SlideShare a Scribd company logo
1 of 63
Associate Professor & Head , Department of Chemistry
SAIVA BHANU KSHATRIYA COLLEGE
ARUPPUKOTTAI - 626101
Virudhunagar District, Tamil Nadu, India
ATOMIC STRUCTURE AND PERIODIC TABLE
The important postulates of Bohrโ€™s theory about the atom model are
1. The electron in an atom revolve around the nucleus only in certain selected circular
orbits
2. Each orbits is associated with definite energy and therefore, they are also known as
energy levels or energy shells
3. As long as the electron remains in a particular orbit, it neither loses nor gains energy,
i.e., the energy of an electron remains constant in a particular orbit
THE BOHRโ€™S MODEL OF THE ATOM
4. The energy levels are defined by principal quantum numbers (n = 1,2,3,4,, etc..)
starting from the nucleus and also designated by letters K, L, M, N etc.,
THE BOHRโ€™S MODEL OF THE ATOM
5. The farther the energy level from the nucleus, the greater in the energy associated with it
6. The energy of an electron cannot change continuously. It changes only as the electron jumps
from one energy level to another
7. The angular momentum of an electron moving round the nucleus is quantized i.e.,
the angular momentum of an electron in an atom can have only definite (or) discrete
values given by the expression
Angular momentum =
๐‘›โ„Ž
2๐œ‹
where n is any integer (1,2,3, etc.,)
i.e., the angular momentum of an electron may be
โ„Ž
2๐œ‹
or a simple whole number
multiple of
โ„Ž
2๐œ‹
such as
2โ„Ž
2๐œ‹
,
3โ„Ž
2๐œ‹
, โ€ฆโ€ฆ
๐‘›โ„Ž
2๐œ‹
THE BOHRโ€™S MODEL OF THE ATOM
โ€ข Electron revolves around the nucleus of an atom in elliptical orbits adding to circular orbit
โ€ข There is a major axes and an minor axes having different length when electron revolves in
elliptical orbits
SOMERFIELD - BOHR ATOM MODEL
According to Somerfield โ€“ Bohr atom model
โ€ข The principal quantum number (n) and azimuthal quantum number (k) are related as
๐‘›
๐‘˜
=
๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž ๐‘œ๐‘“ ๐‘š๐‘Ž๐‘—๐‘œ๐‘Ÿ ๐‘Ž๐‘ฅ๐‘’๐‘ 
๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž ๐‘œ๐‘“ ๐‘š๐‘–๐‘›๐‘œ๐‘Ÿ ๐‘Ž๐‘ฅ๐‘’๐‘ 
โ€ข When length of major axes is equal to length of minor axes, then k = n, i.e., the electron
orbit must be circular
โ€ข But, as k becomes smaller ( k < n ), the orbit become elliptical with greater and greater
eccentricity
โ€ข The number of possible value of k is equal to the principal quantum
number (n). i.e., for n = 4 , k can have four values as
shown in the diagram
SOMERFIELD - BOHR ATOM MODEL
โ€ข As the orbit broadens, the length of the two axes become closer and become equal when the
orbit become circular
โ€ข The angular momentum of the electrons revolving in an elliptical orbit is equal to
๐‘˜โ„Ž
2๐œ‹
, where
k is the azimuthal quantum number
โ€ข The energy of an electron depends not only principal quantum number but also azimuthal
quantum number
SOMERFIELD BOHR ATOM MODEL
โ€ข de-Broglie stated that electron can travel (X-ray) as wave and as particle. This character
is known as dual character
Derivation of de-Broglie wave equation :
โ€ข According to Einstein, the energy of an electron (X- ray) is
E = mc2 ---------(1)
Where m ------ mass of the electron
c ------ velocity of electron
โ€ข According to Plank's , the energy of light radiation (X-ray) is
E = h๏ฎ ----------(2)
Where h ------- Plankโ€™s constant
๏ฎ ------- Frequency of light radiation
de โ€“ BROGLIE DUAL NATURE OF ELECTRON
โ€ข Equating equation (1) and (2), we get
mc2 = h๏ฎ ---------(3)
โ€ข Substitute ๏ฎ =
๐‘
๏ฌ
in equation (3), we get
mc2 = h
๐‘
๏ฌ
mc =
โ„Ž
๏ฌ
๏ฌ =
โ„Ž
๐‘š๐‘
This equation is known as de โ€“ Broglie wave equation
de โ€“ BROGLIE WAVE PARTICLE CONCEPT FOR ELECTRON
โ€ข The behavior of electron waves in atoms and molecules is described by the Schrรถdinger wave
equation
SCHRODINGER WAVE EQUATION
Where
ฯˆ is the wave function of electron
E is the total energy of electron
V is the potential energy of electron
E-V is the kinetic energy of the electron
h is the Plankโ€™s constant
Physical significance of the wave function:
1. The wave function ฮจ has no direct physical meaning. It is a complex quality representing
the variation of a matter wave
2. The wave function ฮจ (r,t) describes the position of a particle with respect to time
3. It can be considered as โ€˜probability amplitudeโ€™ since it is used to find the location of
the particle
SCHRODINGER WAVE EQUATION
Definition: Quantum numbers are the numbers which are used to describe completely the
state of electrons in an atom.
Four types of quantum numbers
โ€ข Principal quantum number, denoted by n
โ€ข Azimuthal quantum number, denoted by l
โ€ข Magnetic quantum number, denoted by m
โ€ข Electron spin quantum number, denoted by s
QUANTUM NUMBERS
โ€ข Principal quantum numbers describe the size and energy
level or shell of electron in an atom . It is denoted by โ€˜nโ€™
โ€ข And also describe the distance between the electron and the
nucleus i.e., larger the value of principle quantum number,
greater the distance between electron and the nucleus
โ€ข The value of the principal quantum number might be any
equal to or greater than one. i.e., n = 1,2,3,โ€ฆ.
โ€ข The value n=1 denotes the innermost electron shell of an
atom, which corresponds to the lowest energy state of an
electron and as the n value increases the energy level
increases
PRINCIPLE QUANTUM NUMBER (n)
โ€ข The azimuthal quantum number describes the sub energy level
or subshell of the electron in an atom and also describe the
shape of the electron clouds around the nucleus of an atom. It
is denoted by โ€˜lโ€™
โ€ข This value depends on the value of the principal quantum
number, i.e. the value of the azimuthal quantum number
ranges between 0 and (n-1).
โ€ข For example, if n =3, the azimuthal quantum number are 0,1
and 2. When l=0, the resulting subshell is an โ€˜sโ€™ subshell.
Similarly, when l=1 and l=2, the resulting subshells are โ€˜pโ€™ and
โ€˜dโ€™ subshells (respectively). Therefore, when n=3, the three
possible subshells are 3s, 3p, and 3d.
AZIMUTHAL QUANTUM NUMBER (l)
โ€ข Magnetic quantum number describe the total number of
orbitals in a subshell and the orientation of these orbitals. It
is denoted by โ€˜mโ€™.
โ€ข The value of the magnetic quantum number is dependent
on the value of the azimuthal quantum number.
โ€ข For a given value of l, the value of m ranges between the
interval -l to +l.
โ€ข For example, if l = 1 in an atom, the possible values of the
magnetic quantum number are -1, 0, +1 and the orbitals are
named as px, py and pz
MAGNETIC QUANTUM NUMBER (m)
ELECTRON SPIN QUANTUM NUMBER (s)
โ€ข The electron spin quantum number describe the spinning
nature of the electron which are revolving around the nucleus
of an atom. It is denoted by โ€˜sโ€™
โ€ข The possible values of the electron spin quantum number are
+ยฝ and -ยฝ.
โ€ข The positive value of s implies an upward spin on the electron
which is also called โ€˜spin upโ€™ and is denoted by the symbol โ†‘.
โ€ข The negative value of s implies a downward spin on the
electron which is also called โ€˜spin downโ€™ and is denoted by
the symbol โ†“.
Name and Symbol Meaning and Possible Values
Principal quantum number, n Electron shell, n โ‰ฅ 1
Azimuthal quantum number, l Subshells (s=0, p=1, etc.) , (n-1) โ‰ฅ l โ‰ฅ 0
Magnetic quantum number, ml
Total number and orientation of orbitals,
l โ‰ฅ ml โ‰ฅ -l
Electron spin quantum number, ms The direction of electron spin, ms = ยฑยฝ
SUMMARY OF QUANTUM NUMBER
AUFBAU PRINCIPLE
โ€ข Aufbau principle states that the orbitals are
filled in the order of their increasing
energies. That is the electrons first occupy
the lowest energy orbital available to them.
Once the lower energy orbitals are
completely filled, then the electrons enter
the next higher energy orbitals.
HUNDโ€™S RULE
โ€ข Hundโ€™s rule state that electron pairing in any orbital is not possible until all the
available orbitals of a given subshell contains one electron each (half filled )
Eg: FOR NITROGEN ATOM
PAULIโ€™S EXCLUSION PRINCIPLE
โ€ข Pauli Exclusion Principle states that no two electrons can be identified by the
same set of quantum numbers and the orbital can accommodate only two electrons
with opposite spin
For helium atom the electronic configuration is 1s2
The quantum numbers for the first and second electron are
First electron : n = 1, l = 0, m = 0 & s = + ยฝ
Second electron: n = 1, l = 0, m = 0 & s = - ยฝ
MODERN PERIODIC LAW
The modern periodic law states that the properties of the elements are a periodic
function of their atomic numbers
i.e., the elements are arranged in an increasing order of their atomic number in the periodic
table
โ€ข Repetition of properties of elements in the periodic table after a certain interval
is called periodicity of properties.
โ€ข If elements are arranged in increasing order of their atomic number in the periodic table,
then elements repeat their properties after a definite interval
PERIODICITY IN PROPERTIES
PERIODIC PROPERTIES OF THE ELEMENTS
1. Atomic radii
2. Ionization energy
3. Electron affinity
4. Electronegativity
ATOMIC RADII
ATOMIC RADII IN GROUP
ATOMIC RADII IN PERIOD
IONIZATION ENERGY
IONIZATION ENERGY IN GROUP
IONIZATION ENERGY IN PERIOD
FIRST IONIZATION ENERGY
ELECTRON AFFINITY
H1
H2
โˆ†H = H2 โ€“ H1 = Electron affinity
Where
H1 is the energy of neutral chlorine atom
H2 is the energy of chloride ion
ELECTRON AFFINITY IN GROUP
Down the group in periodic table electron affinity decreases
because of the addition of new shell to each atom decreases is
