SlideShare a Scribd company logo
Crystal Structure
Arpan Deyasi
Dept. of ECE, RCCIIT, Kolkata
Arpan Deyasi
Electron Device
Crystal
A crystal is a homogeneous, anisotropic solid
body having long-range 3D ordering (order may
be Translational/orientational/combination of
both), i.e., constructed by infinite repetition of
identical structural units.
Features:
• Natural shape of polyhedron
• Chemical compound
• Under the action of interatomic forces
• End phase generally becomes solid when passing from
phase transformation under suitable conditions
Arpan Deyasi
Electron Device
Lattice
Space-lattice is a mathematical concept, defined
as infinite number of regular periodic arrays of
points in 3D configuration having long-range
ordering (both in translational & orientational),
with the property that arrangement of points
about any particular point is isotropically
identical.
a2
a
3
a1
u2a2
u
3
a
3
1 1 2 2 3 3
r u a u a u a
= + +
where are translational vectors
1 2 3
, ,
a a a
Arpan Deyasi
Electron Device
Basis
It is the group of atoms, identical in composition, arrangement and orientation, when
repeated in space periodically and isotropically, forms crystal structure.
Basis Lattice Crystal
Arpan Deyasi
Electron Device
Crystalline Solid Amorphous Solid
Atomic
Arrangement
Atoms are arranged in a regular,
repeating pattern
Atoms are arranged randomly,
lacking a long-range order
Melting Point Have a sharp, distinct melting
point
Melt over a range of temperatures,
not a specific point
Hardness When broken, crystalline solids
tend to cleave along specific
planes due to their ordered
structure
Break with irregular or curved
surfaces, not along defined planes
X-ray
Diffraction
Produce sharp, well-defined X-
ray diffraction patterns due to
their ordered structure
Produce broad, diffuse patterns or
no diffraction pattern at all,
indicating the lack of long-range
order
Anisotropy/
Isotropy
Can be anisotropic (physical
properties vary depending on
direction)
Generally isotropic, with similar
properties in all directions
Example Diamond, quartz, salt Glass, rubber, plastic
Arpan Deyasi
Electron Device
Unit Cell
Smallest geometric arrangement whose
repetition in 3D space gives actual crystal
structure.
This elementary pattern of minimum number of
points carry all the characteristics of the crystal.
Unit cell Crystal formation
Arpan Deyasi
Electron Device
Primitive Cell
It is the unit cell which contains lattice points at
corners only.
It is the minimum volume unit cell, and will fill
all the space by repetition of suitable crystal
translational operations.
Each primitive cell is associated with one lattice
point.
No. of atoms in a primitive cell is always the same
for a given crystal structure.
1 2 3
.
p
V a a a
= 
Crystal formation
Arpan Deyasi
Electron Device
Primitive Cell Unit Cell
Repeating
pattern
simplest repeating unit in a
crystal structure
larger repeating unit that can be
primitive or non-primitive
No of points Contains only one lattice point,
which is typically located at the
corners of the cell
Non-primitive unit cells (also
called centered unit cells) contain
additional lattice points within the
cell, along with corner point
Example A cubic primitive unit cell has
lattice points only at the corners
BCC unit cell has lattice points at
the corners and one in the center.
FCC unit cell has lattice points at
the corners and in the center of
each face
Arpan Deyasi
Electron Device
Bravis Lattice
Network of part where position vectors can be expressed
in the form
1 1 2 2 3 3
r u a u a u a
= + +
where the choice of basis vectors is not unique.
A primitive unit cell is called Bravis lattice.
Arpan Deyasi
Electron Device
Classification of Cubic Lattice
Cubic Lattice
Simple Cubic
Body-Centered
Cubic (BCC)
Face-Centered
Cubic (FCC)
Arpan Deyasi
Electron Device
A few properties
Coordination number: It is defined as number of equidistant neighbor that an atom has in the
given structure
Packing Fraction: It is defined as the maximum proportion of available volume in a unit cell
that can be occupied by the closed pack spheres
Arpan Deyasi
Electron Device
Simple Cubic Lattice
Unit cell contains 8 atoms, 1 in each corner
Each corner atom is shared among 8 cells, so
Total no of atoms per unit cell = 8⨯(1/8)=1
No. of atoms per unit cell = 1
Coordination no. = 6
Distance between any two corner atoms = ‘a’
So, radius of closed-packed sphere r = 0.5a
Atomic radius = 0.5a
Packing fraction =
3
3
4
3
r
a

