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Packages for Newbies --- Quantum Field TheoryNode id: 3918collection
- LECS/QFT-01:: Classical Fields
- Module 2:: Pictures in Quantum Mechanics
- Module 4:: Second Quantization of Schrodinger Field
- Module 5:: Second Quantization of Klein Gordon Field
- Module 6:: Dirac Equation
- Module 7:: Quantization of Electro-Magnetic Field
Problem Sessions will start appearing here in near future
Planned course for Newbies
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21-09-14 18:09:55 |
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[2003SM/LNP-14] Lecture-14--Equipartition of EnergyNode id: 5539pageIn this lecture we derive law of equipartition of energy under the assumption that the energy is quadratic function of some variable such as coordinates and momenta. The classical theory of specific heat of gases is given and the Einstein model of taking quantum corrections is briefly discussed. A comparison of the classical and quantum model with experiments is given.
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22-07-07 07:07:20 |
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[1998TH/LNP-34]-Applications of Kinetic Theory of GasesNode id: 5603page |
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22-07-17 19:07:53 |
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[NOTES/QM-11004] Time Reversal SymmetryNode id: 4732page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}\newcommand{\dd}[2][]{\frac{d#1}{d#2}}\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
Time reversal operation in quantum mechanics of one particle is discussed.
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24-06-23 18:06:29 |
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[NOTES/ME-02011]-no title Node id: 5671page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
$\newcommand{\xbf}{\bf x}$
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22-08-14 10:08:37 |
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[NOTES/EM-09006]-Faraday's Law and Maxwell's Second EquationNode id: 5727pageThe Maxwell's equations for static fields get modified by additional terms when the field vary with time slowly. These modifications are describe here.
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22-08-24 16:08:31 |
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21Th-ProbSet7Node id: 5004page |
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21-11-29 19:11:38 |
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[QUE/TH-01002] TH-PROBLEMNode id: 5152pageA bimetallic strip of total thickness $x$ is straight at temperature $T$. What is the radius of curvature of the strip, $R$, when it is heated to temperature $T + ∆T$ ? The coefficients of linear expansion of the two metals are $α_1$ and $α_2$ , respectively, with \(α_1 > α_2 \). Assume each metal has thickness \(x/2\), and that \(x << R.\)
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22-01-13 18:01:05 |
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[QUE/TH-07007] TH-PROBLEMNode id: 5213page A mass $m$ of a liquid at a temperature $T_1$ is mixed with an equal mass of the same liquid at a temperature $T_2$. The system is thermally isolated. Show that the entropy change is given by $$ 2m\,C_p\,\ln\left({(T_1+T_2)/2\over\sqrt{T_1T_2}}\right) $$ and prove that this is necessarily positive.
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22-01-23 11:01:59 |
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[NOTES/EM-01011] $\vec B$ vs $\vec H$ --- Naming convention.Node id: 5953pageWe will call \(\vec B\) field as magnetic field when no medium is present.\\ In presence of a magnetic medium, \(\vec B\) will be called magnetic flux density or magnetic induction. The field \(vec H\) will called magnetic intensity or magnetic field intensity
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23-09-30 03:09:36 |
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[2019EM/QUIZ-08]Node id: 5360pageElectrodynamics Apr 19, 2019 Quiz-VIII
Question 1: A student was asked to find the electric field inside a uniformly polarized sphere. The following answer was received.
Sample Answer:

The answer to the above question as given in Griffiths is
\(\vec{E}=-\frac{\vec{P}}{3\epsilon_0}\)
- Give your comments why is this answer wrong?
- Give a counter example showing that the conclusion arrived by the student is incorrect.
- Give steps to derive the correct answer
Question 2: Consider a parallel plate capacitor with plates having charges \(Q\) and \(-Q\). An insulating medium fills the region between the plates. Assuming that the linear dimensions of the plates are much larger than the separation between the plates, draw a diagram to show
- the distribution of free charges on the plates.