force of attraction
ELECTRON AFFINITY IN PERIOD
In period the electron affinity increases from left to right
because successive atoms have higher nuclear charge and attract the
incoming electrons more towards itself
ELECTRONEGATIVITY
NON POLAR POLAR
ELECTRONEGATIVITY IN GROUP
ELECTRONEGATIVITY IN PERIOD
ELECTRONEGATIVITY SCALE
โ€ข There are three quantitative scales used to evaluate electronegativity of an element
1. Pauling scale
2. Mulliken scale
3. Allred and Rochow scale
PAULING SCALE
โ€ข Pauling derived an electronegativity scale based on experimentally derived values of
bond energies
โ€ข According to Pauling, Bond energy of a compound A-B for pure covalency is a
geometric mean of the bond energies of A-A and B-B
i.e., Bond energy for pure covalency = [D A-A x D B-B ]1/2
โ€ข But actual experimental value D A-B is found to be greater than this expected value
i.e., D A-B (experimental) - [D A-A x D B-B ]1/2 = โˆ†โ€ฒ
โ€ข The difference, โˆ†โ€ฒ is due to electronegativity differences between the atoms.
i.e., the electronegativity difference (XB โ€“ XA) is directly proportional to
(XB โ€“ XA) ๏‚ต โˆ†โ€ฒ
(XB โ€“ XA) = k โˆ†โ€ฒ
PAULING SCALE
โ€ข Where XB is the electronegativity of B
XA is the electronegativity of A
k is the proportionality constant
โ€ข When โˆ†โ€ฒ is zero, Bonding electrons are shared equally i.e., the electronegativity of
A and B atoms are same
โ€ข In general, smaller atoms attract electron more than larger ones and therefore
more electronegative
โ€ข Atoms with nearly filled shells of electrons (example : halogens) will tends to have
higher electronegativity than those with not filled shells
MULLIKEN SCALE
โ€ข According to Mulliken, the electronegativity of an element is the arithmetic mean of
first ionization energy which measures its tendency to hold its own outer electrons,
and its electron affinity which measures its tendency to attract electron of the element
bonded with it
Electronegativity of an element =
๐‘ญ๐’Š๐’“๐’”๐’• ๐’Š๐’๐’๐’Š๐’”๐’•๐’‚๐’Š๐’๐’ ๐’†๐’๐’†๐’“๐’ˆ๐’š+๐‘ฌ๐’๐’†๐’„๐’•๐’“๐’๐’ ๐’‚๐’‡๐’‡๐’Š๐’๐’Š๐’•๐’š
๐Ÿ
โ€ข The Mulliken (M) and Pauling (P) values are related approximately as
XM
B โ€“ XM
A = 2.78 (XP
B - XP
A)
ALLRED AND ROCHOW SCALE
โ€ข Allred and Rochow defined electronegativity as the electrostatic force exerted
by the nucleus on the valence electrons
โ€ข According to them
Electronegativity = 0.359
๐’
โˆ—
๐’“๐Ÿ+ 0.744
where Z* is the effective nuclear charge experienced by the electron
r is the mean radius of the orbital which can be taken equal to the covalent
radius of the atom (in A0)
EFFECTIVE NUCLEAR CHARGE
Definition
โ€ข The effective nuclear charge is the net positive charge experienced by valence electrons.
Slater proposed a formula for calculating the effective nuclear charge
Zeff = Z โ€“ S
where
Zeff is the effective nuclear charge
Z is the atomic number
S is the shielding constant
โ€ข Shielding electrons are the inner shell electrons
which are blocking the valence shell
electron attraction by the nucleus
First Inner shell
Valence shell
Second Inner shell
SLATER RULE
โ€ข Slater formulated the following rules for calculating the screening constant value for
various inner shell electrons for obtaining effective nuclear charge
SLATER RULE
SLATER RULE
SLATER RULE EXAMPLE
APPLICATION OF SLATER RULE
APPLICATION OF SLATER RULE
APPLICATION OF SLATER RULE
APPLICATION OF SLATER RULE
APPLICATION OF SLATER RULE
APPLICATION OF SLATER RULE
APPLICATION OF SLATER RULE
POLARIZING POWER
Definition
โ€ข Polarizing power can be defined as the ability of a cation to attract the electron cloud
towards itself. Polarising power is proportional to charge/size.
DIAGONAL RELATIONSHIP
ANOMALOUS BEHAVIOUR OF FIRST ELEMENT IN A GROUP
โ€ข The anomalous behaviour of first element of s and p block elements of each group
as compared to other group members is due to following reasons:
1. Small size of atom
2. Large charge/radius ratio,
3. High electronegativity
4. Non availability of d-orbitals in their valence shell
BALANCING OF REDOX EQUATION
Reduction
โ€ข Gain of electron is called reduction
Oxidation
โ€ข Loss of electron is called oxidation
Redox reaction
โ€ข Both gain and loss of electron occur in the chemical reaction is called redox reaction
Zn โ†’ Zn2+ + 2e-
Cu2+ + 2e- โ†’ Cu
4Zn + 10 HNO3 โ†’ 4Zn(NO3)2 + N2O + 5H2O
โ€ข Here Zinc is oxidized from zero state to +2 state and nitrogen is reduced from
+5 state to +2 state
BALANCING OF REDOX EQUATION
There are two methods used for balancing the redox equation
1. Oxidation number method
2. Ion โ€“ electron method
Oxidation Method : Rules
1. Assign oxidation number to the atom that shows changes
2. Balance the total number of atoms undergoing the changes in oxidation state
3. Count the total number of electrons gained and lost respectively by the oxidizing agent
and reducing agent
4. Chose the proper ratio of oxidizing agent to the reducing agent so that the oxidation
number change is balanced
5. Make appropriate change in the coefficient of the products corresponding to the change
of coefficients in step 4
6. Balance the oxygen atom on bot sides by adding H2O to the side that is deficient in
oxygen
BALANCING OF REDOX EQUATION
7. Balance the hydrogen atoms on both sides by adding H+ to the side that is deficient in
hydrogen
8. The equation is balanced if the reaction taking place in acidic solution. If , however the
reaction proceeds in basic solution, add sufficient number of OH- to get rid of H+ but
add equal number of OH- on both side
BALANCING OF REDOX EQUATION
Example : Write the balanced equation for
Cr2O7
2- + Fe2+ + H+ โ†’ Cr3+ + Fe3+ +H2O
Solution:
1) Writing the skeleton equation
Cr2O7
2- + Fe2+ + H+ โ†’ 2Cr3+ + Fe3+ +H2O
2) Marking reducing agent and oxidizing agent. In this equation oxidation state of Fe2+ is raised to Fe3+
Therefore it is reducing agent. The oxidation state of Cr in Cr2O7
2- is reduced from -6 to +3. Hence
it is an oxidizing agent
3) Writing half reaction for oxidation of reducing agent (Fe3+) taking care of
balancing of atoms of Fe and the charge
Fe2+ โ†’ Fe3+ + e- ------------(1)
There are no oxygen or hydrogen atoms attached with the species. So question
of balancing them does not arise
BALANCING OF REDOX EQUATION
4) Writing other half reaction for reduction of oxidizing agent () while balancing
i) Cr and ii) O by adding H+ ions on the oxygen exceeding side and iii) charge
by adding electrons as
Cr2O7
2- + 14 H+ + 6e- โ†’ 2Cr3+ + 7H2O ------------(2)
5) To equalize the number of electrons
6) Multiplying the half reaction (1) by 6 and adding to the half reaction (2)
6Fe2+ โ†’ 6Fe3+ +6 e-
Cr2O7
2- + 14 H+ + 6e- โ†’ 2Cr3+ + 7H2O
Cr2O7
2- + 14 H+ + 6 Fe2+ โ†’ 2Cr3+ + 6 Fe3+ 7H2O
BALANCING OF REDOX EQUATION
Ion โ€“ Electron Method : Rules
1. Write the skeleton equation, showing oxidation state of the elements undergoing a change
in oxidation state
2. Mark the reducing agent ( having the atom whose oxidation number is raised) and also
the oxidizing agent ( one having the atom whose oxidation number is lowered)
3. Write down one half reaction for oxidation of the reducing agent balancing
i) the number of atoms undergoing the change in oxidation state
ii) the oxygen atoms on the two sides by adding H2O to the side deficient in oxygen or
H+ ions to the side with excess of oxygen
iii) the charge by putting the required number of electrons on R.H.S
BALANCING OF REDOX EQUATION
4. In a similar manner write down the other half of the reaction for reduction of the oxidizing
agent. To balance the charge electron would now be added on the L.H.S
5. Add these two balanced half โ€“ reactions in such a way that the electrons appearing on the
right of one half-reaction and on the left of the other cancel. For this each half-reaction will
be multiplied by appropriate numbers before addition
6. If the reaction proceeds in basic solution, add enough OH- on both sides of the half-reaction
to get rid of H+ appearing there. Combine H+ and OH- to give H2O and remove H2O
duplication
BALANCING OF REDOX EQUATION
Example: Write the balanced equation for
Zn + HNO3 โ†’ Zn2+ + N2O + 4H2O
Solution:
1. Assigning oxidation state to atoms that shows change in oxidation state and balancing number
of atoms balancing number of atoms showing this change on both sides (Zn and N atoms)
Zn + 2HNO3 โ†’ Zn + N2O + H2O -------------(1)
โ†“ โ†‘
2e- 4e-
2. Equalizing electrons lost = electron gained
Total number of electrons lost by one Zn = 1 x 2 = 2
Total number of electrons gained by two N atoms = 2 x 4 = 8
To equalize the electrons lost = electrons gained, we multiply Zn by 4 and 2HNO3 by 1.
4Zn + 2HNO3 โ†’ 4Zn 2+ + N2O + H2O -------------(2)
BALANCING OF REDOX EQUATION
3. Balancing O-atom, the number of O atoms on right hand side is 2 while on left hand side is 6.
To balance O-atoms, add 4H2O on R.H.S
4Zn + 2HNO3 โ†’ 4Zn 2+ + N2O + 5H2O -------------(3)
4. Balancing H-atoms, in equation (3) the number of H-atoms is 8 more on R.H.S than their
number on L.H.S . Add 8H+ ions on L.H.S. By doing so the charge on both sides also
balanced.
4Zn + 2HNO3 + 8H+ โ†’ 4Zn 2+ + N2O + 5H2O
(or) 4Zn + 2NO-
3 + 10H+ โ†’ 4Zn 2+ + N2O + 5H2O
BALANCING OF REDOX EQUATION
โ€ข If however it is desired to have 4Zn(NO3)2 instead of 4Zn2+ on R.H.S, we can do so by
adding 8NO3
- ions on both sides
4Zn + 2H+ +2NO-
3 + 8H+ + 8NO3
- โ†’ 4Zn2+ + 8NO3
- + N2O + 5H2O
then the molecular equation is
4Zn + 10HNO3 โ†’ 4Zn (NO3)2 + N2O + 5H2O
BALANCING OF REDOX EQUATION
ATOMIC STRUCTURE AND PERIODIC TABLE

