
negative, ∆H must be negative (that is, the process is
exothermic).
• Exceptions may occur if the adsorbate dissociates
and has high translational mobility on the surface.
Enthalpies of Physi- and Chemisorption
Exothermic reactions, enthalpy change is negative
Enthalpies of chemisorption are greater than enthalpies of
physisorption. These enthalpies are close to covalent bond enthalpies.
Vs
Quantitative Models on
Adsorption
Amount of gas adsorbed on a solid depends on T and P (or
concentration of solution species) of the gas in contact with the
solid surface.
The amount of gas adsorbed on the solid surface is studied at
constant temperature.
The plot of amount of gas adsorbed as a function of pressure is
known as adsorption isotherm.
This behavior can be explained by empirical or theoretical models.
Langmuir Adsorption Isotherm
A
S (Surface of adsorbent)
1. Surface of the adsorbent is homogeneous
2. It has Nactive sites
3. The fraction of sites adsorbed θ = Na/N
4. Surface only allows the formation of monolayer
5. There is no intermolecular interaction between adsorbate
Adsorptive, A(g)
𝑜𝑟 𝜃 =
number of adsorption sites occupied
number of adsorption sites available
Adsorptionisotherms-Solid-Gasinteraction
Deriving the Langmuir isotherm
You need to consider the dynamic equilibrium between the molecules
(A) in the gas phase and those on the surface (denoted AM):
rate of adsorption
rate of desorption
At equilibrium there is no net change in θ, implying that the sum of these two rates must be
zero:
at equilibrium
p partial pressure
N is the total number of sites
Adsorptionisotherms-Solid-Gasinteraction
Deriving the Langmuir isotherm
At equilibrium there is no net change in θ, implying that the sum of these two rates must be
zero:
at equilibrium
solving for θ gives the Langmuir isotherm
( Some text books use α instead of K)
Langmuir isotherm
Adsorptionisotherms-Solid-Gasinteraction
Langmuir isotherm
Langmuir isotherm
where,
x = mass of adsorbate
m = mass of adsorbent
This model is inadequate to explain some cases of adsorption.
In certain cases the adsorption continues even
after the point of Freundlich saturation limit. (for example liquid
condensation).
Point of saturation
Adsorptionisotherms-Effectof T
Lower the T more the surface coverage (adsorption)
Continued….
kf approximately indicates adsorption capacity
1/n is a function of the strength of adsorption
n varies with the nature of the adsorbent and
range for favorable adsorption is of 1-10.
1/n = 0, x/m = constant, the adsorption is
independent of pressure.
1/n = 1, x/m = k P, i.e. x/m ∝ P, the adsorption
varies directly with pressure.
30
𝑥
𝑚
= 𝑘 𝑝
1
𝑛
Limitations of Freundlich Isotherm
Freundlich equation is purely empirical and
has no theoretical basis.
The equation is valid only upto a
certain pressure and invalid at higher
pressure.
Freundlich's adsorption isotherm fails at
high concentration of the adsorbate.
31
Differences between Freundlich and
Langmuir adsorption isotherms
32
FRENDLICH ADSORPTION
ISOTHERM
• Tells about the quantity of
gas adsorbed by unit mass
of solid adsorbent with
pressure.
• Represented by formula
x/m = KP1/n
LANGMUIR ADSORPTION
ISOTHERM
• Tells about the number
of active site undergoing
adsorption and pressure.
• Represented by formula
θ = 𝐾𝑃
1+ KP
Adsorptionisotherms-Solid-liquidinteraction
where
qe = mass of material adsorbed (at equilibrium) per mass of adsorbent, mg adsorbate/g
adsorbent
C0 = initial concentration of adsorbate, mg/L
Ce = equilibrium concentration in solution when amount adsorbed equals qe, mg/L
V = volume of liquid in the reactor, L
m = mass of adsorbent, g
mass balance equation
for adsorption
kf and n are system specific constants.
Adsorption isotherms: Freundlich isotherm
For the special case that the surface energies are heterogeneous
(particularly good for mixed adsorbates) in which the energy term,
“kF”, varies as a function of surface coverage, the Freundlich
model is appropriate.