3
3
4
3.8
a
a

= 0.523
6

= =
P.F = 0.523
Arpan Deyasi
Electron Device
Body-Centered Cubic Lattice
Unit cell contains 9 atoms, 1 in each corner
and 1 in center
Each corner atom is shared among 8 cells, so
Total no of atoms per unit cell
= 8⨯(1/8) + 1 = 2
No. of atoms per unit cell = 2
Coordination no. = 8
Lattice constant = ‘a’
So, length of body diagonal = √3. a = 4r
Atomic radius = (√3. a)/4
This length contains 3 atoms, where no of corner
atoms = 2
Packing fraction =
3
3
4
3
2
r
a


3
3
4 .3 3.
2
3.8.8
a
a

= 
3
0.68
8

= =
P.F = 0.68
Arpan Deyasi
Electron Device
Face-Centered Cubic Lattice
Unit cell contains 14 atoms, 1 in each corner
and 6 in faces
Each corner atom is shared among 8 cells,
and each face atom is shared among 2 cells,
so total no of atoms per unit cell
= 8⨯(1/8) + 6⨯(1/2) = 4
No. of atoms per unit cell = 4
Coordination no. = 12
Lattice constant = ‘a’
So, length of face diagonal = √2. a = 4r
Atomic radius = 2√2.a
This length contains 3 atoms, where no of corner
atoms = 2
Packing fraction =
3
3
4
3
4
r
a


3
3
4
4
3.16. 2
a
a

=  0.74
3 2

= =
P.F = 0.74
Arpan Deyasi
Electron Device
Comparative Study between SC, BCC, FCC
Feature Simple Cubic (SC)
Body-Centered Cubic
(BCC)
Face-Centered Cubic
(FCC)
Atom Locations
Atoms only at the 8
corners of the cube
Atoms at the 8 corners
and 1 atom at the body
center
Atoms at the 8 corners
and at the center of each
of the 6 faces
Atoms per Unit Cell 1 2 4
Coordination Number 6 8 12 (
Relationship between
Edge Length (a) and
Atomic Radius (r)
a = 2r a = 4r/√3 a = 2√​2 r
Packing Efficiency (APF) 52.4% 68% 74%
Arpan Deyasi
Electron Device
Miller Indices
Position and orientation of a crystal plane is
determined by any three non-collinear points in
the plane. The notation by which the plane is
described, is called Miller Indices.
a2
a
3
a1
u2a2
u
3
a
3
1 1 2 2 3 3
r u a u a u a
= + +
where are translational vectors
1 2 3
, ,
a a a
Arpan Deyasi
Electron Device
How to calculate Miller Indices
Determine intercept of each plane along each of
3 crystallographic directions.
Calculate reciprocals of intercepts.
If fraction appears, multiply each by the
denominator of the smallest fraction.
X
Y
Z
X
Y
Z
X
Y
Z
Arpan Deyasi
Electron Device
Interplanar Spacing
Perpendicular distance between two adjacent parallel
planes in a crystal lattice is called interplanar spacing
X
Y
Z
P
γ
β
α
O
Plane (hkl) intercepts the coordinate system at
(a/h), (b/k), (c/l) respectively
Interplanar spacing dhkl = OP
cos( )
/
hkl
d
a h
 =
cos( )
/
hkl
d
b k
 = cos( )
/
hkl
d
c l
 =
Arpan Deyasi
Electron Device
Interplanar Spacing
X
Y
Z
P
γ
β
α
O
2 2 2
cos ( ) cos ( ) cos ( ) 1
  
+ + =
2 2 2
1
/ / /
hkl hkl hkl
d d d
a h b k c l
     
+ + =
     
     
2 2 2
2 2 2
1
hkl
d
h k l
a b c
=
 
+ +
 
 
For cubic cell
( )
2 2 2
hkl
a
d
h k l
=
+ +
Arpan Deyasi
Electron Device

More Related Content

PPTX
Crystal Systems
PPTX
Crystal structure
PPTX
Phys 4710 lec 3
PDF
Space lattice and crystal structure,miller indices PEC UNIVERSITY CHD
PPTX
Crystal structures
PPTX
Crystallography SP.pptx
PPTX
Engineering Physics - Crystal structure - Dr. Victor Vedanayakam.S
PPTX
Crystal system
Crystal Systems
Crystal structure
Phys 4710 lec 3
Space lattice and crystal structure,miller indices PEC UNIVERSITY CHD
Crystal structures
Crystallography SP.pptx
Engineering Physics - Crystal structure - Dr. Victor Vedanayakam.S
Crystal system

Similar to classification of cubic lattice structure (20)