More Related Content

What's hot

Shape Of Orbitals
Shape  Of  OrbitalsShape  Of  Orbitals
Shape Of Orbitalspallavicute
ย 
Ionization energy
Ionization energyIonization energy
Ionization energyBianca Mangin
ย 
Periodic properties
Periodic propertiesPeriodic properties
Periodic propertiesLALIT SHARMA
ย 
Mo theory
Mo theoryMo theory
Mo theorybapu thorat
ย 
Lecture 14 maxwell-boltzmann distribution. heat capacities
Lecture 14   maxwell-boltzmann distribution. heat capacitiesLecture 14   maxwell-boltzmann distribution. heat capacities
Lecture 14 maxwell-boltzmann distribution. heat capacitiesAlbania Energy Association
ย 
Atomic radius ppt for chem
Atomic radius ppt for chemAtomic radius ppt for chem
Atomic radius ppt for chemroblmcca13
ย 
Rotational Spectra : Microwave Spectroscopy
Rotational Spectra : Microwave SpectroscopyRotational Spectra : Microwave Spectroscopy
Rotational Spectra : Microwave SpectroscopyKhemendra shukla
ย 
Transuranic elements
Transuranic elementsTransuranic elements
Transuranic elementsRamesh Pi
ย 
Quantum numbers
Quantum numbersQuantum numbers
Quantum numbersKris Ann Ferrer
ย 
Bent rule
Bent ruleBent rule
Bent ruleAman Kumar
ย 
Lanthanide Chemistry
Lanthanide ChemistryLanthanide Chemistry
Lanthanide ChemistryAnik Mal
ย 
S & p block elements
S & p block elementsS & p block elements
S & p block elementsSidra Javed
ย 
Magnetic properties of transition metal complexes
Magnetic properties of transition metal complexesMagnetic properties of transition metal complexes
Magnetic properties of transition metal complexesPAYELMAITY1
ย 
Bonding Theories in Chemistry
Bonding Theories in ChemistryBonding Theories in Chemistry
Bonding Theories in ChemistryChris Sonntag
ย 
PPT Partition function.pptx
PPT Partition function.pptxPPT Partition function.pptx
PPT Partition function.pptxSharayuThorat
ย 
P โ€“ block elements 12 Classes
P โ€“ block elements 12 ClassesP โ€“ block elements 12 Classes
P โ€“ block elements 12 ClassesLOURDU ANTHONI
ย 
Valence shell electron pair repulsion theory (VSEPR THEORY)
Valence shell electron pair repulsion theory (VSEPR THEORY)Valence shell electron pair repulsion theory (VSEPR THEORY)
Valence shell electron pair repulsion theory (VSEPR THEORY)Altamash Ali
ย 
Organometallic compounds
Organometallic compoundsOrganometallic compounds
Organometallic compoundsArvind Singh Heer
ย 
Effect of isotopic subsitution on the transition frequencies
Effect of isotopic subsitution on the transition frequenciesEffect of isotopic subsitution on the transition frequencies
Effect of isotopic subsitution on the transition frequenciesApurvaSachdeva
ย 

What's hot (20)

Vsepr theory
Vsepr theoryVsepr theory
Vsepr theory
ย 
Shape Of Orbitals
Shape  Of  OrbitalsShape  Of  Orbitals
Shape Of Orbitals
ย 
Ionization energy
Ionization energyIonization energy
Ionization energy
ย 
Periodic properties
Periodic propertiesPeriodic properties
Periodic properties
ย 
Mo theory
Mo theoryMo theory
Mo theory
ย 
Lecture 14 maxwell-boltzmann distribution. heat capacities
Lecture 14   maxwell-boltzmann distribution. heat capacitiesLecture 14   maxwell-boltzmann distribution. heat capacities
Lecture 14 maxwell-boltzmann distribution. heat capacities
ย 
Atomic radius ppt for chem
Atomic radius ppt for chemAtomic radius ppt for chem
Atomic radius ppt for chem
ย 
Rotational Spectra : Microwave Spectroscopy
Rotational Spectra : Microwave SpectroscopyRotational Spectra : Microwave Spectroscopy
Rotational Spectra : Microwave Spectroscopy
ย 
Transuranic elements
Transuranic elementsTransuranic elements
Transuranic elements
ย 
Quantum numbers
Quantum numbersQuantum numbers
Quantum numbers
ย 
Bent rule
Bent ruleBent rule
Bent rule
ย 
Lanthanide Chemistry
Lanthanide ChemistryLanthanide Chemistry
Lanthanide Chemistry
ย 
S & p block elements
S & p block elementsS & p block elements
S & p block elements
ย 
Magnetic properties of transition metal complexes
Magnetic properties of transition metal complexesMagnetic properties of transition metal complexes
Magnetic properties of transition metal complexes
ย 
Bonding Theories in Chemistry
Bonding Theories in ChemistryBonding Theories in Chemistry
Bonding Theories in Chemistry
ย 
PPT Partition function.pptx
PPT Partition function.pptxPPT Partition function.pptx
PPT Partition function.pptx
ย 
P โ€“ block elements 12 Classes
P โ€“ block elements 12 ClassesP โ€“ block elements 12 Classes
P โ€“ block elements 12 Classes
ย 
Valence shell electron pair repulsion theory (VSEPR THEORY)
Valence shell electron pair repulsion theory (VSEPR THEORY)Valence shell electron pair repulsion theory (VSEPR THEORY)
Valence shell electron pair repulsion theory (VSEPR THEORY)
ย 
Organometallic compounds
Organometallic compoundsOrganometallic compounds
Organometallic compounds
ย 
Effect of isotopic subsitution on the transition frequencies
Effect of isotopic subsitution on the transition frequenciesEffect of isotopic subsitution on the transition frequencies
Effect of isotopic subsitution on the transition frequencies
ย 

