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APPLIED PHYSICS HANDBOOK
P HYSICAL C ONSTANTS AND F ORMULAE
Basic Sciences and Humanities (Physics) Composite Board
Visveswaraya Technological Univesrsity
Jnana Sangama, VTU Main Rd, Machhe, Belagavi, Karnataka 590018
Contents
I
PHYSICAL CONSTANTS and STANDARD VALUES
3
1
Physical constants and Standard Values for all Streams
1.1 Physical Constants . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
1.2 Stadard Values . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
5
5
5
II
2
3
4
FORMULAE
7
Applied Physics for CSE Stream
2.1 Module-1 : LASER and Optical Fibers . . . . . . . . . . . . .
2.1.1 LASER . . . . . . . . . . . . . . . . . . . . . . . . .
2.1.2 Optical Fibers . . . . . . . . . . . . . . . . . . . . . .
2.2 Module-2 : Quantum Mechanics . . . . . . . . . . . . . . . .
2.3 Module -3 : Quantum Computing . . . . . . . . . . . . . . .
2.4 Module -4 : Electrical Properties of Materials and Applications
2.4.1 Electrical conductivity in Solids . . . . . . . . . . . .
2.4.2 Superconductivity . . . . . . . . . . . . . . . . . . .
2.5 Module -5 : Application of Physics in Computing . . . . . . .
2.5.1 Physics of Animation . . . . . . . . . . . . . . . . . .
2.5.2 Statistical Physics for Computing . . . . . . . . . . .
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9
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12
13
Applied Physics for EEE Stream
3.1 Module -1 : Quantum Mechanics . . . . . . . . . .
3.2 Module-2 : Electrical Properties of Materials . . .
3.2.1 Electrical conductivity in Solids . . . . . .
3.2.2 Dielectrics . . . . . . . . . . . . . . . . .
3.2.3 Superconductivity . . . . . . . . . . . . .
3.3 Module - 3 : LASER and Optical Fibers . . . . . .
3.3.1 LASER . . . . . . . . . . . . . . . . . . .
3.3.2 Optical Fibers . . . . . . . . . . . . . . . .
3.4 Module - 4 : Maxwell’s Equations and EM Waves .
3.4.1 Vector Calculus . . . . . . . . . . . . . . .
3.5 Module - 5 : Semiconductors and Devices . . . . .
3.5.1 Electrical Conductivity in Semiconductors
3.5.2 Hall Effect . . . . . . . . . . . . . . . . .
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15
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19
Applied Physics for CV Stream
4.1 Module-1 : Oscillations and Shock waves . . . .
4.1.1 Oscillations . . . . . . . . . . . . . . . .
4.1.2 Shock Waves . . . . . . . . . . . . . . .
4.2 Module-2 : Elasticity . . . . . . . . . . . . . . .
4.3 Module-3 : Acoustics, Radiometry & Photometry
4.3.1 Acoustics . . . . . . . . . . . . . . . . .
4.4 Module -2 : LASER and Optical Fibers . . . . .
4.4.1 LASER . . . . . . . . . . . . . . . . . .
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21
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2
Physical Constants and Formulae
4.5
5
4.4.2 Optical Fibers . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
Module-5 : Natural Hazards and Safety . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
Applied Physics for ME Stream
5.1 Module-1 : Oscillations and Shock waves . . . . . . .
5.1.1 Oscillations . . . . . . . . . . . . . . . . . . .
5.1.2 Shock Waves . . . . . . . . . . . . . . . . . .
5.2 Module-2 : Elasticity . . . . . . . . . . . . . . . . . .
5.3 Module-3 : Thermoelectric Materials . . . . . . . . . .
5.3.1 Thermoelectricity . . . . . . . . . . . . . . . .
5.4 Module-4 : Cryogenics . . . . . . . . . . . . . . . . .
5.5 Module-5 : Materials and Characterization Techniques
Applied Physics-Hand Book
3
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23
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27
Visvesvaraya Technological University
Part I
PHYSICAL CONSTANTS and
STANDARD VALUES
4
Chapter 1
Physical constants and Standard Values
for all Streams
1.1
Physical Constants
Acceleration due to Gravity 𝑔 = 9.8 π‘šπ‘ −2
Avogadro Number 6.023 × 1026 𝐽 π‘˜π‘šπ‘œπ‘™π‘’ −1 𝐾 −1
Boltzmann Constant π‘˜ = 1.38 × 10−23 𝐽𝐾 −1
Charge on the electron 𝑒 = −1.6 × 10−19 𝐢
Charge on the Proton 𝑒 = 1.6 × 10−19 𝐢
Magnetic Peameability of Free Space πœ‡0 = 4πœ‹ × 10−7 π»π‘š −1
Permittivity of Free Space πœ– 0 = 8.854 × 10−23 πΉπ‘š −1
Planck’s Constant β„Ž = 6.625 × 10−34 𝐽𝑠
Rest Mass of the Electron π‘š 𝑒 = 9.1 × 10−31 𝐾𝑔
Rest Mass of the Proton π‘š 𝑝 = 1.6726 × 10−27 𝐾𝑔
Rest Mass of the Neutron π‘š 𝑛 = 1.6749 × 10−27 𝐾𝑔
Speed of Light 𝑐 = 3 × 108 π‘šπ‘ −1
Universal Gas constant 𝑅 = 8.314π½π‘šπ‘œπ‘™π‘’ −1 𝐾 −1
1.2
Stadard Values
Youngs Modulus of Steel 𝐸 = 200πΊπ‘ƒπ‘Ž
Rigidity Modulus of Steel 𝐾 = 80πΊπ‘ƒπ‘Ž
5
Physical Constants and Formulae
Bulk Modulus of Steel 𝐾 = 160πΊπ‘ƒπ‘Ž
Fermi Energy of Copper 𝐸 𝐹 = 7𝑒𝑉
Horizontal Component of Earth’s Magnetic Field 𝐡 𝐻 = 0.3 × 10−4𝑇
Applied Physics-Hand Book
6
Visvesvaraya Technological University
Part II
FORMULAE
7
Ignore this page
Chapter 2
Applied Physics for CSE Stream
2.1
2.1.1
Module-1 : LASER and Optical Fibers
LASER
1. Expression for the number of photons emitted per 𝑑 seconds 𝑁 =
𝑃 is LASER Power Output in watt, 𝑑 is the time in second,
πœ† is the wavelength of LASER in m,
β„Ž is Planck’s Constant and
𝑐 is the speed of light.