PPTX
Crystal Structure
PDF
Physics - topic 2.pdf, physics sem1 ece
PDF
Chapter 3 - Atomic and Ionic Arrangements.pdf
PPT
Presentation1
 
PPTX
1676375195643 civil mechPPT Unit-IV.pptx
PPTX
Engineering Materials _ Crystal Geometry
PDF
Structure and its types
PDF
Solid state physics unit 1.pdf
PDF
Solid state physics by Dr. kamal Devlal.pdf
PDF
Jif 419 webex 1 2016-2017
PPT
Space lattices
 
PDF
Lab-2 Crystallography in Materials Science
PPTX
Crystallography
PPTX
Crystal structures in material science
PPTX
MET 205 METALLURGY & MATERIAL SCIENCE
PDF
Solid state physics Lec2_Lattice updated till 15_2.pdf
PPTX
Ic technology- Crystal structure and Crystal growth
PDF
Crystal and Crystal Systems PowerPoint Presentation
Crystal Structure
Physics - topic 2.pdf, physics sem1 ece
Chapter 3 - Atomic and Ionic Arrangements.pdf
Presentation1
 
1676375195643 civil mechPPT Unit-IV.pptx
Engineering Materials _ Crystal Geometry
Structure and its types
Solid state physics unit 1.pdf
Solid state physics by Dr. kamal Devlal.pdf
Jif 419 webex 1 2016-2017
Space lattices
 
Lab-2 Crystallography in Materials Science
Crystallography
Crystal structures in material science
MET 205 METALLURGY & MATERIAL SCIENCE
Solid state physics Lec2_Lattice updated till 15_2.pdf
Ic technology- Crystal structure and Crystal growth
Crystal and Crystal Systems PowerPoint Presentation
Ad

More from RCC Institute of Information Technology (20)

PDF
Scaling in conventional MOSFET for constant electric field and constant voltage
PDF
Carrier scattering and ballistic transport
PDF
Electromagnetic Wave Propagations
PDF
PDF
Reflection and Transmission coefficients in transmission line
PDF
Impedance in transmission line
PDF
Distortionless Transmission Line
PDF
PDF
Electrical Properties of Dipole
PDF
Application of Gauss' Law
PDF
Fundamentals of Gauss' Law
PDF
Fundamentals of Coulomb's Law
PDF
Scalar and vector differentiation
PDF
Coordinate transformation
Scaling in conventional MOSFET for constant electric field and constant voltage
Carrier scattering and ballistic transport
Electromagnetic Wave Propagations
Reflection and Transmission coefficients in transmission line
Impedance in transmission line
Distortionless Transmission Line
Electrical Properties of Dipole
Application of Gauss' Law
Fundamentals of Gauss' Law
Fundamentals of Coulomb's Law
Scalar and vector differentiation
Coordinate transformation
Ad

Recently uploaded (20)

PDF
Model Code of Practice - Construction Work - 21102022 .pdf
PPT
Mechanical Engineering MATERIALS Selection
PPTX
CARTOGRAPHY AND GEOINFORMATION VISUALIZATION chapter1 NPTE (2).pptx
PPTX
UNIT 4 Total Quality Management .pptx
PPTX
web development for engineering and engineering
PDF
Enhancing Cyber Defense Against Zero-Day Attacks using Ensemble Neural Networks
PPTX
Foundation to blockchain - A guide to Blockchain Tech
DOCX
ASol_English-Language-Literature-Set-1-27-02-2023-converted.docx
PPTX
Lecture Notes Electrical Wiring System Components
PPTX
Recipes for Real Time Voice AI WebRTC, SLMs and Open Source Software.pptx
PPT
CRASH COURSE IN ALTERNATIVE PLUMBING CLASS
PDF
PRIZ Academy - 9 Windows Thinking Where to Invest Today to Win Tomorrow.pdf
PDF
R24 SURVEYING LAB MANUAL for civil enggi
DOCX
573137875-Attendance-Management-System-original
PDF
Evaluating the Democratization of the Turkish Armed Forces from a Normative P...
PPTX
Infosys Presentation by1.Riyan Bagwan 2.Samadhan Naiknavare 3.Gaurav Shinde 4...
PDF
Automation-in-Manufacturing-Chapter-Introduction.pdf
PDF
BMEC211 - INTRODUCTION TO MECHATRONICS-1.pdf
PPTX
IOT PPTs Week 10 Lecture Material.pptx of NPTEL Smart Cities contd
PDF
keyrequirementskkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkk
Model Code of Practice - Construction Work - 21102022 .pdf
Mechanical Engineering MATERIALS Selection
CARTOGRAPHY AND GEOINFORMATION VISUALIZATION chapter1 NPTE (2).pptx
UNIT 4 Total Quality Management .pptx
web development for engineering and engineering
Enhancing Cyber Defense Against Zero-Day Attacks using Ensemble Neural Networks
Foundation to blockchain - A guide to Blockchain Tech
ASol_English-Language-Literature-Set-1-27-02-2023-converted.docx
Lecture Notes Electrical Wiring System Components
Recipes for Real Time Voice AI WebRTC, SLMs and Open Source Software.pptx
CRASH COURSE IN ALTERNATIVE PLUMBING CLASS
PRIZ Academy - 9 Windows Thinking Where to Invest Today to Win Tomorrow.pdf
R24 SURVEYING LAB MANUAL for civil enggi
573137875-Attendance-Management-System-original
Evaluating the Democratization of the Turkish Armed Forces from a Normative P...
Infosys Presentation by1.Riyan Bagwan 2.Samadhan Naiknavare 3.Gaurav Shinde 4...
Automation-in-Manufacturing-Chapter-Introduction.pdf
BMEC211 - INTRODUCTION TO MECHATRONICS-1.pdf
IOT PPTs Week 10 Lecture Material.pptx of NPTEL Smart Cities contd
keyrequirementskkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkk

classification of cubic lattice structure

  • 1. Crystal Structure Arpan Deyasi Dept. of ECE, RCCIIT, Kolkata Arpan Deyasi Electron Device
  • 2. Crystal A crystal is a homogeneous, anisotropic solid body having long-range 3D ordering (order may be Translational/orientational/combination of both), i.e., constructed by infinite repetition of identical structural units. Features: • Natural shape of polyhedron • Chemical compound • Under the action of interatomic forces • End phase generally becomes solid when passing from phase transformation under suitable conditions Arpan Deyasi Electron Device
  • 3. Lattice Space-lattice is a mathematical concept, defined as infinite number of regular periodic arrays of points in 3D configuration having long-range ordering (both in translational & orientational), with the property that arrangement of points about any particular point is isotropically identical. a2 a 3 a1 u2a2 u 3 a 3 1 1 2 2 3 3 r u a u a u a = + + where are translational vectors 1 2 3 , , a a a Arpan Deyasi Electron Device
  • 4. Basis It is the group of atoms, identical in composition, arrangement and orientation, when repeated in space periodically and isotropically, forms crystal structure. Basis Lattice Crystal Arpan Deyasi Electron Device
  • 5. Crystalline Solid Amorphous Solid Atomic Arrangement Atoms are arranged in a regular, repeating pattern Atoms are arranged randomly, lacking a long-range order Melting Point Have a sharp, distinct melting point Melt over a range of temperatures, not a specific point Hardness When broken, crystalline solids tend to cleave along specific planes due to their ordered structure Break with irregular or curved surfaces, not along defined planes X-ray Diffraction Produce sharp, well-defined X- ray diffraction patterns due to their ordered structure Produce broad, diffuse patterns or no diffraction pattern at all, indicating the lack of long-range order Anisotropy/ Isotropy Can be anisotropic (physical properties vary depending on direction) Generally isotropic, with similar properties in all directions Example Diamond, quartz, salt Glass, rubber, plastic Arpan Deyasi Electron Device
  • 6. Unit Cell Smallest geometric arrangement whose repetition in 3D space gives actual crystal structure. This elementary pattern of minimum number of points carry all the characteristics of the crystal. Unit cell Crystal formation Arpan Deyasi Electron Device
  • 7. Primitive Cell It is the unit cell which contains lattice points at corners only. It is the minimum volume unit cell, and will fill all the space by repetition of suitable crystal translational operations. Each primitive cell is associated with one lattice point. No. of atoms in a primitive cell is always the same for a given crystal structure. 1 2 3 . p V a a a =  Crystal formation Arpan Deyasi Electron Device
  • 8. Primitive Cell Unit Cell Repeating pattern simplest repeating unit in a crystal structure larger repeating unit that can be primitive or non-primitive No of points Contains only one lattice point, which is typically located at the corners of the cell Non-primitive unit cells (also called centered unit cells) contain additional lattice points within the cell, along with corner point Example A cubic primitive unit cell has lattice points only at the corners BCC unit cell has lattice points at the corners and one in the center. FCC unit cell has lattice points at the corners and in the center of each face Arpan Deyasi Electron Device
  • 9. Bravis Lattice Network of part where position vectors can be expressed in the form 1 1 2 2 3 3 r u a u a u a = + + where the choice of basis vectors is not unique. A primitive unit cell is called Bravis lattice. Arpan Deyasi Electron Device