The model equation is:
Adsorptionisotherms-Solid-liquidinteraction
𝑞𝑒 = 𝑘𝑓𝐶𝑒
1
𝑛
q
e
Ce
Shape of the Freundlich isotherm changes upon changing the
values of n and k
0
a e
e
e
K Q C
q
1 K C
 

 
0
a
Q represents the maximum adsorption capacity
(monolayer coverage) (g solute/g adsorbent).
Ce has units of mg/L
K Langmuir equilibrium constant has units of
L/mg
Adsorption isotherms: Langmuir model
This model assumes monolayer coverage and constant binding
energy between surface and adsorbate.
The model equation is:
Adsorptionisotherms-Solid-liquidinteraction
⇒ 𝐶𝑒
𝑞𝑒
=
1
𝐾𝑄𝑎
0 +
𝐶𝑒
𝑄𝑎
0
Adsorption isotherms: Langmuir model
Adsorptionisotherms-Solid-liquidinteraction
𝐶𝑒
𝑞𝑒
=
1
𝐾𝑄𝑎
0 +
𝐶𝑒
𝑄𝑎
0
Slope =
1
𝑄𝑎
0
Intercept
=
1
𝐾𝑄𝑎
0
Application of Adsorbents
• Organic contaminants such as pharmaceuticals, cosmetics,
pesticides can be removed from water using the method of
adsorption.
• To speed up chemical reactions (catalysis)
• To remove bad odor and color in water
• Used as a solid support purify proteins and chemical
compounds
• Used to remove unwanted impurities from gas
38
• Uses
Remove man-made organic chemicals
Remove miscellaneous tastes and
odor from water assuming no bacterial
problems
Remove radon gas from water
• Maintenance
Carbon must be replaced routinely
Uses of activated carbon as a adsorbent
Porous Nature of Activated Carbon
Generally activated carbon is porous. They provide large surface area
(m2/g). Pore size depends on the carbon source.
Example 1
Adsorption of benzene onto activated carbon has been reported
to obey the following Freundlich isotherm equation, where c is in
mg/L and q is in mg/g:
A solution at 25o
C containing 0.50 mg/L benzene is to be treated
in a batch process to reduce the concentration to less than
0.01 mg/L. The adsorbent is activated carbon with a specific
surface area of 650 m2/g.
Compute the required activated carbon dose.
0.533
50.1
benz benz
q c

Problems
Example 1
Solution:
𝐶0 = 0.5 𝑚𝑔/𝐿
𝐶𝑒 = 0.01 mg/L
𝑞𝑒 = ?
𝑚
𝑉
= ?
𝑞𝑒 = 𝑘 𝐶𝑒
1/𝑛
0.533
50.1
benz benz
q c

𝑞𝑒 = 50.1 (0.01)0.533
𝑞𝑒 = 4.30 𝑚𝑔/𝑔
Example 1
Solution:
𝐶0 = 0.5 𝑚𝑔/𝐿
𝐶𝑒 = 0.01 mg/L
𝑞𝑒 = 4.30 mg/g
𝑚
𝑉
= ?
𝑚
𝑣
=
𝐶0 − 𝐶𝑒
𝑞𝑒
𝑚
𝑣
=
0.5 − 0.01
4.3
𝑚
𝑣
= 0.114 g/L
mg/g
mg/L
Example 2
The data given below are for the adsorption of CO on charcoal at 273
K. Confirm that they fit the Langmuir isotherm, and find the constant
K and the volume corresponding to complete coverage.
Solution:
a plot of p/V against p should give a straight
line of slope 1/V∞ and intercept
1/KV∞.
1/Vm = 1/V∞
Example 2
Solution:
Slope =
1
𝑉∞
= 0.00900 (from graph)
𝑉
∞ = 111 𝑐𝑚3
Intercept =
1
𝐾𝑉∞
= 1.20 (from graph)
y = mx + c
Example 3
Determine the maximum P adsorption capacity of this clay
(mg P / g clay).