π‘ƒπ‘‘πœ†
β„Žπ‘
Photons.
β„Žπ‘
2. The Boltzmann relation 𝑁2 = 𝑁1 𝑒 − πœ†π‘˜π‘‡
𝑁2 is the Number of Atoms in the higher energy state.
𝑁1 is the Number of Atoms in the Lower Energy State,
πœ† is the wavelength of LASER,
π‘˜is Boltzmann Constant,
𝑇 is Absolute Temperature.
2.1.2
Optical Fibers
√οΈ‚
1. Expression for Numerical Aperture of an Optical Fiber 𝑁 𝐴 =
𝑛0 is the RI of the surrounding medium,
𝑛1 is the RI of the Core,
𝑛2 is the RI of Cladding.
2. The Acceptance Angle πœƒ = 𝑆𝑖𝑛−1 (𝑁 𝐴)
π‘ƒπ‘œ
3. Attenuation Co-efficient 𝛼 = −10
π‘™π‘œπ‘”
10 𝑃𝑖 𝑑𝐡/π‘˜π‘š
𝐿
𝐿 is the length of the fiber in km.
π‘ƒπ‘œ is the Power Output of the fiber in π‘Š.
9
𝑛21 −𝑛22
𝑛20
Physical Constants and Formulae
𝑃𝑖 is the Power input of the fiber in π‘Š.
𝑑𝐡 is the unit in decibel.
2.2
Module-2 : Quantum Mechanics
1. The relation between Kinetic Energy and Momentum 𝐸 =
π‘š is the mass of the particle in π‘˜π‘”,
𝑝 is the momentum of the particle in 𝑁 𝑠.
𝑝2
2π‘š ,
2. Energy of the photon 𝐸 = β„Žπœˆ = β„Žπ‘
πœ† ,
β„Ž is Planck’s Constant,
𝜈 is the frequency of the radiation in 𝐻𝑧,
πœ† is the wavelength of the radiation in π‘š, 𝑐 is the speed of light.
β„Ž
in π‘šπ‘’π‘‘π‘’π‘Ÿ
3. de Broglie Wavelength πœ† = β„Žπ‘ = π‘šπ‘£
β„Ž is Planck’s Constant,
π‘š is mass of the particle in kg,
𝑣 is the velocity of the particle π‘šπ‘ −1 .
4. de Broglie Wavelength πœ† = √ β„Ž
2π‘šπΈ
β„Ž is Planck’s Constant,
π‘š is mass of the particle in kg,
𝐸 is the Kinetic Energy of the particle in 𝐽.
5. de Broglie Wavelength πœ† = √
β„Ž
2π‘šπ‘žπ‘‰
β„Ž is Planck’s Constant,
π‘š is the mass of the particle in kg,
π‘ž is the charge on the particle in 𝐢 ,
𝑉 is the accelerating potential in 𝑉.
√
6. de Broglie Wavelength πœ† = √2π‘šβ„Ž 𝑒𝑉 = 12.27×10
𝑉
𝑒
β„Ž is Planck’s Constant,
π‘š 𝑒 is the mass of the electron in kg,
𝑒 is the charge on the electron in 𝐢 ,
𝑉 is the electron accelerating potential in 𝑉.
−10
π‘š
7. Heisenberg’s Uncertainty Principle
β„Ž
Δπ‘₯Δ𝑝 π‘₯ ≥ 4πœ‹
β„Ž
Δ𝐸Δ𝑇 ≥ 4πœ‹
Δπ‘₯ is the uncertainty in the measurement of Position,
Δ𝑃 is the uncertainty in the measurement of Momentum,
Δ𝐸 is the uncertainty in the measurement of Energy,
Δ𝑇 is the uncertainty inn the measurement of transition time.
Applied Physics-Hand Book
10
Visvesvaraya Technological University
Physical Constants and Formulae
8. The uncertainty in the measurement of momentum Δ𝑃 = π‘šΔ𝑣.
Δ𝑣 is the uncertainty in the measurement of velocity.
9. Eigen Energy Values for a Particle in a one dimensional potential well of infinite depth
𝑛2 β„Ž 2
𝐸 𝑛 = 8π‘šπ‘Ž
2,
𝑛 = 1, 2, 3... for the Ground, First and Second energy states etc.,
β„Ž is Planck’s Constant,
π‘š is the mass of the particle in π‘˜π‘”,
π‘Ž is the width of the potential well in π‘š.
2.3
Module -3 : Quantum Computing
1. The wave !function in Ket notation |πœ“βŸ© (Ket Vector), πœ“ is the wave function.
𝛼1
|πœ“βŸ© =
𝛼2
2. The matrix
|0⟩ and |1⟩.
! for of the states
!
1
0
|0⟩ =
and |1⟩ =
0
1
!