Similar to ATOMIC STRUCTURE AND PERIODIC TABLE

ELECTRONIC STRUCTURE OF ATOMS AND PERIODICITY (STU).pptx
ELECTRONIC STRUCTURE OF ATOMS AND PERIODICITY (STU).pptxELECTRONIC STRUCTURE OF ATOMS AND PERIODICITY (STU).pptx
ELECTRONIC STRUCTURE OF ATOMS AND PERIODICITY (STU).pptxiftinanwafiyah
ย 
Chemistry teaching
Chemistry teachingChemistry teaching
Chemistry teachingsujathanellore
ย 
Atomic Scvgggggggytttttttttyyytructure.pptx
Atomic Scvgggggggytttttttttyyytructure.pptxAtomic Scvgggggggytttttttttyyytructure.pptx
Atomic Scvgggggggytttttttttyyytructure.pptxehtesamzunnuryn
ย 
Chemistry-Presentation.pptx
Chemistry-Presentation.pptxChemistry-Presentation.pptx
Chemistry-Presentation.pptxJulimarCabaya
ย 
Ch. 6 Electronic Structure of Atoms
Ch. 6 Electronic Structure of AtomsCh. 6 Electronic Structure of Atoms
Ch. 6 Electronic Structure of Atomsewalenta
ย 
AP Chemistry Chapter 6 Outline
AP Chemistry Chapter 6 OutlineAP Chemistry Chapter 6 Outline
AP Chemistry Chapter 6 OutlineJane Hamze
ย 
Ch06 outline
Ch06 outlineCh06 outline
Ch06 outlineAP_Chem
ย 
Atomic Structures - Dr. Mahbub.pptx
Atomic Structures - Dr. Mahbub.pptxAtomic Structures - Dr. Mahbub.pptx
Atomic Structures - Dr. Mahbub.pptxNaymulHasan1
ย 
Adv chem chapt 7
Adv chem chapt 7Adv chem chapt 7
Adv chem chapt 7bobcatchemistry
ย 
Electronic structure of the atom
Electronic structure of the atomElectronic structure of the atom
Electronic structure of the atomRaphaelZuela
ย 
bohrsmodelforhydrogenatom-141216074739-conversion-gate02.pdf
bohrsmodelforhydrogenatom-141216074739-conversion-gate02.pdfbohrsmodelforhydrogenatom-141216074739-conversion-gate02.pdf
bohrsmodelforhydrogenatom-141216074739-conversion-gate02.pdfSachinSachinKumar4
ย 
Bohrsmodelforhydrogenatom 141216074739-conversion-gate02
Bohrsmodelforhydrogenatom 141216074739-conversion-gate02Bohrsmodelforhydrogenatom 141216074739-conversion-gate02
Bohrsmodelforhydrogenatom 141216074739-conversion-gate02Rajat Jain
ย 
Structure of atom plus one focus area notes
Structure of atom plus one focus area notesStructure of atom plus one focus area notes
Structure of atom plus one focus area notessaranyaHC1
ย 
Electrons in atoms notes
Electrons in atoms notesElectrons in atoms notes
Electrons in atoms notesmartykilroy
ย 
202006151236284892NK-Bohr Model of Hydrogen Atom.pdf
202006151236284892NK-Bohr Model of Hydrogen Atom.pdf202006151236284892NK-Bohr Model of Hydrogen Atom.pdf
202006151236284892NK-Bohr Model of Hydrogen Atom.pdfsasukekun12
ย 

Similar to ATOMIC STRUCTURE AND PERIODIC TABLE (20)

ELECTRONIC STRUCTURE OF ATOMS AND PERIODICITY (STU).pptx
ELECTRONIC STRUCTURE OF ATOMS AND PERIODICITY (STU).pptxELECTRONIC STRUCTURE OF ATOMS AND PERIODICITY (STU).pptx
ELECTRONIC STRUCTURE OF ATOMS AND PERIODICITY (STU).pptx
ย 
Quantum no.ppt
Quantum no.pptQuantum no.ppt
Quantum no.ppt
ย 
Chemistry teaching
Chemistry teachingChemistry teaching
Chemistry teaching
ย 
Quantum Chemistry
Quantum ChemistryQuantum Chemistry
Quantum Chemistry
ย 
Atomic Scvgggggggytttttttttyyytructure.pptx
Atomic Scvgggggggytttttttttyyytructure.pptxAtomic Scvgggggggytttttttttyyytructure.pptx
Atomic Scvgggggggytttttttttyyytructure.pptx
ย 
Chemistry-Presentation.pptx
Chemistry-Presentation.pptxChemistry-Presentation.pptx
Chemistry-Presentation.pptx
ย 
Ch. 6 Electronic Structure of Atoms
Ch. 6 Electronic Structure of AtomsCh. 6 Electronic Structure of Atoms
Ch. 6 Electronic Structure of Atoms
ย 
AP Chemistry Chapter 6 Outline
AP Chemistry Chapter 6 OutlineAP Chemistry Chapter 6 Outline
AP Chemistry Chapter 6 Outline
ย 
Ch06 outline
Ch06 outlineCh06 outline
Ch06 outline
ย 
Atomic Structures - Dr. Mahbub.pptx
Atomic Structures - Dr. Mahbub.pptxAtomic Structures - Dr. Mahbub.pptx
Atomic Structures - Dr. Mahbub.pptx
ย 
Adv chem chapt 7
Adv chem chapt 7Adv chem chapt 7
Adv chem chapt 7
ย 
Electronic structure of the atom
Electronic structure of the atomElectronic structure of the atom
Electronic structure of the atom
ย 
Bell301
Bell301Bell301
Bell301
ย 
bohrsmodelforhydrogenatom-141216074739-conversion-gate02.pdf
bohrsmodelforhydrogenatom-141216074739-conversion-gate02.pdfbohrsmodelforhydrogenatom-141216074739-conversion-gate02.pdf
bohrsmodelforhydrogenatom-141216074739-conversion-gate02.pdf
ย 
Bohrsmodelforhydrogenatom 141216074739-conversion-gate02
Bohrsmodelforhydrogenatom 141216074739-conversion-gate02Bohrsmodelforhydrogenatom 141216074739-conversion-gate02
Bohrsmodelforhydrogenatom 141216074739-conversion-gate02
ย 
Structure of atom plus one focus area notes
Structure of atom plus one focus area notesStructure of atom plus one focus area notes
Structure of atom plus one focus area notes
ย 
Electrons in atoms notes
Electrons in atoms notesElectrons in atoms notes
Electrons in atoms notes
ย 
Chem chapt 5
Chem chapt 5Chem chapt 5
Chem chapt 5
ย 
202006151236284892NK-Bohr Model of Hydrogen Atom.pdf
202006151236284892NK-Bohr Model of Hydrogen Atom.pdf202006151236284892NK-Bohr Model of Hydrogen Atom.pdf
202006151236284892NK-Bohr Model of Hydrogen Atom.pdf
ย 
Atom1
Atom1Atom1
Atom1
ย 

More from Saiva Bhanu Kshatriya College, Aruppukottai.

POTENTIAL ENERGY SURFACE. KINETIC ISOTOPE EFFECT AND THEORIES OF UNI MOLECULA...
POTENTIAL ENERGY SURFACE. KINETIC ISOTOPE EFFECT AND THEORIES OF UNI MOLECULA...POTENTIAL ENERGY SURFACE. KINETIC ISOTOPE EFFECT AND THEORIES OF UNI MOLECULA...
POTENTIAL ENERGY SURFACE. KINETIC ISOTOPE EFFECT AND THEORIES OF UNI MOLECULA...Saiva Bhanu Kshatriya College, Aruppukottai.
ย 

More from Saiva Bhanu Kshatriya College, Aruppukottai. (20)