Example 3 Solution: 𝐶𝑒
𝑞𝑒
=
1
𝐾𝑄𝑎
0 +
𝐶𝑒
𝑄𝑎
0

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Module 2-States of mater.pptx

  • 1. CHY1009 ; Module 2 -States of mater and adsorption isotherms
  • 3. The Physical States of Matter - Particulate theory of matter Greek philosopher Democritus described matter as made up of tiny microscopic particles. the particulate theory of matter was first presented by Democritus in 400 BC Traditionally there are three states of matter
  • 4. John Dalton who is credited with first developing the modern atomic theory of matter in the early 1800s. The theory presented by Democritus was predominately a philosophical statement and therefore not widely accepted. In contrast, Dalton’s theory was based on careful experimental observations and measurements and so became the first atomic theory of matter founded on scientific concepts and principles. According to the modern atomic theory, matter can be classified according to both its physical and chemical state The Physical States of Matter - Particulate theory of matter
  • 5. The Physical States of Matter - Particulate theory of matter
  • 6. Physical States of Mater- Properties Gas Liquid Solid These characteristics affect the physical properties of matter, such as volume occupancy, density, light scattering, etc.,
  • 7. Interparticle distance decreases, this decreases volume. Density (ρ ) ∝ 1/Volume (V) Density (mass/cm3) of Gas, Liquid, Solids ρ = mass/unit volume = M/V For a given mass of substance, density increases while going from gas-to-liquid and liquid-to-solid.
  • 8. Solid (g/cm3) Liquid (g/cm3) Gas (g/cm3) Ar 1.65 1.40 0.001784 N2 1.026 0.8081 0.001251 O2 1.426 1.149 0.001429 Density (mass/cm3) of Gas, Liquid, Solids - Examples -the density of a typical solid is about 20% larger than the corresponding liquid, -while the liquid is roughly 800 times as dense as the gas.
  • 9. Plasma – 4th states of Matter • Plasma is a “superheated matter” comprised of ions formed from atoms or molecules by striping of at least one electron. • It comprises over 99% of the visible universe. • In the night sky, plasma glows in the form of stars, nebulas, and even the auroras that sometimes ripple above the north and south poles. • Plasma is often called “the fourth state of matter,” along with solid, liquid and gas.
  • 11. Adsorption isotherms Surface chemistry is the study of processes that occur at the interface of two bulk phases. Bulk phase may be a solid or liquid or gas Liquid- liquid
  • 12. Interaction Open Surfaces solid with Gases Phenomena of Adsorption Adsorbate Adsorbent Except in special cases, adsorption is an exothermic process, releases heat to the surrounding. Enthalpy change is negative ∆Had = -Ve The phenomena of interaction of a gas or liquid, or ionic species with a solid surface is referred as adsorption. Adsorptive
  • 13. Examples of Adsorption  (i) Adsorption of O2, H2, CO, Cl2, NH3 or SO2 on surface of charcoal,  (ii) In a solution of an organic dye, say methylene blue on the surface of charcoal, i.e., are adsorbed.  (iii) Aqueous solution of raw sugar, when passed over beds of animal charcoal, becomes colourless as the colouring substances are adsorbed by the charcoal.  (iv) The air becomes dry in the presence of silica gel because the water molecules get adsorbed on the surface of the gel. The process of removing an adsorbed substance from a surface on which it is adsorbed is called desorption.
  • 14. The attractive interaction can be either long range or short range 1. Long range interaction: Physical contact, due to Van der Waals force. 2. Short range interaction: Chemical bonding, such as covalent, ionic, metallic bonding What kind of bonding interaction occurs between adsorbent and adsorbate? Accordingly, the first one is called physisorption (Physical adsorption) and the second one is called chemisorption (Chemical adsorption).
  • 15. Sticking of benzene-like molecules, for example coronene, on the surface of gold (111) is an example of physisorption. Example of Physisorption Surface of gold atoms Coronene
  • 16. a) Metal surface (adsorbent) b) Physisorption of H2 through van der Waals interaction c) Chemisorptions of H2 through M-H bond (metal hydrides) d) Chemisorbed H atom may slid into the bulk metal through diffusion Example of Chemisorption http://cdn.intechopen.com/pdfs-wm/40231.pdf “Chemisorption always accompanied by physisorption” Metal hydride is formed through chemical bonding, hence, chemisorption.