1 0
3. Identity Operator 𝐼 =
0 1
4. Pauli Matrices
!
1 0
• 𝜎0 = 𝐼 =
.
0 1
!
0 1
• 𝜎1 = 𝜎π‘₯ = 𝑋 =
.
1 0
!
0 −𝑖
• 𝜎2 = πœŽπ‘¦ = π‘Œ =
.
𝑖 0
!
1 0
• 𝜎3 = πœŽπ‘§ = 𝑍 =
.
0 −1
5. A Matrix is said to be Unitary Matrix is π‘ˆ †π‘ˆ = 𝐼,
Here π‘ˆ † is the conjugate-transpose of a matrix π‘ˆ.
6. A matrix 𝐴 is Hermitian if 𝐴† = 𝐴
7. The wave
in Bra notation βŸ¨πœ“| (bra Vector), πœ“ is the wave function.
function
βŸ¨πœ“| = 𝛼1∗ 𝛼2∗
Applied Physics-Hand Book
11
Visvesvaraya Technological University
Physical Constants and Formulae
8. Inner Product βŸ¨πœ“|πœ™βŸ© = βŸ¨πœ“| ∗ |πœ™βŸ©. Here βŸ¨πœ“| is a Row Vector and |πœ™βŸ© is a Column Vector.
The result is always a scalar product.
9. The product βŸ¨πœ“|πœ“βŸ© = |πœ“| 2 , the probability density.
10. Orthogonality βŸ¨πœ“|πœ™βŸ© = 0
2.4
2.4.1
Module -4 : Electrical Properties of Materials and Applications
Electrical conductivity in Solids
1
1. The Fermi Factor 𝑓 (𝐸) =
𝐸 −𝐸𝐹
π‘˜π‘‡
𝑒
+1
𝐸 is the energy of the level above or below fermi level in, 𝐸 𝐹 is the Fermi Energy, π‘˜ is
Boltzmann Constant, 𝑇 is Absolute Temperature.
2.4.2
Superconductivity
i
h
2
1. The variation of Critical Field with Temperature 𝐻𝑐 = 𝐻0 1 − 𝑇𝑇 2 tesla,
𝑐
𝐻𝑐 is the critical field at a temperature 𝑇 less than the critical temperature 𝑇𝑐 ,
𝐻0 is the critical field at 0𝐾.
2.5
2.5.1
Module -5 : Application of Physics in Computing
Physics of Animation
1. The Odd Rule :When acceleration is constant, one can use the Odd Rule to time the
frames. With this method, one calculate the distance the object moves between frames
using a simple pattern of odd numbers. Between consecutive frames, the distance the
object moves is a multiple of an odd number. For acceleration, the distance between
frames increases by multiples of 1, 3, 5, 7,...
2. The Odd number multiplier for consecutive frames= (( 𝑓 π‘Ÿπ‘Žπ‘šπ‘’# − 1) ∗ 2) − 1
3. Multiplier for distance from first frame to current frame = (π‘π‘’π‘Ÿπ‘Ÿπ‘’π‘›π‘‘ 𝑓 π‘Ÿπ‘Žπ‘šπ‘’# − 1)2
4. π΅π‘Žπ‘ π‘’ π‘‘π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’ =
𝑇 π‘œπ‘‘π‘Žπ‘™ π‘‘π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’
(πΏπ‘Žπ‘ π‘‘ 𝑓 π‘Ÿπ‘Žπ‘šπ‘’ π‘›π‘’π‘šπ‘π‘’π‘Ÿ−1)2
5. Jump Magnification 𝐽 𝑀 =
6. 𝐽𝐻 =
π½π‘’π‘š 𝑝 π‘‘π‘–π‘šπ‘’
π‘ƒπ‘’π‘ β„Ž π‘‘π‘–π‘šπ‘’
=
π½π‘’π‘š 𝑝 π»π‘’π‘–π‘”β„Žπ‘‘
π‘ƒπ‘’π‘ β„Ž π»π‘’π‘–π‘”β„Žπ‘‘
=
π‘ƒπ‘’π‘ β„Ž π΄π‘π‘π‘’π‘™π‘’π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘›
π½π‘’π‘š 𝑝 π΄π‘π‘π‘’π‘™π‘’π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘›
π‘ƒπ‘’π‘ β„Ž π΄π‘π‘π‘’π‘™π‘’π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘›
πΊπ‘Ÿπ‘Žπ‘£π‘–π‘‘π‘Žπ‘‘π‘–π‘œπ‘›π‘Žπ‘™ π΄π‘π‘π‘’π‘™π‘’π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘›
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2.5.2
Statistical Physics for Computing
1. Poisson Distribution Probability Mass Function = 𝑓 (π‘˜; πœ†) = 𝑃(𝑋 = π‘˜) =
πœ† π‘˜ 𝑒 −πœ†
π‘˜!
2. The Decay Equation 𝑁 = 𝑁0 𝑒 −πœ†π‘‘
πœ† is decay constant,
𝑑 is the time, 𝑁0 is Initial Number of Events,
𝑁 is number of events after time 𝑑.
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Chapter 3
Applied Physics for EEE Stream
3.1
Module -1 : Quantum Mechanics
1. The relation between Kinetic Energy and Momentum 𝐸 =
π‘š is the mass of the particle in π‘˜π‘”,
𝑝 is the momentum of the particle in 𝑁 𝑠.
𝑝2
2π‘š ,
2. Energy of the photon 𝐸 = β„Žπœˆ = β„Žπ‘
πœ† ,
β„Ž is Planck’s Constant,
𝜈 is the frequency of the radiation in 𝐻𝑧,
πœ† is the wavelength of the radiation in π‘š, 𝑐 is the speed of light.