NMR.pptx
NMR.pptxNMR.pptx
NMR.pptx
ย 
Thermodynamics introduction
Thermodynamics introductionThermodynamics introduction
Thermodynamics introduction
ย 
NUCLEAR QUADRUPOLE RESONANCE SPECTROSCOPY
NUCLEAR QUADRUPOLE RESONANCE SPECTROSCOPY NUCLEAR QUADRUPOLE RESONANCE SPECTROSCOPY
NUCLEAR QUADRUPOLE RESONANCE SPECTROSCOPY
ย 
Quantum mechanics I
Quantum mechanics IQuantum mechanics I
Quantum mechanics I
ย 
POTENTIAL ENERGY SURFACE. KINETIC ISOTOPE EFFECT AND THEORIES OF UNI MOLECULA...
POTENTIAL ENERGY SURFACE. KINETIC ISOTOPE EFFECT AND THEORIES OF UNI MOLECULA...POTENTIAL ENERGY SURFACE. KINETIC ISOTOPE EFFECT AND THEORIES OF UNI MOLECULA...
POTENTIAL ENERGY SURFACE. KINETIC ISOTOPE EFFECT AND THEORIES OF UNI MOLECULA...
ย 
ELECTROCHEMISTRY - ELECTRICAL DOUBLE LAYER
ELECTROCHEMISTRY - ELECTRICAL DOUBLE LAYERELECTROCHEMISTRY - ELECTRICAL DOUBLE LAYER
ELECTROCHEMISTRY - ELECTRICAL DOUBLE LAYER
ย 
Thermodynamics II
Thermodynamics IIThermodynamics II
Thermodynamics II
ย 
Electrochemistry
ElectrochemistryElectrochemistry
Electrochemistry
ย 
Alkenes and alkynes
Alkenes and alkynesAlkenes and alkynes
Alkenes and alkynes
ย 
Thermodynamics i
Thermodynamics iThermodynamics i
Thermodynamics i
ย 
Thermodynamic of equilibria
Thermodynamic of equilibria Thermodynamic of equilibria
Thermodynamic of equilibria
ย 
Ideal solution
Ideal solutionIdeal solution
Ideal solution
ย 
Thermodynamics III
Thermodynamics IIIThermodynamics III
Thermodynamics III
ย 
Unsaturated hydrocarbons
Unsaturated hydrocarbonsUnsaturated hydrocarbons
Unsaturated hydrocarbons
ย 
Inner transition elements
Inner transition elementsInner transition elements
Inner transition elements
ย 
Kinetics of solution in reaction
Kinetics of solution in reactionKinetics of solution in reaction
Kinetics of solution in reaction
ย 
Kinetics of Thermochemical chain reactions
Kinetics of Thermochemical chain reactionsKinetics of Thermochemical chain reactions
Kinetics of Thermochemical chain reactions
ย 
Kinetics of Chain reaction
Kinetics of Chain reactionKinetics of Chain reaction
Kinetics of Chain reaction
ย 
Electron Spin Resonance Spectroscopy
Electron Spin Resonance Spectroscopy Electron Spin Resonance Spectroscopy
Electron Spin Resonance Spectroscopy
ย 
Molecular spectroscopy
Molecular spectroscopyMolecular spectroscopy
Molecular spectroscopy
ย 

Recently uploaded

Monthly Social Media Update April 2024 pptx.pptx
Monthly Social Media Update April 2024 pptx.pptxMonthly Social Media Update April 2024 pptx.pptx
Monthly Social Media Update April 2024 pptx.pptxAndy Lambert
ย 
0183760ssssssssssssssssssssssssssss00101011 (27).pdf
0183760ssssssssssssssssssssssssssss00101011 (27).pdf0183760ssssssssssssssssssssssssssss00101011 (27).pdf
0183760ssssssssssssssssssssssssssss00101011 (27).pdfRenandantas16
ย 
DEPED Work From Home WORKWEEK-PLAN.docx
DEPED Work From Home  WORKWEEK-PLAN.docxDEPED Work From Home  WORKWEEK-PLAN.docx
DEPED Work From Home WORKWEEK-PLAN.docxRodelinaLaud
ย 
Russian Faridabad Call Girls(Badarpur) : โ˜Ž 8168257667, @4999
Russian Faridabad Call Girls(Badarpur) : โ˜Ž 8168257667, @4999Russian Faridabad Call Girls(Badarpur) : โ˜Ž 8168257667, @4999
Russian Faridabad Call Girls(Badarpur) : โ˜Ž 8168257667, @4999Tina Ji
ย 
Enhancing and Restoring Safety & Quality Cultures - Dave Litwiller - May 2024...
Enhancing and Restoring Safety & Quality Cultures - Dave Litwiller - May 2024...Enhancing and Restoring Safety & Quality Cultures - Dave Litwiller - May 2024...
Enhancing and Restoring Safety & Quality Cultures - Dave Litwiller - May 2024...Dave Litwiller
ย 
GD Birla and his contribution in management
GD Birla and his contribution in managementGD Birla and his contribution in management
GD Birla and his contribution in managementchhavia330
ย 
Tech Startup Growth Hacking 101 - Basics on Growth Marketing
Tech Startup Growth Hacking 101  - Basics on Growth MarketingTech Startup Growth Hacking 101  - Basics on Growth Marketing
Tech Startup Growth Hacking 101 - Basics on Growth MarketingShawn Pang
ย 
MONA 98765-12871 CALL GIRLS IN LUDHIANA LUDHIANA CALL GIRL
MONA 98765-12871 CALL GIRLS IN LUDHIANA LUDHIANA CALL GIRLMONA 98765-12871 CALL GIRLS IN LUDHIANA LUDHIANA CALL GIRL
MONA 98765-12871 CALL GIRLS IN LUDHIANA LUDHIANA CALL GIRLSeo
ย 
VIP Call Girls In Saharaganj ( Lucknow ) ๐Ÿ” 8923113531 ๐Ÿ” Cash Payment (COD) ๐Ÿ‘’
VIP Call Girls In Saharaganj ( Lucknow  ) ๐Ÿ” 8923113531 ๐Ÿ”  Cash Payment (COD) ๐Ÿ‘’VIP Call Girls In Saharaganj ( Lucknow  ) ๐Ÿ” 8923113531 ๐Ÿ”  Cash Payment (COD) ๐Ÿ‘’
VIP Call Girls In Saharaganj ( Lucknow ) ๐Ÿ” 8923113531 ๐Ÿ” Cash Payment (COD) ๐Ÿ‘’anilsa9823
ย 
VIP Kolkata Call Girl Howrah ๐Ÿ‘‰ 8250192130 Available With Room
VIP Kolkata Call Girl Howrah ๐Ÿ‘‰ 8250192130  Available With RoomVIP Kolkata Call Girl Howrah ๐Ÿ‘‰ 8250192130  Available With Room
VIP Kolkata Call Girl Howrah ๐Ÿ‘‰ 8250192130 Available With Roomdivyansh0kumar0
ย 
Vip Dewas Call Girls #9907093804 Contact Number Escorts Service Dewas
Vip Dewas Call Girls #9907093804 Contact Number Escorts Service DewasVip Dewas Call Girls #9907093804 Contact Number Escorts Service Dewas
Vip Dewas Call Girls #9907093804 Contact Number Escorts Service Dewasmakika9823
ย 
Monte Carlo simulation : Simulation using MCSM
Monte Carlo simulation : Simulation using MCSMMonte Carlo simulation : Simulation using MCSM
Monte Carlo simulation : Simulation using MCSMRavindra Nath Shukla
ย 
Catalogue ONG NUOC PPR DE NHAT .pdf
Catalogue ONG NUOC PPR DE NHAT      .pdfCatalogue ONG NUOC PPR DE NHAT      .pdf
Catalogue ONG NUOC PPR DE NHAT .pdfOrient Homes
ย 
Regression analysis: Simple Linear Regression Multiple Linear Regression
Regression analysis:  Simple Linear Regression Multiple Linear RegressionRegression analysis:  Simple Linear Regression Multiple Linear Regression
Regression analysis: Simple Linear Regression Multiple Linear RegressionRavindra Nath Shukla
ย 
Keppel Ltd. 1Q 2024 Business Update Presentation Slides
Keppel Ltd. 1Q 2024 Business Update  Presentation SlidesKeppel Ltd. 1Q 2024 Business Update  Presentation Slides
Keppel Ltd. 1Q 2024 Business Update Presentation SlidesKeppelCorporation
ย 
Socio-economic-Impact-of-business-consumers-suppliers-and.pptx
Socio-economic-Impact-of-business-consumers-suppliers-and.pptxSocio-economic-Impact-of-business-consumers-suppliers-and.pptx
Socio-economic-Impact-of-business-consumers-suppliers-and.pptxtrishalcan8
ย 
The Coffee Bean & Tea Leaf(CBTL), Business strategy case study
The Coffee Bean & Tea Leaf(CBTL), Business strategy case studyThe Coffee Bean & Tea Leaf(CBTL), Business strategy case study
The Coffee Bean & Tea Leaf(CBTL), Business strategy case studyEthan lee
ย 
Cash Payment 9602870969 Escort Service in Udaipur Call Girls
Cash Payment 9602870969 Escort Service in Udaipur Call GirlsCash Payment 9602870969 Escort Service in Udaipur Call Girls
Cash Payment 9602870969 Escort Service in Udaipur Call GirlsApsara Of India
ย 
RE Capital's Visionary Leadership under Newman Leech
RE Capital's Visionary Leadership under Newman LeechRE Capital's Visionary Leadership under Newman Leech
RE Capital's Visionary Leadership under Newman LeechNewman George Leech
ย 

Recently uploaded (20)