  • 17. Thermodynamic Considerations • Adsorption (or any) spontaneous process requires ∆G < 0. Because the translational freedom of the adsorbate is reduced when it is adsorbed, ∆S is negative. • Therefore, in order for ∆G = ∆ H − T∆S to be negative, ∆H must be negative (that is, the process is exothermic). • Exceptions may occur if the adsorbate dissociates and has high translational mobility on the surface.
  • 18.
  • 19. Enthalpies of Physi- and Chemisorption Exothermic reactions, enthalpy change is negative Enthalpies of chemisorption are greater than enthalpies of physisorption. These enthalpies are close to covalent bond enthalpies.
  • 20. Vs
  • 21. Quantitative Models on Adsorption Amount of gas adsorbed on a solid depends on T and P (or concentration of solution species) of the gas in contact with the solid surface. The amount of gas adsorbed on the solid surface is studied at constant temperature. The plot of amount of gas adsorbed as a function of pressure is known as adsorption isotherm. This behavior can be explained by empirical or theoretical models.
  • 22.
  • 23. Langmuir Adsorption Isotherm A S (Surface of adsorbent) 1. Surface of the adsorbent is homogeneous 2. It has Nactive sites 3. The fraction of sites adsorbed θ = Na/N 4. Surface only allows the formation of monolayer 5. There is no intermolecular interaction between adsorbate Adsorptive, A(g) 𝑜𝑟 𝜃 = number of adsorption sites occupied number of adsorption sites available
  • 24. Adsorptionisotherms-Solid-Gasinteraction Deriving the Langmuir isotherm You need to consider the dynamic equilibrium between the molecules (A) in the gas phase and those on the surface (denoted AM): rate of adsorption rate of desorption At equilibrium there is no net change in θ, implying that the sum of these two rates must be zero: at equilibrium p partial pressure N is the total number of sites
  • 25. Adsorptionisotherms-Solid-Gasinteraction Deriving the Langmuir isotherm At equilibrium there is no net change in θ, implying that the sum of these two rates must be zero: at equilibrium solving for θ gives the Langmuir isotherm ( Some text books use α instead of K) Langmuir isotherm
  • 27. where, x = mass of adsorbate m = mass of adsorbent
  • 28. This model is inadequate to explain some cases of adsorption. In certain cases the adsorption continues even after the point of Freundlich saturation limit. (for example liquid condensation). Point of saturation
  • 29. Adsorptionisotherms-Effectof T Lower the T more the surface coverage (adsorption)
  • 30. Continued…. kf approximately indicates adsorption capacity 1/n is a function of the strength of adsorption n varies with the nature of the adsorbent and range for favorable adsorption is of 1-10. 1/n = 0, x/m = constant, the adsorption is independent of pressure. 1/n = 1, x/m = k P, i.e. x/m ∝ P, the adsorption varies directly with pressure. 30 𝑥 𝑚 = 𝑘 𝑝 1 𝑛
  • 31. Limitations of Freundlich Isotherm Freundlich equation is purely empirical and has no theoretical basis. The equation is valid only upto a certain pressure and invalid at higher pressure. Freundlich's adsorption isotherm fails at high concentration of the adsorbate. 31
  • 32. Differences between Freundlich and Langmuir adsorption isotherms 32 FRENDLICH ADSORPTION ISOTHERM • Tells about the quantity of gas adsorbed by unit mass of solid adsorbent with pressure. • Represented by formula x/m = KP1/n LANGMUIR ADSORPTION ISOTHERM • Tells about the number of active site undergoing adsorption and pressure. • Represented by formula θ = 𝐾𝑃 1+ KP