β„Ž
3. de Broglie Wavelength πœ† = β„Žπ‘ = π‘šπ‘£
in π‘šπ‘’π‘‘π‘’π‘Ÿ
β„Ž is Planck’s Constant,
π‘š is mass of the particle in kg,
𝑣 is the velocity of the particle π‘šπ‘ −1 .
4. de Broglie Wavelength πœ† = √ β„Ž
2π‘šπΈ
β„Ž is Planck’s Constant,
π‘š is mass of the particle in kg,
𝐸 is the Kinetic Energy of the particle in 𝐽.
5. de Broglie Wavelength πœ† = √
β„Ž
2π‘šπ‘žπ‘‰
β„Ž is Planck’s Constant,
π‘š is the mass of the particle in kg,
π‘ž is the charge on the particle in 𝐢 ,
𝑉 is the accelerating potential in 𝑉.
6. de Broglie Wavelength πœ† = √2π‘šβ„Ž 𝑒𝑉 =
𝑒
β„Ž is Planck’s Constant,
π‘š 𝑒 is the mass of the electron in kg,
−10
12.27×10
√
𝑉
15
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Physical Constants and Formulae
𝑒 is the charge on the electron in 𝐢 ,
𝑉 is the electron accelerating potential in 𝑉.
7. Heisenberg’s Uncertainty Principle
β„Ž
Δπ‘₯Δ𝑝 π‘₯ ≥ 4πœ‹
β„Ž
Δ𝐸Δ𝑇 ≥ 4πœ‹
Δπ‘₯ is the uncertainty in the measurement of Position,
Δ𝑃 is the uncertainty in the measurement of Momentum,
Δ𝐸 is the uncertainty in the measurement of Energy,
Δ𝑇 is the uncertainty inn the measurement of transition time.
8. The uncertainty in the measurement of momentum Δ𝑃 = π‘šΔ𝑣.
Δ𝑣 is the uncertainty in the measurement of velocity.
9. Eigen Energy Values for a Particle in a one dimensional potential well of infinite depth
𝑛2 β„Ž 2
𝐸 𝑛 = 8π‘šπ‘Ž
2,
𝑛 = 1, 2, 3... for the Ground, First and Second energy states etc.,
β„Ž is Planck’s Constant,
π‘š is the mass of the particle in π‘˜π‘”,
π‘Ž is the width of the potential well in π‘š.
3.2
3.2.1
Module-2 : Electrical Properties of Materials
Electrical conductivity in Solids
𝜎
1. The free electron mobility πœ‡ = 𝑣𝐸𝑑 = 𝑛𝑒
π‘š 2𝑉 −1 𝑠−1 ,
𝑣 𝑑 is the drift velocity of the free electrons,
𝐸 the applied electric field strength.
1
2. The Fermi Factor 𝑓 (𝐸) =
𝑒
𝐸 −𝐸𝐹
π‘˜π‘‡
+1
𝐸 is the energy of the level above or below fermi level,
𝐸 𝐹 is the Fermi Energy,
π‘˜ is Boltzmann Constant,
𝑇 is Absolute Temperature.
3. The electrical conductivity of metals as per Quantum Free Electron Theory 𝜎 =
𝑛 is number density of free electron (free electron concentration) in π‘š −3
𝑒 is electronic charge in 𝐢,
πœ† 𝐹 is fermi level mean free path in π‘š,
π‘š is the rest mass of the electron in π‘˜π‘”,
𝑣 𝐹 is the fermi velocity in π‘šπ‘ −1
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1
𝜌
=
𝑛𝑒 2 πœ† 𝐹
π‘šπ‘£ 𝐹
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Physical Constants and Formulae
4. Free electron concentration is given by 𝑛 =
𝑁 is the number of free electrons per atom.
𝑁 𝐴 Avogadro number per kilo mole,
𝐷 is the density of material in π‘˜π‘”,
𝐴 is the atomic mass.
3.2.2
𝑁 𝑁 𝐴 𝐷 −3
𝐴 π‘š
Dielectrics
1. The Dipole Moment πœ‡ = π‘žπ‘‘π‘₯,
π‘ž is either of the charge,
𝑑π‘₯ is the separation between the charges.
2. The Electronic Polarizability 𝛼𝑒 = πœ‡πΈπ‘’ .
𝐸 is the applied electric field strength.
|
3. The polarization 𝑃 = 𝑁 πœ‡ = π‘žπ΄ ,
𝑁 is number of dipoles per unit volume,
π‘ž | is surface image charge,
𝐴 is the surface area.
®
4. The polarization 𝑃® = πœ–0 (πœ–π‘Ÿ − 1) 𝐸,
πœ– 0 is Permittivity of Free Space,
πœ–π‘Ÿ is Dielectric Constant,
𝐸 is the magnitude of Applied Field strength.
1.2πœ‡
5. The internal field 𝐸𝑖 = 𝐸 + πœ‹πœ–
3 in one dimension.
0π‘Ž
π‘Ž is the inter-dipole distance in π‘š.
6. The internal field in Three Dimension is 𝐸𝑖 = 𝐸 +
𝛾 is internal field constant.
𝛾𝑁𝛼𝑒 𝐸
3πœ–0
in one dimension.
7. The internal field for elemental solid dielectric is called Lorentz Field 𝐸 𝐿 = 𝐸 +
8. Clausius-Mossotti relation
3.2.3
𝑁𝛼𝑒
3πœ–0
=
πœ–π‘Ÿ −1
πœ–π‘Ÿ +2 ,
𝑃
3πœ–0
Applicable only for Elemental Solid Dielectrics.