Nepali Escort Girl Kakori \ 9548273370 Indian Call Girls Service Lucknow โ‚น,9517
Nepali Escort Girl Kakori \ 9548273370 Indian Call Girls Service Lucknow โ‚น,9517Nepali Escort Girl Kakori \ 9548273370 Indian Call Girls Service Lucknow โ‚น,9517
Nepali Escort Girl Kakori \ 9548273370 Indian Call Girls Service Lucknow โ‚น,9517
ย 
Monthly Social Media Update April 2024 pptx.pptx
Monthly Social Media Update April 2024 pptx.pptxMonthly Social Media Update April 2024 pptx.pptx
Monthly Social Media Update April 2024 pptx.pptx
ย 
0183760ssssssssssssssssssssssssssss00101011 (27).pdf
0183760ssssssssssssssssssssssssssss00101011 (27).pdf0183760ssssssssssssssssssssssssssss00101011 (27).pdf
0183760ssssssssssssssssssssssssssss00101011 (27).pdf
ย 
DEPED Work From Home WORKWEEK-PLAN.docx
DEPED Work From Home  WORKWEEK-PLAN.docxDEPED Work From Home  WORKWEEK-PLAN.docx
DEPED Work From Home WORKWEEK-PLAN.docx
ย 
Russian Faridabad Call Girls(Badarpur) : โ˜Ž 8168257667, @4999
Russian Faridabad Call Girls(Badarpur) : โ˜Ž 8168257667, @4999Russian Faridabad Call Girls(Badarpur) : โ˜Ž 8168257667, @4999
Russian Faridabad Call Girls(Badarpur) : โ˜Ž 8168257667, @4999
ย 
Enhancing and Restoring Safety & Quality Cultures - Dave Litwiller - May 2024...
Enhancing and Restoring Safety & Quality Cultures - Dave Litwiller - May 2024...Enhancing and Restoring Safety & Quality Cultures - Dave Litwiller - May 2024...
Enhancing and Restoring Safety & Quality Cultures - Dave Litwiller - May 2024...
ย 
GD Birla and his contribution in management
GD Birla and his contribution in managementGD Birla and his contribution in management
GD Birla and his contribution in management
ย 
Tech Startup Growth Hacking 101 - Basics on Growth Marketing
Tech Startup Growth Hacking 101  - Basics on Growth MarketingTech Startup Growth Hacking 101  - Basics on Growth Marketing
Tech Startup Growth Hacking 101 - Basics on Growth Marketing
ย 
MONA 98765-12871 CALL GIRLS IN LUDHIANA LUDHIANA CALL GIRL
MONA 98765-12871 CALL GIRLS IN LUDHIANA LUDHIANA CALL GIRLMONA 98765-12871 CALL GIRLS IN LUDHIANA LUDHIANA CALL GIRL
MONA 98765-12871 CALL GIRLS IN LUDHIANA LUDHIANA CALL GIRL
ย 
VIP Call Girls In Saharaganj ( Lucknow ) ๐Ÿ” 8923113531 ๐Ÿ” Cash Payment (COD) ๐Ÿ‘’
VIP Call Girls In Saharaganj ( Lucknow  ) ๐Ÿ” 8923113531 ๐Ÿ”  Cash Payment (COD) ๐Ÿ‘’VIP Call Girls In Saharaganj ( Lucknow  ) ๐Ÿ” 8923113531 ๐Ÿ”  Cash Payment (COD) ๐Ÿ‘’
VIP Call Girls In Saharaganj ( Lucknow ) ๐Ÿ” 8923113531 ๐Ÿ” Cash Payment (COD) ๐Ÿ‘’
ย 
VIP Kolkata Call Girl Howrah ๐Ÿ‘‰ 8250192130 Available With Room
VIP Kolkata Call Girl Howrah ๐Ÿ‘‰ 8250192130  Available With RoomVIP Kolkata Call Girl Howrah ๐Ÿ‘‰ 8250192130  Available With Room
VIP Kolkata Call Girl Howrah ๐Ÿ‘‰ 8250192130 Available With Room
ย 
Vip Dewas Call Girls #9907093804 Contact Number Escorts Service Dewas
Vip Dewas Call Girls #9907093804 Contact Number Escorts Service DewasVip Dewas Call Girls #9907093804 Contact Number Escorts Service Dewas
Vip Dewas Call Girls #9907093804 Contact Number Escorts Service Dewas
ย 
Monte Carlo simulation : Simulation using MCSM
Monte Carlo simulation : Simulation using MCSMMonte Carlo simulation : Simulation using MCSM
Monte Carlo simulation : Simulation using MCSM
ย 
Catalogue ONG NUOC PPR DE NHAT .pdf
Catalogue ONG NUOC PPR DE NHAT      .pdfCatalogue ONG NUOC PPR DE NHAT      .pdf
Catalogue ONG NUOC PPR DE NHAT .pdf
ย 
Regression analysis: Simple Linear Regression Multiple Linear Regression
Regression analysis:  Simple Linear Regression Multiple Linear RegressionRegression analysis:  Simple Linear Regression Multiple Linear Regression
Regression analysis: Simple Linear Regression Multiple Linear Regression
ย 
Keppel Ltd. 1Q 2024 Business Update Presentation Slides
Keppel Ltd. 1Q 2024 Business Update  Presentation SlidesKeppel Ltd. 1Q 2024 Business Update  Presentation Slides
Keppel Ltd. 1Q 2024 Business Update Presentation Slides
ย 
Socio-economic-Impact-of-business-consumers-suppliers-and.pptx
Socio-economic-Impact-of-business-consumers-suppliers-and.pptxSocio-economic-Impact-of-business-consumers-suppliers-and.pptx
Socio-economic-Impact-of-business-consumers-suppliers-and.pptx
ย 
The Coffee Bean & Tea Leaf(CBTL), Business strategy case study
The Coffee Bean & Tea Leaf(CBTL), Business strategy case studyThe Coffee Bean & Tea Leaf(CBTL), Business strategy case study
The Coffee Bean & Tea Leaf(CBTL), Business strategy case study
ย 
Cash Payment 9602870969 Escort Service in Udaipur Call Girls
Cash Payment 9602870969 Escort Service in Udaipur Call GirlsCash Payment 9602870969 Escort Service in Udaipur Call Girls
Cash Payment 9602870969 Escort Service in Udaipur Call Girls
ย 
RE Capital's Visionary Leadership under Newman Leech
RE Capital's Visionary Leadership under Newman LeechRE Capital's Visionary Leadership under Newman Leech
RE Capital's Visionary Leadership under Newman Leech
ย 