  • 10. Classification of Cubic Lattice Cubic Lattice Simple Cubic Body-Centered Cubic (BCC) Face-Centered Cubic (FCC) Arpan Deyasi Electron Device
  • 11. A few properties Coordination number: It is defined as number of equidistant neighbor that an atom has in the given structure Packing Fraction: It is defined as the maximum proportion of available volume in a unit cell that can be occupied by the closed pack spheres Arpan Deyasi Electron Device
  • 12. Simple Cubic Lattice Unit cell contains 8 atoms, 1 in each corner Each corner atom is shared among 8 cells, so Total no of atoms per unit cell = 8⨯(1/8)=1 No. of atoms per unit cell = 1 Coordination no. = 6 Distance between any two corner atoms = ‘a’ So, radius of closed-packed sphere r = 0.5a Atomic radius = 0.5a Packing fraction = 3 3 4 3 r a  3 3 4 3.8 a a  = 0.523 6  = = P.F = 0.523 Arpan Deyasi Electron Device
  • 13. Body-Centered Cubic Lattice Unit cell contains 9 atoms, 1 in each corner and 1 in center Each corner atom is shared among 8 cells, so Total no of atoms per unit cell = 8⨯(1/8) + 1 = 2 No. of atoms per unit cell = 2 Coordination no. = 8 Lattice constant = ‘a’ So, length of body diagonal = √3. a = 4r Atomic radius = (√3. a)/4 This length contains 3 atoms, where no of corner atoms = 2 Packing fraction = 3 3 4 3 2 r a   3 3 4 .3 3. 2 3.8.8 a a  =  3 0.68 8  = = P.F = 0.68 Arpan Deyasi Electron Device
  • 14. Face-Centered Cubic Lattice Unit cell contains 14 atoms, 1 in each corner and 6 in faces Each corner atom is shared among 8 cells, and each face atom is shared among 2 cells, so total no of atoms per unit cell = 8⨯(1/8) + 6⨯(1/2) = 4 No. of atoms per unit cell = 4 Coordination no. = 12 Lattice constant = ‘a’ So, length of face diagonal = √2. a = 4r Atomic radius = 2√2.a This length contains 3 atoms, where no of corner atoms = 2 Packing fraction = 3 3 4 3 4 r a   3 3 4 4 3.16. 2 a a  =  0.74 3 2  = = P.F = 0.74 Arpan Deyasi Electron Device
  • 15. Comparative Study between SC, BCC, FCC Feature Simple Cubic (SC) Body-Centered Cubic (BCC) Face-Centered Cubic (FCC) Atom Locations Atoms only at the 8 corners of the cube Atoms at the 8 corners and 1 atom at the body center Atoms at the 8 corners and at the center of each of the 6 faces Atoms per Unit Cell 1 2 4 Coordination Number 6 8 12 ( Relationship between Edge Length (a) and Atomic Radius (r) a = 2r a = 4r/√3 a = 2√​2 r Packing Efficiency (APF) 52.4% 68% 74% Arpan Deyasi Electron Device
  • 16. Miller Indices Position and orientation of a crystal plane is determined by any three non-collinear points in the plane. The notation by which the plane is described, is called Miller Indices. a2 a 3 a1 u2a2 u 3 a 3 1 1 2 2 3 3 r u a u a u a = + + where are translational vectors 1 2 3 , , a a a Arpan Deyasi Electron Device
  • 17. How to calculate Miller Indices Determine intercept of each plane along each of 3 crystallographic directions. Calculate reciprocals of intercepts. If fraction appears, multiply each by the denominator of the smallest fraction. X Y Z X Y Z X Y Z Arpan Deyasi Electron Device
  • 18. Interplanar Spacing Perpendicular distance between two adjacent parallel planes in a crystal lattice is called interplanar spacing X Y Z P γ β α O Plane (hkl) intercepts the coordinate system at (a/h), (b/k), (c/l) respectively Interplanar spacing dhkl = OP cos( ) / hkl d a h  = cos( ) / hkl d b k  = cos( ) / hkl d c l  = Arpan Deyasi Electron Device
  • 19. Interplanar Spacing X Y Z P γ β α O 2 2 2 cos ( ) cos ( ) cos ( ) 1    + + = 2 2 2 1 / / / hkl hkl hkl d d d a h b k c l       + + =             2 2 2 2 2 2 1 hkl d h k l a b c =   + +     For cubic cell ( ) 2 2 2 hkl a d h k l = + + Arpan Deyasi Electron Device