Superconductivity
i
h
2
1. The variation of Critical Field with Temperature 𝐻𝑐 = 𝐻0 1 − 𝑇𝑇 2 tesla,
𝑐
𝐻𝑐 is the critical field at a temperature 𝑇 less than the critical temperature 𝑇𝑐 ,
𝐻0 is the critical field at 0𝐾.
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3.3
3.3.1
Module - 3 : LASER and Optical Fibers
LASER
1. Expression for the number of photons emitted per 𝑑 seconds 𝑁 =
𝑃 is LASER Power Output in watt, 𝑑 is the time in second,
πœ† is the wavelength of LASER in m,
β„Ž is Planck’s Constant and
𝑐 is the speed of light.
π‘ƒπ‘‘πœ†
β„Žπ‘
Photons.
β„Žπ‘
2. The Boltzmann relation 𝑁2 = 𝑁1 𝑒 − πœ†π‘˜π‘‡
𝑁2 is the Number of Atoms in the higher energy state.
𝑁1 is the Number of Atoms in the Lower Energy State,
πœ† is the wavelength of LASER,
’k’is Boltzmann Constant,
T’ is Absolute Temperature.
3.3.2
Optical Fibers
√οΈ‚
1. Expression for Numerical Aperture of an Optical Fiber 𝑁 𝐴 =
𝑛21 −𝑛22
𝑛20
𝑛0 is the RI of the surrounding medium,
𝑛1 is the RI of the Core,
𝑛2 is the RI of Cladding.
2. The Acceptance Angle πœƒ = 𝑆𝑖𝑛−1 (𝑁 𝐴)
𝑛1 −𝑛2
𝑛1
3. The fractional RI change Δ =
√οΈƒ
4. V-Number 𝑉 = 2πœ‹π‘‘
(𝑛21 − 𝑛22 )
πœ†
𝑑 is the diameter of the fiber in π‘š,
πœ† is the wavelength of light in π‘š
5. The number of modes 𝑁 =
𝑉2
2
π‘ƒπ‘œ
−10
𝐿 π‘™π‘œπ‘”10 𝑃𝑖
6. Attenuation Co-efficient 𝛼 =
𝐿 is the length of the fiber in km.
π‘ƒπ‘œ is the Power Output of the fiber in π‘Š
𝑃𝑖 is the Power input of the fiber in π‘Š.
𝑑𝐡 is the unit in decibel.
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3.4
3.4.1
Module - 4 : Maxwell’s Equations and EM Waves
Vector Calculus
πœ•
πœ•
π‘₯ˆ + πœ•π‘¦
𝑦ˆ + πœ•πœ• 𝑧ˆ and a vector field 𝐸® is given by (𝐸 π‘₯ π‘₯ˆ + 𝐸 𝑦 𝑦ˆ +
1. The ∇ operator is given by πœ•π‘₯
𝐸 𝑧 𝑧ˆ)
®
Then the
Divergence of a vector field 𝐸 is given by
πœ•πΈ 𝑦
πœ•πΈ 𝑧
πœ•
π‘₯
∇. 𝐸® = πœ•π‘₯
π‘₯ˆ + πœ•πœ• 𝑦ˆ + πœ•πœ• 𝑧ˆ .(𝐸 π‘₯ π‘₯ˆ + 𝐸 𝑦 𝑦ˆ + 𝐸 𝑧 𝑧ˆ) = πœ•πΈ
πœ•π‘₯ + πœ•π‘¦ + πœ•π‘§
Divergence of a vector field signifies whether the point in a vector field is a source or a
sink. If the divergence is zero then the vector field is Solenoidal.
πœ•
πœ•
2. ∇ operator is given by πœ•π‘₯
π‘₯ˆ + πœ•π‘¦
𝑦ˆ + πœ•πœ• 𝑧ˆ and a vector field 𝐸® is given by (𝐸 π‘₯ π‘₯ˆ + 𝐸 𝑦 𝑦ˆ + 𝐸 𝑧 𝑧ˆ)
Then the curl of a vector field 𝐸® is given by
∇ × πΈ® =
πœ•
πœ•π‘₯ π‘₯ˆ
+ πœ•πœ• 𝑦ˆ + πœ•πœ• 𝑧ˆ × (𝐸 π‘₯ π‘₯ˆ + 𝐸 𝑦 𝑦ˆ + 𝐸 𝑧 𝑧ˆ) =
π‘₯ˆ
𝑦ˆ
𝑧ˆ
πœ•
πœ•π‘₯
πœ•
πœ•π‘¦
πœ•
πœ•π‘§
𝐸π‘₯ 𝐸 𝑦 𝐸 𝑧
The Curl of a vector field signifies how much the vector field rotates at a given point. If
the Curl of a vector field is zero then the vector field is called Irrotational.
3.5
3.5.1
Module - 5 : Semiconductors and Devices
Electrical Conductivity in Semiconductors
1. The electrical conductivity of a semiconductor is πœŽπ‘– = 𝜌1𝑖 = 𝑛𝑖 𝑒(πœ‡ 𝑒 + πœ‡ β„Ž )
𝑛𝑖 is the intrinsic carrier concentration in π‘š −3 ,
𝑒 is electronic charge in 𝐢,
πœ‡ 𝑒 and πœ‡ β„Ž are electron and hole mobilities in π‘š 2𝑉 −1 𝑠−1 .
2. Relation between fermi energy 𝐸 𝐹 and energy gap 𝐸 𝑔 is given by
𝐸
𝐸 𝑓 = 2𝑔
3. Law of mass action 𝑛𝑖2 = 𝑁 𝑒 𝑁 β„Ž
𝑁 𝑒 and 𝑁 β„Ž are electron and hole concentrations respectively.