  • 33. Adsorptionisotherms-Solid-liquidinteraction where qe = mass of material adsorbed (at equilibrium) per mass of adsorbent, mg adsorbate/g adsorbent C0 = initial concentration of adsorbate, mg/L Ce = equilibrium concentration in solution when amount adsorbed equals qe, mg/L V = volume of liquid in the reactor, L m = mass of adsorbent, g mass balance equation for adsorption
  • 34. kf and n are system specific constants. Adsorption isotherms: Freundlich isotherm For the special case that the surface energies are heterogeneous (particularly good for mixed adsorbates) in which the energy term, “kF”, varies as a function of surface coverage, the Freundlich model is appropriate. The model equation is: Adsorptionisotherms-Solid-liquidinteraction 𝑞𝑒 = 𝑘𝑓𝐶𝑒 1 𝑛
  • 35. q e Ce Shape of the Freundlich isotherm changes upon changing the values of n and k
  • 36. 0 a e e e K Q C q 1 K C      0 a Q represents the maximum adsorption capacity (monolayer coverage) (g solute/g adsorbent). Ce has units of mg/L K Langmuir equilibrium constant has units of L/mg Adsorption isotherms: Langmuir model This model assumes monolayer coverage and constant binding energy between surface and adsorbate. The model equation is: Adsorptionisotherms-Solid-liquidinteraction ⇒ 𝐶𝑒 𝑞𝑒 = 1 𝐾𝑄𝑎 0 + 𝐶𝑒 𝑄𝑎 0
  • 37. Adsorption isotherms: Langmuir model Adsorptionisotherms-Solid-liquidinteraction 𝐶𝑒 𝑞𝑒 = 1 𝐾𝑄𝑎 0 + 𝐶𝑒 𝑄𝑎 0 Slope = 1 𝑄𝑎 0 Intercept = 1 𝐾𝑄𝑎 0
  • 38. Application of Adsorbents • Organic contaminants such as pharmaceuticals, cosmetics, pesticides can be removed from water using the method of adsorption. • To speed up chemical reactions (catalysis) • To remove bad odor and color in water • Used as a solid support purify proteins and chemical compounds • Used to remove unwanted impurities from gas 38
  • 39. • Uses Remove man-made organic chemicals Remove miscellaneous tastes and odor from water assuming no bacterial problems Remove radon gas from water • Maintenance Carbon must be replaced routinely Uses of activated carbon as a adsorbent
  • 40.
  • 41. Porous Nature of Activated Carbon Generally activated carbon is porous. They provide large surface area (m2/g). Pore size depends on the carbon source.
  • 42. Example 1 Adsorption of benzene onto activated carbon has been reported to obey the following Freundlich isotherm equation, where c is in mg/L and q is in mg/g: A solution at 25o C containing 0.50 mg/L benzene is to be treated in a batch process to reduce the concentration to less than 0.01 mg/L. The adsorbent is activated carbon with a specific surface area of 650 m2/g. Compute the required activated carbon dose. 0.533 50.1 benz benz q c  Problems
  • 43. Example 1 Solution: 𝐶0 = 0.5 𝑚𝑔/𝐿 𝐶𝑒 = 0.01 mg/L 𝑞𝑒 = ? 𝑚 𝑉 = ? 𝑞𝑒 = 𝑘 𝐶𝑒 1/𝑛 0.533 50.1 benz benz q c  𝑞𝑒 = 50.1 (0.01)0.533 𝑞𝑒 = 4.30 𝑚𝑔/𝑔
  • 44. Example 1 Solution: 𝐶0 = 0.5 𝑚𝑔/𝐿 𝐶𝑒 = 0.01 mg/L 𝑞𝑒 = 4.30 mg/g 𝑚 𝑉 = ? 𝑚 𝑣 = 𝐶0 − 𝐶𝑒 𝑞𝑒 𝑚 𝑣 = 0.5 − 0.01 4.3 𝑚 𝑣 = 0.114 g/L mg/g mg/L
  • 45. Example 2 The data given below are for the adsorption of CO on charcoal at 273 K. Confirm that they fit the Langmuir isotherm, and find the constant K and the volume corresponding to complete coverage. Solution: a plot of p/V against p should give a straight line of slope 1/V∞ and intercept 1/KV∞. 1/Vm = 1/V∞
  • 46. Example 2 Solution: Slope = 1 𝑉∞ = 0.00900 (from graph) 𝑉 ∞ = 111 𝑐𝑚3 Intercept = 1 𝐾𝑉∞ = 1.20 (from graph) y = mx + c
  • 47. Example 3 Determine the maximum P adsorption capacity of this clay (mg P / g clay).
  • 48. Example 3 Solution: 𝐶𝑒 𝑞𝑒 = 1 𝐾𝑄𝑎 0 + 𝐶𝑒 𝑄𝑎 0