ATOMIC STRUCTURE AND PERIODIC TABLE

  • 1. Associate Professor & Head , Department of Chemistry SAIVA BHANU KSHATRIYA COLLEGE ARUPPUKOTTAI - 626101 Virudhunagar District, Tamil Nadu, India ATOMIC STRUCTURE AND PERIODIC TABLE
  • 2. The important postulates of Bohrโ€™s theory about the atom model are 1. The electron in an atom revolve around the nucleus only in certain selected circular orbits 2. Each orbits is associated with definite energy and therefore, they are also known as energy levels or energy shells 3. As long as the electron remains in a particular orbit, it neither loses nor gains energy, i.e., the energy of an electron remains constant in a particular orbit THE BOHRโ€™S MODEL OF THE ATOM
  • 3. 4. The energy levels are defined by principal quantum numbers (n = 1,2,3,4,, etc..) starting from the nucleus and also designated by letters K, L, M, N etc., THE BOHRโ€™S MODEL OF THE ATOM
  • 4. 5. The farther the energy level from the nucleus, the greater in the energy associated with it 6. The energy of an electron cannot change continuously. It changes only as the electron jumps from one energy level to another 7. The angular momentum of an electron moving round the nucleus is quantized i.e., the angular momentum of an electron in an atom can have only definite (or) discrete values given by the expression Angular momentum = ๐‘›โ„Ž 2๐œ‹ where n is any integer (1,2,3, etc.,) i.e., the angular momentum of an electron may be โ„Ž 2๐œ‹ or a simple whole number multiple of โ„Ž 2๐œ‹ such as 2โ„Ž 2๐œ‹ , 3โ„Ž 2๐œ‹ , โ€ฆโ€ฆ ๐‘›โ„Ž 2๐œ‹ THE BOHRโ€™S MODEL OF THE ATOM
  • 5. โ€ข Electron revolves around the nucleus of an atom in elliptical orbits adding to circular orbit โ€ข There is a major axes and an minor axes having different length when electron revolves in elliptical orbits SOMERFIELD - BOHR ATOM MODEL According to Somerfield โ€“ Bohr atom model
  • 6. โ€ข The principal quantum number (n) and azimuthal quantum number (k) are related as ๐‘› ๐‘˜ = ๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž ๐‘œ๐‘“ ๐‘š๐‘Ž๐‘—๐‘œ๐‘Ÿ ๐‘Ž๐‘ฅ๐‘’๐‘  ๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž ๐‘œ๐‘“ ๐‘š๐‘–๐‘›๐‘œ๐‘Ÿ ๐‘Ž๐‘ฅ๐‘’๐‘  โ€ข When length of major axes is equal to length of minor axes, then k = n, i.e., the electron orbit must be circular โ€ข But, as k becomes smaller ( k < n ), the orbit become elliptical with greater and greater eccentricity โ€ข The number of possible value of k is equal to the principal quantum number (n). i.e., for n = 4 , k can have four values as shown in the diagram SOMERFIELD - BOHR ATOM MODEL
  • 7. โ€ข As the orbit broadens, the length of the two axes become closer and become equal when the orbit become circular โ€ข The angular momentum of the electrons revolving in an elliptical orbit is equal to ๐‘˜โ„Ž 2๐œ‹ , where k is the azimuthal quantum number โ€ข The energy of an electron depends not only principal quantum number but also azimuthal quantum number SOMERFIELD BOHR ATOM MODEL
  • 8. โ€ข de-Broglie stated that electron can travel (X-ray) as wave and as particle. This character is known as dual character Derivation of de-Broglie wave equation : โ€ข According to Einstein, the energy of an electron (X- ray) is E = mc2 ---------(1) Where m ------ mass of the electron c ------ velocity of electron โ€ข According to Plank's , the energy of light radiation (X-ray) is E = h๏ฎ ----------(2) Where h ------- Plankโ€™s constant ๏ฎ ------- Frequency of light radiation de โ€“ BROGLIE DUAL NATURE OF ELECTRON
  • 9. โ€ข Equating equation (1) and (2), we get mc2 = h๏ฎ ---------(3) โ€ข Substitute ๏ฎ = ๐‘ ๏ฌ in equation (3), we get mc2 = h ๐‘ ๏ฌ mc = โ„Ž ๏ฌ ๏ฌ = โ„Ž ๐‘š๐‘ This equation is known as de โ€“ Broglie wave equation de โ€“ BROGLIE WAVE PARTICLE CONCEPT FOR ELECTRON
  • 10. โ€ข The behavior of electron waves in atoms and molecules is described by the Schrรถdinger wave equation SCHRODINGER WAVE EQUATION Where ฯˆ is the wave function of electron E is the total energy of electron V is the potential energy of electron E-V is the kinetic energy of the electron h is the Plankโ€™s constant
  • 11. Physical significance of the wave function: 1. The wave function ฮจ has no direct physical meaning. It is a complex quality representing the variation of a matter wave 2. The wave function ฮจ (r,t) describes the position of a particle with respect to time 3. It can be considered as โ€˜probability amplitudeโ€™ since it is used to find the location of the particle SCHRODINGER WAVE EQUATION
  • 12. Definition: Quantum numbers are the numbers which are used to describe completely the state of electrons in an atom. Four types of quantum numbers โ€ข Principal quantum number, denoted by n โ€ข Azimuthal quantum number, denoted by l โ€ข Magnetic quantum number, denoted by m โ€ข Electron spin quantum number, denoted by s QUANTUM NUMBERS
  • 13. โ€ข Principal quantum numbers describe the size and energy level or shell of electron in an atom . It is denoted by โ€˜nโ€™ โ€ข And also describe the distance between the electron and the nucleus i.e., larger the value of principle quantum number, greater the distance between electron and the nucleus โ€ข The value of the principal quantum number might be any equal to or greater than one. i.e., n = 1,2,3,โ€ฆ. โ€ข The value n=1 denotes the innermost electron shell of an atom, which corresponds to the lowest energy state of an electron and as the n value increases the energy level increases PRINCIPLE QUANTUM NUMBER (n)
  • 14. โ€ข The azimuthal quantum number describes the sub energy level or subshell of the electron in an atom and also describe the shape of the electron clouds around the nucleus of an atom. It is denoted by โ€˜lโ€™ โ€ข This value depends on the value of the principal quantum number, i.e. the value of the azimuthal quantum number ranges between 0 and (n-1). โ€ข For example, if n =3, the azimuthal quantum number are 0,1 and 2. When l=0, the resulting subshell is an โ€˜sโ€™ subshell. Similarly, when l=1 and l=2, the resulting subshells are โ€˜pโ€™ and โ€˜dโ€™ subshells (respectively). Therefore, when n=3, the three possible subshells are 3s, 3p, and 3d. AZIMUTHAL QUANTUM NUMBER (l)
  • 15. โ€ข Magnetic quantum number describe the total number of orbitals in a subshell and the orientation of these orbitals. It is denoted by โ€˜mโ€™. โ€ข The value of the magnetic quantum number is dependent on the value of the azimuthal quantum number. โ€ข For a given value of l, the value of m ranges between the interval -l to +l. โ€ข For example, if l = 1 in an atom, the possible values of the magnetic quantum number are -1, 0, +1 and the orbitals are named as px, py and pz MAGNETIC QUANTUM NUMBER (m)
  • 16. ELECTRON SPIN QUANTUM NUMBER (s) โ€ข The electron spin quantum number describe the spinning nature of the electron which are revolving around the nucleus of an atom. It is denoted by โ€˜sโ€™ โ€ข The possible values of the electron spin quantum number are +ยฝ and -ยฝ. โ€ข The positive value of s implies an upward spin on the electron which is also called โ€˜spin upโ€™ and is denoted by the symbol โ†‘. โ€ข The negative value of s implies a downward spin on the electron which is also called โ€˜spin downโ€™ and is denoted by the symbol โ†“.
  • 17. Name and Symbol Meaning and Possible Values Principal quantum number, n Electron shell, n โ‰ฅ 1 Azimuthal quantum number, l Subshells (s=0, p=1, etc.) , (n-1) โ‰ฅ l โ‰ฅ 0 Magnetic quantum number, ml Total number and orientation of orbitals, l โ‰ฅ ml โ‰ฅ -l Electron spin quantum number, ms The direction of electron spin, ms = ยฑยฝ SUMMARY OF QUANTUM NUMBER
  • 18. AUFBAU PRINCIPLE โ€ข Aufbau principle states that the orbitals are filled in the order of their increasing energies. That is the electrons first occupy the lowest energy orbital available to them. Once the lower energy orbitals are completely filled, then the electrons enter the next higher energy orbitals.
  • 19. HUNDโ€™S RULE โ€ข Hundโ€™s rule state that electron pairing in any orbital is not possible until all the available orbitals of a given subshell contains one electron each (half filled ) Eg: FOR NITROGEN ATOM
  • 20. PAULIโ€™S EXCLUSION PRINCIPLE โ€ข Pauli Exclusion Principle states that no two electrons can be identified by the same set of quantum numbers and the orbital can accommodate only two electrons with opposite spin For helium atom the electronic configuration is 1s2 The quantum numbers for the first and second electron are First electron : n = 1, l = 0, m = 0 & s = + ยฝ Second electron: n = 1, l = 0, m = 0 & s = - ยฝ
  • 21. MODERN PERIODIC LAW The modern periodic law states that the properties of the elements are a periodic function of their atomic numbers i.e., the elements are arranged in an increasing order of their atomic number in the periodic table
  • 22. โ€ข Repetition of properties of elements in the periodic table after a certain interval is called periodicity of properties. โ€ข If elements are arranged in increasing order of their atomic number in the periodic table, then elements repeat their properties after a definite interval PERIODICITY IN PROPERTIES PERIODIC PROPERTIES OF THE ELEMENTS 1. Atomic radii 2. Ionization energy 3. Electron affinity 4. Electronegativity
  • 25. ATOMIC RADII IN PERIOD
  • 30. ELECTRON AFFINITY H1 H2 โˆ†H = H2 โ€“ H1 = Electron affinity Where H1 is the energy of neutral chlorine atom H2 is the energy of chloride ion
  • 31. ELECTRON AFFINITY IN GROUP Down the group in periodic table electron affinity decreases because of the addition of new shell to each atom decreases is force of attraction