3.5.2
Hall Effect
1. The Hall Coefficient 𝑅𝐻 = πœŒπ‘›1 𝑒
𝑛𝑒 is the free electron concentration.
𝑅𝐻 is positive for holes and negative for electrons.
2. Hall field 𝐸 𝐻 = 𝑅𝐻 𝐡𝐽
𝐡 is the applied magnetic flux density,
𝐽 is the current density.
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3. Hall Voltage 𝑉𝐻 = 𝑅𝐻 𝐡𝐽𝑑
𝐡 is the applied magnetic flux density,
𝐽 is the current density,
𝑑 is the thickness of the material.
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Chapter 4
Applied Physics for CV Stream
4.1
Module-1 : Oscillations and Shock waves
4.1.1
Oscillations
1. The angular velocity or angular frequency πœ” = 2πœ‹πœˆ =
𝜈 is the frequency of Oscillations in 𝐻𝑧,
𝑇 is the Time Period of oscillations in 𝑠,
π‘˜ is the force constant/stiffness factor in 𝑁 𝑠−1 ,
π‘š is the mass of the body in π‘˜π‘”.
2πœ‹
𝑇
=
√οΈƒ
π‘˜
π‘š
2. Effective spring constant π‘˜ 𝑠 for 𝑛 springs in series π‘˜1𝑆 = π‘˜11 + π‘˜12 + π‘˜13 + . . .
π‘˜ 1 , π‘˜ 2 , π‘˜ 3 ... are the spring constants of individual springs in π‘π‘š −1 .
for 𝑛 identical springs π‘˜ 𝑠 = π‘›π‘˜
π‘˜ is the stiffness factor of each spring in π‘π‘š −1 ..
1
π‘˜3
3. Effective spring constant π‘˜ 𝑝 for 𝑛 springs in parallel π‘˜ 𝑝 = π‘˜ 1 + π‘˜ 2 + π‘˜ 3 + . . . π‘˜ 𝑛
π‘˜ 1 , π‘˜ 2 , π‘˜ 3 ... are the spring constants of individual springs in π‘π‘š −1 .
for 𝑛 identical springs π‘˜ 𝑝 = π‘›π‘˜
π‘˜ is the stiffness factor of each spring in π‘π‘š −1 ..
−𝑏
4. The amplitude of damped oscillations 𝐴𝑑 = 𝐴𝑒 2π‘š 𝑑 in π‘š.
𝑏 is damping constant,
𝑑 is the time.
5. Amplitude in forced oscillations (As per the book Vibrations and Waves by A P French)
𝐴=
𝑓0
π‘š
√οΈƒ
(πœ”20 −πœ”2 ) 2 +(π›Ύπœ”) 2
𝑓0
π‘š
is the amplitude of the applied periodic force per unit mass.
𝛾 is damping ration.
πœ”0 is the natural angular frequency of the system.
πœ” is the angular frequency of the applied periodic force.
21
Physical Constants and Formulae
or 𝐴 = √
𝑏=
4.1.2
π‘Ÿ
2π‘š ,
𝑓0
π‘š
2
(πœ”2 −𝑝 2 ) +4𝑏 2 𝑝 2
𝑝 is the frequency of the applied periodic force.
Shock Waves
1. Mach Number 𝑀 = 𝑣𝑣 0𝑠
𝑣 0 is the velocity of the object or flow in a medium.
𝑣 𝑠 is the velocity of sound in the same medium.
2. Mach Angle πœƒ 𝑀 = 𝑆𝑖𝑛−1
4.2
1
𝑀
Module-2 : Elasticity
1. The Young’s Modulus of the material of a wire of circular cross section loaded at one and
𝐹𝐿
fixed at the other π‘Œ = πœ‹π‘Ÿ
π‘π‘š −2 π‘œπ‘Ÿ π‘ƒπ‘Ž
2𝑙
𝐹 is the applied force in 𝑁,
𝐿 is the original length of the wire in π‘š,
π‘Ÿ is the radius of the wire in π‘š,
𝑙 is the extension in the wire in π‘š.
2. The bulk modulus of the material is given by 𝐾 =
𝑃𝑉
−2
Δ𝑉 π‘π‘š π‘œπ‘Ÿ π‘ƒπ‘Ž
𝑃 is the uniform pressure in π‘ƒπ‘Ž,
𝑉 is the original volume in π‘š −3 ,
Δ𝑉 is he change in volume in π‘š −3
3. The Rigidity Modulus of the material of a wire of circular cross section loaded at one and
fixed at the other πœ‚ = 𝐹𝐴π‘₯𝐿 π‘π‘š −2 π‘œπ‘Ÿ π‘ƒπ‘Ž
𝐹 is the applied force tangentially to the top surface 𝑁,
𝐿 length of the edge of the cube π‘š,
𝐴 is the surface area of te top surface π‘š 2 ,
π‘₯ is the shearing distance π‘š.
4. The Bending moment of a beam is given by 𝑀 = π‘Œπ‘… 𝐼𝑔 π‘π‘š
π‘Œ is the Young’s Modulus of the material of the beam in π‘ƒπ‘Ž,
𝑅 is the radius of curvature of the beam in π‘š 2 ,
𝐼𝑔 is the geometrical moment inertia of the beam in π‘˜π‘”π‘š 2 .