- distribution of the bound charges on the surface of the dielectric material.
- Use Gauss law to obtain \(\vec{D}\). Use your result for \(\vec{D}\) and obtain \(\vec{E}\), the potential difference between the plates and the capacitance.
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22-04-04 17:04:06 |
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[2018EM/HMW-03]Node id: 5424page |
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22-06-21 08:06:16 |
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[NOTES/EM-02005] Flux of $\bar{E}$ and Using Gauss lawNode id: 5577pageThe flux of electric field is defined and As a simple example, the flux of the electric field due to a point charge at the center of a sphere is explicitly computed. Other cases are briefly mentioned an statement of Gauss law is given.
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23-10-02 12:10:31 |
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Quantum Mechanics --- Notes for Lectures and Problems [QM-MIXED-LOT]Node id: 4671collection
TABLE OF CONTENTS
- [QM-01] Classical Theories Revisited
- [QM-02] A Quick Review of Vector Spaces
- [QM-03] Inner Product Spaces
- [QM-04]* Infinite Dimensional vector spaces
- [QM-05] 30 years that shook Physics
- [QM-06] Postulates of Quantum Mechanics
- [QM-07] Canonical Quantization
- [QM-08] Eigenvalues Using Commutators
- [QM-09] Time Development
- [QM-10] Coordinate and Momentum Representation
- [QM-11] Time Dependent Schrodinger Equation
- [[QM-12] Free Particle and Particle in Box
- [QM-13] Energy Eigenvalue Problems in One Dimension
- [QM-14] Reflection and Transmission
- [QM-15] Problems in Two Dimensions
- [QM-16] Spherically Symmetric Potential Problems
- [QM-17] Angular Momentum in Quantum Mechanics
- [QM-18] Scattering -- Three Dimensions
- [QM-19] Method of Partial Waves
- [QM-20] Spin and Identical Particles
- [QM-21] Variation Method
- [QM-22] WKB Approximation
- [QM-23] Time Independent Perturbation Theory
- [QM-24] Approximation Methods for Time Dependent Problems
- [QM-25] Semi-Classical Theory of Radiation
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22-05-30 11:05:24 |
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[NOTES/EM-03004]-The Electric Stress TensorNode id: 5641pageAn expression for the electric stress tensor is derived for a charge distribution in a volume \(V\). The surface integral of the stress tensor gives the total electric force on the charge in the volume \(V\).
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23-10-17 14:10:45 |
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[NOTES/QM-17004] Recurrence Relations for CG CoefficientsNode id: 4817page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ $\newcommand{\ket}[1]{\langle #1\rangle}$ qm-lec-17004
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22-03-04 09:03:38 |
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[NOTES/ME-14007]-Parallel Axes TheoremNode id: 5701page |
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22-08-16 16:08:43 |
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[NOTES/EM-12001]-Lorentz transformations Node id: 5757page
The basic equations of Maxwell's theory are written down in relativistic notation. Using Lorentz transformations of the potentials, the expressions of the scalar and vector potentials of a point charge moving with a uniform velocity are obtained.
$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
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23-03-03 21:03:55 |
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[QUE/SM-03005] --- SM-PROBLEMNode id: 5069pageA system consists of three particles and each particle can exist in five possible states. Find the total number of microstates and the number of microstates that energy level has two particles assuming
- the particles are non-identical
- are identical bosons
- are identical fermions.
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22-01-09 20:01:30 |
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[QUE/TH-13002] TH-PROBLEMNode id: 5187pagea) An ion of mass m and electric charge e is moving in a dilute gas of molecules with which it collides. The mean time between collisions is $\tau$. Let there be a uniform electric field $E$ along the x-axis. Show that the mean distance travelled by the ion is $$ \frac{Ee}{m}\tau^2$$ assuming the velocity of the ion is zero immediately after collision.
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22-01-14 13:01:21 |
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