  • 32. ELECTRON AFFINITY IN PERIOD In period the electron affinity increases from left to right because successive atoms have higher nuclear charge and attract the incoming electrons more towards itself
  • 36. ELECTRONEGATIVITY SCALE โ€ข There are three quantitative scales used to evaluate electronegativity of an element 1. Pauling scale 2. Mulliken scale 3. Allred and Rochow scale
  • 37. PAULING SCALE โ€ข Pauling derived an electronegativity scale based on experimentally derived values of bond energies โ€ข According to Pauling, Bond energy of a compound A-B for pure covalency is a geometric mean of the bond energies of A-A and B-B i.e., Bond energy for pure covalency = [D A-A x D B-B ]1/2 โ€ข But actual experimental value D A-B is found to be greater than this expected value i.e., D A-B (experimental) - [D A-A x D B-B ]1/2 = โˆ†โ€ฒ โ€ข The difference, โˆ†โ€ฒ is due to electronegativity differences between the atoms. i.e., the electronegativity difference (XB โ€“ XA) is directly proportional to (XB โ€“ XA) ๏‚ต โˆ†โ€ฒ (XB โ€“ XA) = k โˆ†โ€ฒ
  • 38. PAULING SCALE โ€ข Where XB is the electronegativity of B XA is the electronegativity of A k is the proportionality constant โ€ข When โˆ†โ€ฒ is zero, Bonding electrons are shared equally i.e., the electronegativity of A and B atoms are same โ€ข In general, smaller atoms attract electron more than larger ones and therefore more electronegative โ€ข Atoms with nearly filled shells of electrons (example : halogens) will tends to have higher electronegativity than those with not filled shells
  • 39. MULLIKEN SCALE โ€ข According to Mulliken, the electronegativity of an element is the arithmetic mean of first ionization energy which measures its tendency to hold its own outer electrons, and its electron affinity which measures its tendency to attract electron of the element bonded with it Electronegativity of an element = ๐‘ญ๐’Š๐’“๐’”๐’• ๐’Š๐’๐’๐’Š๐’”๐’•๐’‚๐’Š๐’๐’ ๐’†๐’๐’†๐’“๐’ˆ๐’š+๐‘ฌ๐’๐’†๐’„๐’•๐’“๐’๐’ ๐’‚๐’‡๐’‡๐’Š๐’๐’Š๐’•๐’š ๐Ÿ โ€ข The Mulliken (M) and Pauling (P) values are related approximately as XM B โ€“ XM A = 2.78 (XP B - XP A)
  • 40. ALLRED AND ROCHOW SCALE โ€ข Allred and Rochow defined electronegativity as the electrostatic force exerted by the nucleus on the valence electrons โ€ข According to them Electronegativity = 0.359 ๐’ โˆ— ๐’“๐Ÿ+ 0.744 where Z* is the effective nuclear charge experienced by the electron r is the mean radius of the orbital which can be taken equal to the covalent radius of the atom (in A0)
  • 41. EFFECTIVE NUCLEAR CHARGE Definition โ€ข The effective nuclear charge is the net positive charge experienced by valence electrons. Slater proposed a formula for calculating the effective nuclear charge Zeff = Z โ€“ S where Zeff is the effective nuclear charge Z is the atomic number S is the shielding constant โ€ข Shielding electrons are the inner shell electrons which are blocking the valence shell electron attraction by the nucleus First Inner shell Valence shell Second Inner shell
  • 42. SLATER RULE โ€ข Slater formulated the following rules for calculating the screening constant value for various inner shell electrons for obtaining effective nuclear charge
  • 46. APPLICATION OF SLATER RULE APPLICATION OF SLATER RULE
  • 47. APPLICATION OF SLATER RULE APPLICATION OF SLATER RULE
  • 48. APPLICATION OF SLATER RULE APPLICATION OF SLATER RULE
  • 49. POLARIZING POWER Definition โ€ข Polarizing power can be defined as the ability of a cation to attract the electron cloud towards itself. Polarising power is proportional to charge/size.
  • 51. ANOMALOUS BEHAVIOUR OF FIRST ELEMENT IN A GROUP โ€ข The anomalous behaviour of first element of s and p block elements of each group as compared to other group members is due to following reasons: 1. Small size of atom 2. Large charge/radius ratio, 3. High electronegativity 4. Non availability of d-orbitals in their valence shell
  • 52. BALANCING OF REDOX EQUATION Reduction โ€ข Gain of electron is called reduction Oxidation โ€ข Loss of electron is called oxidation Redox reaction โ€ข Both gain and loss of electron occur in the chemical reaction is called redox reaction Zn โ†’ Zn2+ + 2e- Cu2+ + 2e- โ†’ Cu 4Zn + 10 HNO3 โ†’ 4Zn(NO3)2 + N2O + 5H2O โ€ข Here Zinc is oxidized from zero state to +2 state and nitrogen is reduced from +5 state to +2 state
  • 53. BALANCING OF REDOX EQUATION There are two methods used for balancing the redox equation 1. Oxidation number method 2. Ion โ€“ electron method
  • 54. Oxidation Method : Rules 1. Assign oxidation number to the atom that shows changes 2. Balance the total number of atoms undergoing the changes in oxidation state 3. Count the total number of electrons gained and lost respectively by the oxidizing agent and reducing agent 4. Chose the proper ratio of oxidizing agent to the reducing agent so that the oxidation number change is balanced 5. Make appropriate change in the coefficient of the products corresponding to the change of coefficients in step 4 6. Balance the oxygen atom on bot sides by adding H2O to the side that is deficient in oxygen BALANCING OF REDOX EQUATION
  • 55. 7. Balance the hydrogen atoms on both sides by adding H+ to the side that is deficient in hydrogen 8. The equation is balanced if the reaction taking place in acidic solution. If , however the reaction proceeds in basic solution, add sufficient number of OH- to get rid of H+ but add equal number of OH- on both side BALANCING OF REDOX EQUATION
  • 56. Example : Write the balanced equation for Cr2O7 2- + Fe2+ + H+ โ†’ Cr3+ + Fe3+ +H2O Solution: 1) Writing the skeleton equation Cr2O7 2- + Fe2+ + H+ โ†’ 2Cr3+ + Fe3+ +H2O 2) Marking reducing agent and oxidizing agent. In this equation oxidation state of Fe2+ is raised to Fe3+ Therefore it is reducing agent. The oxidation state of Cr in Cr2O7 2- is reduced from -6 to +3. Hence it is an oxidizing agent 3) Writing half reaction for oxidation of reducing agent (Fe3+) taking care of balancing of atoms of Fe and the charge Fe2+ โ†’ Fe3+ + e- ------------(1) There are no oxygen or hydrogen atoms attached with the species. So question of balancing them does not arise BALANCING OF REDOX EQUATION
  • 57. 4) Writing other half reaction for reduction of oxidizing agent () while balancing i) Cr and ii) O by adding H+ ions on the oxygen exceeding side and iii) charge by adding electrons as Cr2O7 2- + 14 H+ + 6e- โ†’ 2Cr3+ + 7H2O ------------(2) 5) To equalize the number of electrons 6) Multiplying the half reaction (1) by 6 and adding to the half reaction (2) 6Fe2+ โ†’ 6Fe3+ +6 e- Cr2O7 2- + 14 H+ + 6e- โ†’ 2Cr3+ + 7H2O Cr2O7 2- + 14 H+ + 6 Fe2+ โ†’ 2Cr3+ + 6 Fe3+ 7H2O BALANCING OF REDOX EQUATION
  • 58. Ion โ€“ Electron Method : Rules 1. Write the skeleton equation, showing oxidation state of the elements undergoing a change in oxidation state 2. Mark the reducing agent ( having the atom whose oxidation number is raised) and also the oxidizing agent ( one having the atom whose oxidation number is lowered) 3. Write down one half reaction for oxidation of the reducing agent balancing i) the number of atoms undergoing the change in oxidation state ii) the oxygen atoms on the two sides by adding H2O to the side deficient in oxygen or H+ ions to the side with excess of oxygen iii) the charge by putting the required number of electrons on R.H.S BALANCING OF REDOX EQUATION
  • 59. 4. In a similar manner write down the other half of the reaction for reduction of the oxidizing agent. To balance the charge electron would now be added on the L.H.S 5. Add these two balanced half โ€“ reactions in such a way that the electrons appearing on the right of one half-reaction and on the left of the other cancel. For this each half-reaction will be multiplied by appropriate numbers before addition 6. If the reaction proceeds in basic solution, add enough OH- on both sides of the half-reaction to get rid of H+ appearing there. Combine H+ and OH- to give H2O and remove H2O duplication BALANCING OF REDOX EQUATION
  • 60. Example: Write the balanced equation for Zn + HNO3 โ†’ Zn2+ + N2O + 4H2O Solution: 1. Assigning oxidation state to atoms that shows change in oxidation state and balancing number of atoms balancing number of atoms showing this change on both sides (Zn and N atoms) Zn + 2HNO3 โ†’ Zn + N2O + H2O -------------(1) โ†“ โ†‘ 2e- 4e- 2. Equalizing electrons lost = electron gained Total number of electrons lost by one Zn = 1 x 2 = 2 Total number of electrons gained by two N atoms = 2 x 4 = 8 To equalize the electrons lost = electrons gained, we multiply Zn by 4 and 2HNO3 by 1. 4Zn + 2HNO3 โ†’ 4Zn 2+ + N2O + H2O -------------(2) BALANCING OF REDOX EQUATION
  • 61. 3. Balancing O-atom, the number of O atoms on right hand side is 2 while on left hand side is 6. To balance O-atoms, add 4H2O on R.H.S 4Zn + 2HNO3 โ†’ 4Zn 2+ + N2O + 5H2O -------------(3) 4. Balancing H-atoms, in equation (3) the number of H-atoms is 8 more on R.H.S than their number on L.H.S . Add 8H+ ions on L.H.S. By doing so the charge on both sides also balanced. 4Zn + 2HNO3 + 8H+ โ†’ 4Zn 2+ + N2O + 5H2O (or) 4Zn + 2NO- 3 + 10H+ โ†’ 4Zn 2+ + N2O + 5H2O BALANCING OF REDOX EQUATION
  • 62. โ€ข If however it is desired to have 4Zn(NO3)2 instead of 4Zn2+ on R.H.S, we can do so by adding 8NO3 - ions on both sides 4Zn + 2H+ +2NO- 3 + 8H+ + 8NO3 - โ†’ 4Zn2+ + 8NO3 - + N2O + 5H2O then the molecular equation is 4Zn + 10HNO3 โ†’ 4Zn (NO3)2 + N2O + 5H2O BALANCING OF REDOX EQUATION