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4.3
4.3.1
Module-3 : Acoustics, Radiometry & Photometry
Acoustics
1. The absorption coefficient of a material surface 𝛼 =
π‘†π‘œπ‘’π‘›π‘‘ πΈπ‘›π‘’π‘Ÿπ‘”π‘¦ π΄π‘π‘ π‘œπ‘Ÿπ‘π‘’π‘‘
𝑇 π‘œπ‘‘π‘Žπ‘™ π‘†π‘œπ‘’π‘›π‘‘ πΈπ‘›π‘’π‘Ÿπ‘”π‘¦ 𝐼𝑛𝑐𝑖𝑑𝑒𝑛𝑑
Í
2. The total absorption co-efficient of all the materials in a hall is 𝐴 = 1𝑛 𝛼𝑛 𝑆𝑛 .
𝛼1 , 𝛼2 ... are the absorption coefficients of the surfaces with areas 𝑆1 , 𝑆2 ....
3. Sabine’s Formula for Reverberation time is 𝑇 =
𝑉 is the volume of the Hall.
4.4
4.4.1
0.161𝑉
𝐴
Module -2 : LASER and Optical Fibers
LASER
1. Expression for the number of photons emitted per 𝑑 seconds 𝑁 =
𝑃 is LASER Power Output in watt, 𝑑 is the time in second,
πœ† is the wavelength of LASER in m,
β„Ž is Planck’s Constant and
𝑐 is the speed of light.
π‘ƒπ‘‘πœ†
β„Žπ‘
Photons.
β„Žπ‘
2. The Boltzmann relation 𝑁2 = 𝑁1 𝑒 − πœ†π‘˜π‘‡
𝑁2 is the Number of Atoms in the higher energy state.
𝑁1 is the Number of Atoms in the Lower Energy State,
πœ† is the wavelength of LASER,
’k’is Boltzmann Constant,
T’ is Absolute Temperature.
4.4.2
Optical Fibers
√οΈ‚
1. Expression for Numerical Aperture of an Optical Fiber 𝑁 𝐴 =
𝑛21 −𝑛22
𝑛20
𝑛0 is the RI of the surrounding medium,
𝑛1 is the RI of the Core,
𝑛2 is the RI of Cladding.
2. The Acceptance Angle πœƒ = 𝑆𝑖𝑛−1 (𝑁 𝐴)
−10
3. Attenuation Co-efficient 𝛼 = 𝐿 π‘™π‘œπ‘”10 π‘ƒπ‘ƒπ‘œπ‘– 𝑑𝐡
𝐿 is the length of the fiber in km.
π‘ƒπ‘œ is the Power Output of the fiber.
𝑃𝑖 is the Power input of the fiber.
𝑑𝐡 is the unit in decibel.
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4.5
Module-5 : Natural Hazards and Safety
1. Energy released during earthquake π‘™π‘œπ‘”πΈ = 5.24 + 1.44𝑀𝑀 ,
𝑀𝑀 is the magnitude of the earthquake.
2. Magnitude of the earthquake 𝑀𝑀 = 23 π‘™π‘œπ‘”π‘€0 − 10.7
𝑀0 is the Seismic moment of the earthquake.
3. Magnitude of the earthquake interms of intensities𝑀 = π‘™π‘œπ‘”
earthquake and 𝐼0 is the base intensity.
4. Ratio of intensities of two earthquakes π‘™π‘œπ‘” 𝐼𝐼12 = 10 𝑀1 −𝑀2
𝐼1 and 𝐼2 are the intensities of two different earthquakes,
𝑀1 and 𝑀2 are the respective magnitudes.
𝐼
𝐼0
, 𝐼 is the intensity of
In all the above equations π‘™π‘œπ‘” is π‘™π‘œπ‘”10
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Chapter 5
Applied Physics for ME Stream
5.1
Module-1 : Oscillations and Shock waves
5.1.1
Oscillations
1. The angular velocity or angular frequency πœ” = 2πœ‹πœˆ =
𝜈 is the frequency of Oscillations in 𝐻𝑧,
𝑇 is the Time Period of oscillations in 𝑠,
π‘˜ is the force constant/stiffness factor in 𝑁 𝑠−1 ,
π‘š is the mass of the body in π‘˜π‘”.
2πœ‹
𝑇
=
√οΈƒ
π‘˜
π‘š
2. Effective spring constant π‘˜ 𝑠 for 𝑛 springs in series π‘˜1𝑆 = π‘˜11 + π‘˜12 + π‘˜13 + . . .
π‘˜ 1 , π‘˜ 2 , π‘˜ 3 ... are the spring constants of individual springs in π‘π‘š −1 .
for 𝑛 identical springs π‘˜ 𝑠 = π‘›π‘˜
π‘˜ is the stiffness factor of each spring in π‘π‘š −1 ..
1
π‘˜3
3. Effective spring constant π‘˜ 𝑝 for 𝑛 springs in parallel π‘˜ 𝑝 = π‘˜ 1 + π‘˜ 2 + π‘˜ 3 + . . . π‘˜ 𝑛
π‘˜ 1 , π‘˜ 2 , π‘˜ 3 ... are the spring constants of individual springs in π‘π‘š −1 .
for 𝑛 identical springs π‘˜ 𝑝 = π‘›π‘˜
π‘˜ is the stiffness factor of each spring in π‘π‘š −1 ..
−𝑏
4. The amplitude of damped oscillations 𝐴𝑑 = 𝐴𝑒 2π‘š 𝑑 in π‘š.
𝑏 is damping constant,
𝑑 is the time.
5. Amplitude in forced oscillations (As per the book Vibrations and Waves by A P French)
𝐴=
𝑓0
π‘š
√οΈƒ
(πœ”20 −πœ”2 ) 2 +(π›Ύπœ”) 2
𝑓0
π‘š
is the amplitude of the applied periodic force per unit mass.
𝛾 is damping ratio given by π‘šπ‘ .
πœ”0 is the natural angular frequency of the system.
πœ” is the angular frequency of the applied periodic force.
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Physical Constants and Formulae
or 𝐴 = √
𝑏=
5.1.2
π‘Ÿ
2π‘š ,
𝑓0
π‘š
2
(πœ”2 −𝑝 2 ) +4𝑏 2 𝑝 2
𝑝 is the frequency of the applied periodic force.
Shock Waves
1. Mach Number 𝑀 = 𝑣𝑣 0𝑠
𝑣 0 is the velocity of the object or flow in a medium.
𝑣 𝑠 is the velocity of sound in the same medium.
2. Mach Angle πœƒ 𝑀 = 𝑆𝑖𝑛−1
5.2
1
𝑀
Module-2 : Elasticity
1. The Young’s Modulus of the material of a wire of circular cross section loaded at one and
𝐹𝐿
fixed at the other π‘Œ = πœ‹π‘Ÿ
π‘π‘š −2 π‘œπ‘Ÿ π‘ƒπ‘Ž
2𝑙
𝐹 is the applied force in 𝑁,
𝐿 is the original length of the wire in π‘š,
π‘Ÿ is the radius of the wire in π‘š,
𝑙 is the extension in the wire in π‘š.
2. The bulk modulus of the material is given by 𝐾 =
𝑃𝑉
−2
Δ𝑉 π‘π‘š π‘œπ‘Ÿ π‘ƒπ‘Ž
𝑃 is the uniform pressure in π‘ƒπ‘Ž,
𝑉 is the original volum in π‘š −3 ,
Δ𝑉 is he change in volume in π‘š −3
3. The Rigidity Modulus of the material of a wire of circular cross section loaded at one and
fixed at the other πœ‚ = 𝐹𝐴π‘₯𝐿 π‘π‘š −2 π‘œπ‘Ÿ π‘ƒπ‘Ž
𝐹 is the applied force tangentially to the top surface 𝑁,
𝐿 length of the edge of the cube π‘š,
𝐴 is the surface area of te top surface π‘š 2 ,
π‘₯ is the shearing distance π‘š.
4. The Bending moment of a beam is given by 𝑀 = π‘Œπ‘… 𝐼𝑔 π‘π‘š
π‘Œ is the Young’s Modulus of the material of the beam in π‘ƒπ‘Ž,
𝑅 is the radius of curvature of the beam in π‘š 2 ,
𝐼𝑔 is the geometrical moment inertia of the beam in π‘˜π‘”π‘š 2 .
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Physical Constants and Formulae
5.3
5.3.1
Module-3 : Thermoelectric Materials
Thermoelectricity
1. Seebeck effect, The voltage generated at the junction is 𝑉 = 𝛼(𝑇2 − 𝑇1 )
𝛼 = 𝛼 𝐴 + 𝛼𝐡 are the Seebeck coefficients of metals A annd B.
𝑇1 and 𝑇2 are the temperatures at the two junctions.
𝐸
2. The 𝛼 = Δ𝑉
Δ𝑇 = Δ𝑇
𝐸 is the electric field in 𝑉 π‘š −1
Δ𝑇 is the temperature gradient.
3. the peltiere coefficient πœ‹π‘Žπ‘ = 𝐻
𝐼𝑑 ,
𝐼 is the junction current,
𝐻 is the heat absorbed in 𝑑 seconds.
4. The variation of thermo emf with temperature is 𝑒 = π‘Žπ‘‘ + 12 𝑏𝑑 2 .
π‘Ž and 𝑏 are Seebeck constants and 𝑑 = 𝑇2 − 𝑇1 ,
𝑇2 is the hot end emperature in 𝐾 and 𝑇1 is the cold end temperature in 𝐾.
2
5. Figure of Merit 𝑍 = π›ΌπΎπœŽ .
𝛼 is the Seebeck coefficient of the material in π‘šπ‘–π‘π‘Ÿπ‘œπ‘£π‘œπ‘™π‘‘/𝐾,
𝜎 is electrical conductivity,
𝐾 is Total thermal conductivity.
6. The Therefrom EMF 𝑒 in terms of temperatures 𝑇1 and 𝑇2 is given by 𝑒 =
πœ‹1 is peltier coefficient.
5.4
πœ‹1
𝑇1 (𝑇2
− 𝑇1 ).
Module-4 : Cryogenics
𝛿𝑇
𝛿𝑃 𝐻
1
𝐢𝑝
2π‘Ž
𝑅𝑇
=
1. Joule Thomson Effect
−𝑏
π‘Ž and 𝑏 are Van der wall’s constant,
𝑅 is universal gas constant = 8.314 Joule/mole/K.
2π‘Ž
2. Inversion Temperature 𝑇𝑖 = 𝑏𝑅
π‘Ž and 𝑏 are Van der wall’s constant,
𝑅 is universal gas constant = 8.314 Joule/mole/K
5.5
Module-5 : Materials and Characterization Techniques
1. Braggs’ Lawπ‘›πœ† = 2𝑑𝑠𝑖𝑛(πœƒ)
𝑛 is the order of diffraction and can take values 1,2,3...,
πœ† is the wavelength of X-rays,
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Physical Constants and Formulae
𝑑 is the inter-planar spacing, and
πœƒ is the glancing angle corresponding to the order of diffraction 𝑛.
π‘˜πœ†
2. Schrrer’s Equation 𝐡(2πœƒ) = πΏπ‘π‘œπ‘ πœƒ
𝐡(2πœƒ) is the full width at half maximum,
πœ† is the wavelength of X-rays, 𝐿 is the crystallite size,
π‘˜ is scherrer constant with the most common value 0.94,
πœƒ is the glancing angle.
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